- reactionThe full reaction equation.
C++ Type:std::string
Unit:(no unit assumed)
Controllable:No
Description:The full reaction equation.
- variableThe name of the variable that this object applies to
C++ Type:AuxVariableName
Unit:(no unit assumed)
Controllable:No
Description:The name of the variable that this object applies to
ProcRateForRateCoeffThreeBody
Reaction rate for three body collisions in units of #/ms. User can pass choice of elastic, excitation, or ionization reaction rate coefficients
Overview
ProcRateForRateCoeffThreeBody
returns the production rate for a three body reactions determined by rate coefficients in units of #/ms.
The production rate is defined as
Where is the production rate determined by rate coefficients, is the rate coefficient for the reaction, is the density for the first species, is the density for the second species, and is the density for the third species. When converting the density to logarithmic form, ProcRateForRateCoeffThreeBody
is defined as
Where , and is the molar density of the species in logarithmic form, and is Avogadro's number.
When coupling Zapdos with CRANE, ProcRateForRateCoeffThreeBody
serves the same function as CRANE's ReactionRateThirdOrderLog
.
Example Input File Syntax
An example of how to use ProcRateForRateCoeffThreeBody
can be found in the test file Lymberopoulos_with_argon_metastables.i
.
[AuxKernels]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[]
(test/tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables.i)Input Parameters
- blockThe list of blocks (ids or names) that this object will be applied
C++ Type:std::vector<SubdomainName>
Unit:(no unit assumed)
Controllable:No
Description:The list of blocks (ids or names) that this object will be applied
- boundaryThe list of boundaries (ids or names) from the mesh where this object applies
C++ Type:std::vector<BoundaryName>
Unit:(no unit assumed)
Controllable:No
Description:The list of boundaries (ids or names) from the mesh where this object applies
- check_boundary_restrictedTrueWhether to check for multiple element sides on the boundary in the case of a boundary restricted, element aux variable. Setting this to false will allow contribution to a single element's elemental value(s) from multiple boundary sides on the same element (example: when the restricted boundary exists on two or more sides of an element, such as at a corner of a mesh
Default:True
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:Whether to check for multiple element sides on the boundary in the case of a boundary restricted, element aux variable. Setting this to false will allow contribution to a single element's elemental value(s) from multiple boundary sides on the same element (example: when the restricted boundary exists on two or more sides of an element, such as at a corner of a mesh
- execute_onLINEAR TIMESTEP_ENDThe list of flag(s) indicating when this object should be executed. For a description of each flag, see https://mooseframework.inl.gov/source/interfaces/SetupInterface.html.
Default:LINEAR TIMESTEP_END
C++ Type:ExecFlagEnum
Unit:(no unit assumed)
Options:NONE, INITIAL, LINEAR, NONLINEAR_CONVERGENCE, NONLINEAR, POSTCHECK, TIMESTEP_END, TIMESTEP_BEGIN, MULTIAPP_FIXED_POINT_END, MULTIAPP_FIXED_POINT_BEGIN, FINAL, CUSTOM, PRE_DISPLACE
Controllable:No
Description:The list of flag(s) indicating when this object should be executed. For a description of each flag, see https://mooseframework.inl.gov/source/interfaces/SetupInterface.html.
- prop_getter_suffixAn optional suffix parameter that can be appended to any attempt to retrieve/get material properties. The suffix will be prepended with a '_' character.
C++ Type:MaterialPropertyName
Unit:(no unit assumed)
Controllable:No
Description:An optional suffix parameter that can be appended to any attempt to retrieve/get material properties. The suffix will be prepended with a '_' character.
- use_interpolated_stateFalseFor the old and older state use projected material properties interpolated at the quadrature points. To set up projection use the ProjectedStatefulMaterialStorageAction.
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:For the old and older state use projected material properties interpolated at the quadrature points. To set up projection use the ProjectedStatefulMaterialStorageAction.
- vThe first variable that is reacting to create u.
C++ Type:std::vector<VariableName>
Unit:(no unit assumed)
Controllable:No
Description:The first variable that is reacting to create u.
- wThe second variable that is reacting to create u.
C++ Type:std::vector<VariableName>
Unit:(no unit assumed)
Controllable:No
Description:The second variable that is reacting to create u.
- xThe third variable that is reacting to create u.
C++ Type:std::vector<VariableName>
Unit:(no unit assumed)
Controllable:No
Description:The third variable that is reacting to create u.
Optional Parameters
- control_tagsAdds user-defined labels for accessing object parameters via control logic.
C++ Type:std::vector<std::string>
Unit:(no unit assumed)
Controllable:No
Description:Adds user-defined labels for accessing object parameters via control logic.
- enableTrueSet the enabled status of the MooseObject.
Default:True
C++ Type:bool
Unit:(no unit assumed)
Controllable:Yes
Description:Set the enabled status of the MooseObject.
- seed0The seed for the master random number generator
Default:0
C++ Type:unsigned int
Unit:(no unit assumed)
Controllable:No
Description:The seed for the master random number generator
- use_displaced_meshFalseWhether or not this object should use the displaced mesh for computation. Note that in the case this is true but no displacements are provided in the Mesh block the undisplaced mesh will still be used.
Default:False
C++ Type:bool
Unit:(no unit assumed)
Controllable:No
Description:Whether or not this object should use the displaced mesh for computation. Note that in the case this is true but no displacements are provided in the Mesh block the undisplaced mesh will still be used.
Advanced Parameters
Input Files
- (test/tests/accelerations/Acceleration_By_Shooting_Method_SensitivityMatrix.i)
- (test/tests/DriftDiffusionAction/2D_RF_Plasma_no_actions.i)
- (test/tests/Conference_Syntax_Tests/Lymberopoulos_with_argon_metastables_2D_At1Torr.i)
- (test/tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables.i)
- (test/tests/DriftDiffusionAction/RF_Plasma_no_actions.i)
- (test/tests/accelerations/Acceleration_By_Shooting_Method.i)
- (test/tests/accelerations/Acceleration_By_Averaging_main.i)
- (test/tests/DriftDiffusionAction/2D_RF_Plasma_actions.i)
- (test/tests/Conference_Syntax_Tests/Lymberopoulos_with_argon_metastables_2D_At100mTorr.i)
- (test/tests/DriftDiffusionAction/RF_Plasma_actions.i)
- (test/tests/Conference_Syntax_Tests/Lymberopoulos_with_argon_metastables.i)
- (test/tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables_2D_At100mTorr_CoarseMesh.i)
(test/tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
#[emDeBug]
#[]
#[Ar+_DeBug]
#[]
#[Ar*_DeBug]
#[]
#[mean_enDeBug]
#[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efield]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[]
[AuxKernels]
#[emDeBug]
# type = DebugResidualAux
# variable = emDeBug
# debug_variable = em
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[Ar+_DeBug]
# type = DebugResidualAux
# variable = Ar+_DeBug
# debug_variable = Ar+
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[mean_enDeBug]
# type = DebugResidualAux
# variable = mean_enDeBug
# debug_variable = mean_en
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[Ar*_DeBug]
# type = DebugResidualAux
# variable = Ar*_DeBug
# debug_variable = Ar*
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = Efield
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
preset = false
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
preset = false
[]
#New Boundary conditions for electons, same as in paper
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 100
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = '0.100 * (25.4e-3 - x)'
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log(3./2.) + log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
#end_time = 0.00737463126
end_time = 3e-7
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-08
#nl_abs_tol = 7.6e-5 #Commit out do to test falure on Mac
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
[TimeSteppers]
[Postprocessor]
type = PostprocessorDT
postprocessor = InversePlasmaFreq
[]
[]
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/accelerations/Acceleration_By_Shooting_Method_SensitivityMatrix.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos_paper.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[SMDeriv]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = ADEEDFReactionLog
variable = em
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = ADEEDFReactionLog
variable = em
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ADReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = ADEEDFReactionLog
variable = Ar+
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = ADEEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ADReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = ADEEDFReactionLog
variable = Ar*
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = ADEEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = ADEEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = ADEEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ADReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ADReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ADReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = ADEEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = ADEEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = ADEEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = ADEEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
#Argon Excited Equations For Shooting Method
#Time Derivative term of excited Argon
[SM_Ar*_time_deriv]
type = TimeDerivative
variable = SMDeriv
[]
#Diffusion term of excited Argon
[SM_Ar*_diffusion]
type = CoeffDiffusionForShootMethod
variable = SMDeriv
density = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon loss from step-wise ionization
[SM_Ar*_stepwise_ionization]
type = EEDFReactionLogForShootMethod
variable = SMDeriv
density = Ar*
electron = em
energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[SM_Ar*_collisions]
type = EEDFReactionLogForShootMethod
variable = SMDeriv
density = Ar*
electron = em
energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[SM_Ar*_quenching]
type = ReactionSecondOrderLogForShootMethod
variable = SMDeriv
density = Ar*
v = em
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[SM_Ar*_pooling]
type = ReactionSecondOrderLogForShootMethod
variable = SMDeriv
density = Ar*
v = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
[]
#Net excited Argon loss from two-body quenching
[SM_Ar*_2B_quenching]
type = ReactionSecondOrderLogForShootMethod
variable = SMDeriv
density = Ar*
v = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
[]
#Net excited Argon loss from three-body quenching
[SM_Ar*_3B_quenching]
type = ReactionThirdOrderLogForShootMethod
variable = SMDeriv
density = Ar*
v = Ar
w = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
[]
[]
[AuxVariables]
[emDeBug]
[]
[Ar+_DeBug]
[]
[Ar*_DeBug]
[]
[mean_enDeBug]
[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efield]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[]
[AuxKernels]
[emDeBug]
type = DebugResidualAux
variable = emDeBug
debug_variable = em
#execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
[]
[Ar+_DeBug]
type = DebugResidualAux
variable = Ar+_DeBug
debug_variable = Ar+
#execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
[]
[mean_enDeBug]
type = DebugResidualAux
variable = mean_enDeBug
debug_variable = mean_en
#execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
[]
[Ar*_DeBug]
type = DebugResidualAux
variable = Ar*_DeBug
debug_variable = Ar*
#execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
[]
[emRate]
type = ADProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ADProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ADProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ADProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ADProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ADProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ADProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ADProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = Efield
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
preset = false
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
preset = false
[]
#New Boundary conditions for electons, same as in paper
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 1e-5
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 1e-5
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*pi*13.56e6*t)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ADZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar -> em + Ar*.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ADZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar -> em + em + Ar+.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ADZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar* -> em + Ar.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ADZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar* -> em + em + Ar+.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = ADGenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = ADGenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = ADGenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = ADGenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-43
reaction_rate_value = 39890.9324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 73.74631268e-9
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-08
#nl_abs_tol = 7.6e-5 #Commit out do to test falure on Mac
dtmin = 1e-14
l_max_its = 20
scheme = bdf2
dt = 1e-9
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/DriftDiffusionAction/2D_RF_Plasma_no_actions.i)
#This is the input file that supplied the gold output file.
#It is the same as the input file in
#tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables_2D_At100mTorr_CoarseMesh.i,
#execpt some of the Aux Variables are renamed for the Action test
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = V
use_moles = true
[]
[Mesh]
type = FileMesh
file = 'GEC_mesh_coarse.msh'
coord_type = RZ
rz_coord_axis = Y
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[potential_ion]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential_ion
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
# Energy loss from elastic collisions
[Elastic_loss]
type = EEDFElasticLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar'
[]
#Effective potential for the Ions
[Ion_potential_time_deriv]
type = TimeDerivative
variable = potential_ion
[]
[Ion_potential_reaction]
type = ScaledReaction
variable = potential_ion
collision_freq = 1283370.875
[]
[Ion_potential_coupled_force]
type = CoupledForce
variable = potential_ion
v = potential
coef = 1283370.875
[]
[]
[AuxVariables]
[e_temp]
order = CONSTANT
family = MONOMIAL
[]
[x_position]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[y_position]
order = CONSTANT
family = MONOMIAL
[]
[y_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_density]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_density]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_density]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efieldx]
order = CONSTANT
family = MONOMIAL
[]
[Efieldy]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[Current_Ar+]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[]
[AuxKernels]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[e_temp]
type = ElectronTemperature
variable = e_temp
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x_position
component = 0
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
component = 0
position_units = ${dom0Scale}
[]
[y_g]
type = Position
variable = y_position
component = 1
position_units = ${dom0Scale}
[]
[y_ng]
type = Position
variable = y_node
component = 1
position_units = ${dom0Scale}
[]
[em_density]
type = DensityMoles
variable = em_density
density_log = em
[]
[Ar+_density]
type = DensityMoles
variable = Ar+_density
density_log = Ar+
[]
[Ar*_density]
type = DensityMoles
variable = Ar*_density
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e2
value = -5.231208
execute_on = INITIAL
[]
[Efieldx_calc]
type = Efield
component = 0
potential = potential
variable = Efieldx
position_units = ${dom0Scale}
[]
[Efieldy_calc]
type = Efield
component = 1
potential = potential
variable = Efieldy
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential_ion
density_log = Ar+
variable = Current_Ar+
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_top_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Top_Electrode'
function = potential_top_bc_func
[]
[potential_bottom_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Bottom_Electrode'
function = potential_bottom_bc_func
[]
[potential_dirichlet_bottom_plate]
type = DirichletBC
variable = potential
boundary = 'Walls'
value = 0
[]
[potential_Dielectric]
type = EconomouDielectricBC
variable = potential
boundary = 'Top_Insulator Bottom_Insulator'
electrons = em
ions = Ar+
ion_potentials = potential_ion
electron_energy = mean_en
dielectric_constant = 1.859382e-11
thickness = 0.0127
emission_coeffs = 0.01
position_units = ${dom0Scale}
[]
#New Boundary conditions for electons, same as in paper
[em_physical_diffusion]
type = SakiyamaElectronDiffusionBC
variable = em
electron_energy = mean_en
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[em_Ar+_second_emissions]
type = SakiyamaSecondaryElectronBC
variable = em
potential = potential_ion
ions = Ar+
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_advection]
type = SakiyamaIonAdvectionBC
variable = Ar+
potential = potential_ion
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_diffusion]
type = SakiyamaEnergyDiffusionBC
variable = mean_en
electrons = em
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[mean_en_Ar+_second_emissions]
type = SakiyamaEnergySecondaryElectronBC
variable = mean_en
electrons = em
ions = Ar+
potential = potential_ion
Tse_equal_Te = true
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = meta_density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_top_bc_func]
type = ParsedFunction
expression = '50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_bottom_bc_func]
type = ParsedFunction
expression = '-50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = 0
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e14)/6.022e23)'
[]
[meta_density_ic_func]
type = ParsedFunction
expression = 'log((1e16)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log((3./2.) * 4) + log((1e14)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = true
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_se_coeff = 0.00
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 1.44409938
diffusivity = 6.428571e-2
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-2
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_00]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_elastic.txt'
reaction = 'em + Ar -> em + Ar'
electrons = em
[]
[reaction_0]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
mean_energy = mean_en
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
reaction = 'em + Ar* -> em + Ar'
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
mean_energy = mean_en
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
reaction = 'em + Ar* -> em + em + Ar+'
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
mean_energy = mean_en
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
#end_time = 7.4e-3
end_time = 1e-7
dtmax = 1e-9
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-12
#nl_abs_tol = 7.6e-5
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
#[TimeSteppers]
# [Postprocessor]
# type = PostprocessorDT
# postprocessor = InversePlasmaFreq
# scale = 0.1
# []
#[]
[]
[Outputs]
file_base = '2D_RF_out'
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/Conference_Syntax_Tests/Lymberopoulos_with_argon_metastables_2D_At1Torr.i)
dom0Scale = 25.4e-3
#dom0Scale=1.0
[GlobalParams]
potential_units = V
use_moles = true
[]
[Mesh]
type = FileMesh
file = 'GEC_mesh.msh'
coord_type = RZ
rz_coord_axis = Y
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[potential_ion]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential_ion
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
# Energy loss from elastic collisions
[Elastic_loss]
type = EEDFElasticLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar'
[]
#Effective potential for the Ions
[Ion_potential_time_deriv]
type = TimeDerivative
variable = potential_ion
[]
[Ion_potential_reaction]
type = ScaledReaction
variable = potential_ion
collision_freq = 1283370.875
[]
[Ion_potential_coupled_force]
type = CoupledForce
variable = potential_ion
v = potential
coef = 1283370.875
[]
[]
[AuxVariables]
[emDeBug]
[]
[Ar+_DeBug]
[]
[Ar*_DeBug]
[]
[mean_enDeBug]
[]
[potential_DeBug]
[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[y]
order = CONSTANT
family = MONOMIAL
[]
[y_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efieldx]
order = CONSTANT
family = MONOMIAL
[]
[Efieldy]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[]
[AuxKernels]
#[emDeBug]
# type = DebugResidualAux
# variable = emDeBug
# debug_variable = em
#[]
#[Ar+_DeBug]
# type = DebugResidualAux
# variable = Ar+_DeBug
# debug_variable = Ar+
#[]
#[mean_enDeBug]
# type = DebugResidualAux
# variable = mean_enDeBug
# debug_variable = mean_en
#[]
#[Ar*_DeBug]
# type = DebugResidualAux
# variable = Ar*_DeBug
# debug_variable = Ar*
#[]
#[Potential_DeBug]
# type = DebugResidualAux
# variable = potential_DeBug
# debug_variable = potential
#[]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[y_g]
type = Position
variable = y
position_units = ${dom0Scale}
[]
[y_ng]
type = Position
variable = y_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efieldx_calc]
type = Efield
component = 0
potential = potential
variable = Efieldx
position_units = ${dom0Scale}
[]
[Efieldy_calc]
type = Efield
component = 1
potential = potential
variable = Efieldy
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential_ion
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_top_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Top_Electrode'
function = potential_top_bc_func
[]
[potential_bottom_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Bottom_Electrode'
function = potential_bottom_bc_func
[]
[potential_dirichlet_bottom_plate]
type = DirichletBC
variable = potential
boundary = 'Walls'
value = 0
[]
[potential_Dielectric]
type = EconomouDielectricBC
variable = potential
boundary = 'Top_Insulator Bottom_Insulator'
electrons = em
ions = Ar+
ion_potentials = potential_ion
electron_energy = mean_en
dielectric_constant = 1.859382e-11
thickness = 0.0127
emission_coeffs = 0.01
position_units = ${dom0Scale}
[]
#New Boundary conditions for electons, same as in paper
[em_physical_diffusion]
type = SakiyamaElectronDiffusionBC
variable = em
electron_energy = mean_en
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[em_Ar+_second_emissions]
type = SakiyamaSecondaryElectronBC
variable = em
potential = potential_ion
ions = Ar+
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_advection]
type = SakiyamaIonAdvectionBC
variable = Ar+
potential = potential_ion
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_diffusion]
type = SakiyamaEnergyDiffusionBC
variable = mean_en
electrons = em
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[mean_en_Ar+_second_emissions]
type = SakiyamaEnergySecondaryElectronBC
variable = mean_en
electrons = em
ions = Ar+
potential = potential_ion
Tse_equal_Te = true
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = meta_density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_top_bc_func]
type = ParsedFunction
expression = '30*sin(2*3.1415926*13.56e6*t)'
[]
[potential_bottom_bc_func]
type = ParsedFunction
expression = '-30*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = 0
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e14)/6.022e23)'
[]
[meta_density_ic_func]
type = ParsedFunction
expression = 'log((1e16)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log((3./2.)) + log((1e14)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = true
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_se_coeff = 0.00
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 1.44409938
diffusivity = 6.428571e-2
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-2
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_00]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_elastic.txt'
reaction = 'em + Ar -> em + Ar'
electrons = em
[]
[reaction_0]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
mean_energy = mean_en
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
mean_energy = mean_en
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 7.4e-3
automatic_scaling = true
dtmax = 1e-9
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-8
#nl_abs_tol = 7.6e-5
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
#[TimeSteppers]
# [Postprocessor]
# type = PostprocessorDT
# postprocessor = InversePlasmaFreq
# scale = 0.1
# []
#[]
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
#[emDeBug]
#[]
#[Ar+_DeBug]
#[]
#[Ar*_DeBug]
#[]
#[mean_enDeBug]
#[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efield]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[]
[AuxKernels]
#[emDeBug]
# type = DebugResidualAux
# variable = emDeBug
# debug_variable = em
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[Ar+_DeBug]
# type = DebugResidualAux
# variable = Ar+_DeBug
# debug_variable = Ar+
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[mean_enDeBug]
# type = DebugResidualAux
# variable = mean_enDeBug
# debug_variable = mean_en
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[Ar*_DeBug]
# type = DebugResidualAux
# variable = Ar*_DeBug
# debug_variable = Ar*
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = Efield
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
preset = false
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
preset = false
[]
#New Boundary conditions for electons, same as in paper
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 100
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = '0.100 * (25.4e-3 - x)'
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log(3./2.) + log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
#end_time = 0.00737463126
end_time = 3e-7
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-08
#nl_abs_tol = 7.6e-5 #Commit out do to test falure on Mac
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
[TimeSteppers]
[Postprocessor]
type = PostprocessorDT
postprocessor = InversePlasmaFreq
[]
[]
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/DriftDiffusionAction/RF_Plasma_no_actions.i)
#This is the input file that supplied the gold output file.
#It is the same as the input file in
#tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables.i,
#execpt some of the Aux Variables are renamed for the Action test
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
[e_temp]
order = CONSTANT
family = MONOMIAL
[]
[position]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_density]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_density]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_density]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[EFieldx]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
[]
[Current_Ar+]
order = CONSTANT
family = MONOMIAL
[]
[emRate]
order = CONSTANT
family = MONOMIAL
[]
[exRate]
order = CONSTANT
family = MONOMIAL
[]
[swRate]
order = CONSTANT
family = MONOMIAL
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
[]
[quRate]
order = CONSTANT
family = MONOMIAL
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
[]
[]
[AuxKernels]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[e_temp]
type = ElectronTemperature
variable = e_temp
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = position
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_density]
type = DensityMoles
variable = em_density
density_log = em
[]
[Ar+_density]
type = DensityMoles
variable = Ar+_density
density_log = Ar+
[]
[Ar*_density]
type = DensityMoles
variable = Ar*_density
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = EFieldx
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
position_units = ${dom0Scale}
[]
[Current_Ar+]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar+
art_diff = false
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
[]
#New Boundary conditions for electons, same as in paper
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#emission_coeffs = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#emission_coeffs = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 100
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = '0.100 * (25.4e-3 - x)'
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log(3./2.) + log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 3e-7
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
dtmin = 1e-14
l_max_its = 20
scheme = bdf2
dt = 1e-9
[]
[Outputs]
file_base = 'RF_out'
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/accelerations/Acceleration_By_Shooting_Method.i)
#This test starts the simulation at 50 rf cycle, then accelerates
#at the 55 rf cycle mark and stops at 57 rf cycles
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
file = 'Acceleration_By_Shooting_Method_Initial_Conditions.e'
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
initial_from_file_var = em
[]
[Ar+]
initial_from_file_var = Ar+
[]
[Ar*]
initial_from_file_var = Ar*
[]
[mean_en]
initial_from_file_var = mean_en
[]
[potential]
initial_from_file_var = potential
[]
[]
[Kernels]
#Electron Equations
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
mean_energy = mean_en
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
mean_energy = mean_en
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
mean_energy = mean_en
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
mean_energy = mean_en
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Electron Energy Equations
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efield]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[]
[AuxKernels]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = Efield
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
preset = false
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
preset = false
[]
#Boundary conditions for electons
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#Boundary conditions for ions
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for metastables
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 1e-5
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 1e-5
[]
#Boundary conditions for electron mean energy
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*pi*13.56e6*t)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar -> em + Ar*.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar -> em + em + Ar+.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar* -> em + Ar.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar* -> em + em + Ar+.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-43
reaction_rate_value = 39890.9324
[]
[]
[MultiApps]
#MultiApp of Acceleration by Shooting Method
[Shooting]
type = FullSolveMultiApp
input_files = 'Acceleration_By_Shooting_Method_Shooting.i'
execute_on = 'TIMESTEP_END'
enable = false
[]
[]
[Transfers]
#MultiApp Transfers for Acceleration by Shooting Method
[em_to_Shooting]
type = MultiAppCopyTransfer
to_multi_app = Shooting
source_variable = em
variable = em
enable = false
[]
[Ar+_to_Shooting]
type = MultiAppCopyTransfer
to_multi_app = Shooting
source_variable = Ar+
variable = Ar+
enable = false
[]
[mean_en_to_Shooting]
type = MultiAppCopyTransfer
to_multi_app = Shooting
source_variable = mean_en
variable = mean_en
enable = false
[]
[potential_to_Shooting]
type = MultiAppCopyTransfer
to_multi_app = Shooting
source_variable = potential
variable = potential
enable = false
[]
[Ar*_to_Shooting]
type = MultiAppCopyTransfer
to_multi_app = Shooting
source_variable = Ar*
variable = Ar*
enable = false
[]
[Ar*S_to_Shooting]
type = MultiAppCopyTransfer
to_multi_app = Shooting
source_variable = Ar*
variable = Ar*S
enable = false
[]
[Ar*New_from_Shooting]
type = MultiAppCopyTransfer
from_multi_app = Shooting
source_variable = Ar*
variable = Ar*
enable = false
[]
[]
#The Action the add the TimePeriod Controls to turn off and on the MultiApps
[PeriodicControllers]
[Shooting]
Enable_at_cycle_start = 'MultiApps::Shooting
Transfers::em_to_Shooting *::Ar+_to_Shooting *::mean_en_to_Shooting
*::potential_to_Shooting *::Ar*_to_Shooting *::Ar*S_to_Shooting
Transfers::Ar*New_from_Shooting'
starting_cycle = 55
cycle_frequency = 13.56e6
cycles_between_controls = 30
num_controller_set = 2000
name = Shooting
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
start_time = 3.68731563e-6
end_time = 4.20353982e-6
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
dtmin = 1e-14
l_max_its = 20
scheme = bdf2
dt = 1e-9
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/accelerations/Acceleration_By_Averaging_main.i)
#This test runs the simulation for 10 rf cycle, then accelerates
#once and stops at 11 rf cycles
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos_paper.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[]
[Kernels]
#Electron Equations
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
mean_energy = mean_en
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
mean_energy = mean_en
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
mean_energy = mean_en
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
mean_energy = mean_en
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Electron Energy Equations
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efield]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[]
[AuxKernels]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = Efield
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
preset = false
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
preset = false
[]
#Boundary conditions for electons
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#gamma = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#Boundary conditions for ions
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for metastables
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 1e-5
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 1e-5
[]
#Boundary conditions for electron mean energy
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*pi*13.56e6*t)'
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e14)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log((3./2.) * ((1e14)/6.022e23))'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar -> em + Ar*.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar -> em + em + Ar+.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar* -> em + Ar.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/reaction_em + Ar* -> em + em + Ar+.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-43
reaction_rate_value = 39890.9324
[]
[]
[MultiApps]
#MultiApp of Acceleration by Averaging
[Averaging_Acceleration]
type = FullSolveMultiApp
input_files = 'Acceleration_By_Averaging_acceleration.i'
execute_on = 'TIMESTEP_END'
enable = false
[]
[]
[Transfers]
#MultiApp Transfers for Acceleration by Averaging
[em_to_Averaging]
type = MultiAppCopyTransfer
to_multi_app = Averaging_Acceleration
source_variable = em
variable = em
enable = false
[]
[Ar+_to_Averaging]
type = MultiAppCopyTransfer
to_multi_app = Averaging_Acceleration
source_variable = Ar+
variable = Ar+
enable = false
[]
[mean_en_to_Averaging]
type = MultiAppCopyTransfer
to_multi_app = Averaging_Acceleration
source_variable = mean_en
variable = mean_en
enable = false
[]
[potential_to_Averaging]
type = MultiAppCopyTransfer
to_multi_app = Averaging_Acceleration
source_variable = potential
variable = potential
enable = false
[]
[Ar*_to_Averaging]
type = MultiAppCopyTransfer
to_multi_app = Averaging_Acceleration
source_variable = Ar*
variable = Ar*
enable = false
[]
[Ar*S_to_Averaging]
type = MultiAppCopyTransfer
to_multi_app = Averaging_Acceleration
source_variable = Ar*
variable = Ar*S
enable = false
[]
[Ar*New_from_Averaging]
type = MultiAppCopyTransfer
from_multi_app = Averaging_Acceleration
source_variable = Ar*
variable = Ar*
enable = false
[]
[]
#The Action the add the TimePeriod Controls to turn off and on the MultiApps
[PeriodicControllers]
[Averaging_Acceleration]
Enable_at_cycle_start = 'MultiApps::Averaging_Acceleration
Transfers::em_to_Averaging *::Ar+_to_Averaging *::mean_en_to_Averaging
*::potential_to_Averaging *::Ar*_to_Averaging *::Ar*S_to_Averaging
Transfers::Ar*New_from_Averaging'
starting_cycle = 10
cycle_frequency = 13.56e6
cycles_between_controls = 10
num_controller_set = 15
name = Averaging_Acceleration
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 8.2e-7
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
dtmin = 1e-14
l_max_its = 20
scheme = bdf2
dt = 1e-9
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/DriftDiffusionAction/2D_RF_Plasma_actions.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = V
use_moles = true
[]
[Mesh]
type = FileMesh
file = 'GEC_mesh_coarse.msh'
coord_type = RZ
rz_coord_axis = Y
[]
#Effective potentials and their kernels are not defined by the
#DriftDiffusionAction, but charged particles effective by
#this potential can by defined by the action.
[Variables]
[potential_ion]
[]
[]
#Action the supplies the drift-diffusion equations
#This action also adds JouleHeating and the ChargeSourceMoles_KV Kernels
[DriftDiffusionAction]
[Plasma]
electrons = em
secondary_charged_particles = Ar+
Neutrals = Ar*
mean_energy = mean_en
potential = potential
eff_potentials = potential_ion
Is_potential_unique = true
using_offset = false
position_units = ${dom0Scale}
Additional_Outputs = 'ElectronTemperature Current EField'
[]
[]
#The Kernels supply the sources terms
[Kernels]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
# Energy loss from elastic collisions
[Elastic_loss]
type = EEDFElasticLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar'
[]
#Effective potential for the Ions
[Ion_potential_time_deriv]
type = TimeDerivative
variable = potential_ion
[]
[Ion_potential_reaction]
type = ScaledReaction
variable = potential_ion
collision_freq = 1283370.875
[]
[Ion_potential_coupled_force]
type = CoupledForce
variable = potential_ion
v = potential
coef = 1283370.875
[]
[]
[AuxVariables]
[x_node]
[]
[y_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[]
[AuxKernels]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[x_ng]
type = Position
variable = x_node
component = 0
position_units = ${dom0Scale}
[]
[y_ng]
type = Position
variable = y_node
component = 1
position_units = ${dom0Scale}
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e2
value = -5.231208
execute_on = INITIAL
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_top_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Top_Electrode'
function = potential_top_bc_func
preset = false
[]
[potential_bottom_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Bottom_Electrode'
function = potential_bottom_bc_func
preset = false
[]
[potential_dirichlet_bottom_plate]
type = DirichletBC
variable = potential
boundary = 'Walls'
value = 0
preset = false
[]
[potential_Dielectric]
type = EconomouDielectricBC
variable = potential
boundary = 'Top_Insulator Bottom_Insulator'
electrons = em
ions = Ar+
ion_potentials = potential_ion
electron_energy = mean_en
dielectric_constant = 1.859382e-11
thickness = 0.0127
emission_coeffs = 0.01
position_units = ${dom0Scale}
[]
#New Boundary conditions for electons, same as in paper
[em_physical_diffusion]
type = SakiyamaElectronDiffusionBC
variable = em
electron_energy = mean_en
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[em_Ar+_second_emissions]
type = SakiyamaSecondaryElectronBC
variable = em
potential = potential_ion
ions = Ar+
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_advection]
type = SakiyamaIonAdvectionBC
variable = Ar+
potential = potential_ion
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_diffusion]
type = SakiyamaEnergyDiffusionBC
variable = mean_en
electrons = em
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[mean_en_Ar+_second_emissions]
type = SakiyamaEnergySecondaryElectronBC
variable = mean_en
electrons = em
ions = Ar+
potential = potential_ion
Tse_equal_Te = true
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = meta_density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_top_bc_func]
type = ParsedFunction
expression = '50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_bottom_bc_func]
type = ParsedFunction
expression = '-50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = 0
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e14)/6.022e23)'
[]
[meta_density_ic_func]
type = ParsedFunction
expression = 'log((1e16)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log((3./2.) * 4) + log((1e14)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = true
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_se_coeff = 0.00
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 1.44409938
diffusivity = 6.428571e-2
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-2
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_00]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_elastic.txt'
reaction = 'em + Ar -> em + Ar'
electrons = em
[]
[reaction_0]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
mean_energy = mean_en
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
reaction = 'em + Ar* -> em + Ar'
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
mean_energy = mean_en
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
reaction = 'em + Ar* -> em + em + Ar+'
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
mean_energy = mean_en
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
#end_time = 7.4e-3
end_time = 1e-7
dtmax = 1e-9
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-12
#nl_abs_tol = 7.6e-5
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
#[TimeSteppers]
# [Postprocessor]
# type = PostprocessorDT
# postprocessor = InversePlasmaFreq
# scale = 0.1
# []
#[]
[]
[Outputs]
file_base = '2D_RF_out'
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/Conference_Syntax_Tests/Lymberopoulos_with_argon_metastables_2D_At100mTorr.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = V
use_moles = true
[]
[Mesh]
type = FileMesh
file = 'GEC_mesh.msh'
coord_type = RZ
rz_coord_axis = Y
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[potential_ion]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential_ion
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
# Energy loss from elastic collisions
[Elastic_loss]
type = EEDFElasticLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar'
[]
#Effective potential for the Ions
[Ion_potential_time_deriv]
type = TimeDerivative
variable = potential_ion
[]
[Ion_potential_reaction]
type = ScaledReaction
variable = potential_ion
collision_freq = 1283370.875
[]
[Ion_potential_coupled_force]
type = CoupledForce
variable = potential_ion
v = potential
coef = 1283370.875
[]
[]
[AuxVariables]
[emDeBug]
[]
[Ar+_DeBug]
[]
[Ar*_DeBug]
[]
[mean_enDeBug]
[]
[potential_DeBug]
[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[y]
order = CONSTANT
family = MONOMIAL
[]
[y_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efieldx]
order = CONSTANT
family = MONOMIAL
[]
[Efieldy]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[]
[AuxKernels]
#[emDeBug]
# type = DebugResidualAux
# variable = emDeBug
# debug_variable = em
#[]
#[Ar+_DeBug]
# type = DebugResidualAux
# variable = Ar+_DeBug
# debug_variable = Ar+
#[]
#[mean_enDeBug]
# type = DebugResidualAux
# variable = mean_enDeBug
# debug_variable = mean_en
#[]
#[Ar*_DeBug]
# type = DebugResidualAux
# variable = Ar*_DeBug
# debug_variable = Ar*
#[]
#[Potential_DeBug]
# type = DebugResidualAux
# variable = potential_DeBug
# debug_variable = potential
#[]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[y_g]
type = Position
variable = y
position_units = ${dom0Scale}
[]
[y_ng]
type = Position
variable = y_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e2
value = -5.231208
execute_on = INITIAL
[]
[Efieldx_calc]
type = Efield
component = 0
potential = potential
variable = Efieldx
position_units = ${dom0Scale}
[]
[Efieldy_calc]
type = Efield
component = 1
potential = potential
variable = Efieldy
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential_ion
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_top_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Top_Electrode'
function = potential_top_bc_func
[]
[potential_bottom_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Bottom_Electrode'
function = potential_bottom_bc_func
[]
[potential_dirichlet_bottom_plate]
type = DirichletBC
variable = potential
boundary = 'Walls'
value = 0
[]
[potential_Dielectric]
type = EconomouDielectricBC
variable = potential
boundary = 'Top_Insulator Bottom_Insulator'
electrons = em
ions = Ar+
ion_potentials = potential_ion
electron_energy = mean_en
dielectric_constant = 1.859382e-11
thickness = 0.0127
emission_coeffs = 0.01
position_units = ${dom0Scale}
[]
#New Boundary conditions for electons, same as in paper
[em_physical_diffusion]
type = SakiyamaElectronDiffusionBC
variable = em
electron_energy = mean_en
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[em_Ar+_second_emissions]
type = SakiyamaSecondaryElectronBC
variable = em
potential = potential_ion
ions = Ar+
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_advection]
type = SakiyamaIonAdvectionBC
variable = Ar+
potential = potential_ion
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_diffusion]
type = SakiyamaEnergyDiffusionBC
variable = mean_en
electrons = em
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[mean_en_Ar+_second_emissions]
type = SakiyamaEnergySecondaryElectronBC
variable = mean_en
electrons = em
ions = Ar+
potential = potential_ion
Tse_equal_Te = true
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = meta_density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_top_bc_func]
type = ParsedFunction
expression = '50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_bottom_bc_func]
type = ParsedFunction
expression = '-50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = 0
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e14)/6.022e23)'
[]
[meta_density_ic_func]
type = ParsedFunction
expression = 'log((1e16)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log((3./2.) * 4) + log((1e14)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = true
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_se_coeff = 0.00
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 1.44409938
diffusivity = 6.428571e-2
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-2
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_00]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_elastic.txt'
reaction = 'em + Ar -> em + Ar'
electrons = em
[]
[reaction_0]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
mean_energy = mean_en
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
mean_energy = mean_en
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 7.4e-3
dtmax = 1e-9
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-8
#nl_abs_tol = 7.6e-5
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
#[TimeSteppers]
# [Postprocessor]
# type = PostprocessorDT
# postprocessor = InversePlasmaFreq
# scale = 0.1
# []
#[]
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/DriftDiffusionAction/RF_Plasma_actions.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
#Action the supplies the drift-diffusion equations
#This action also adds JouleHeating and the ChargeSourceMoles_KV Kernels
[DriftDiffusionAction]
[Plasma]
electrons = em
charged_particle = Ar+
Neutrals = Ar*
mean_energy = mean_en
potential = potential
Is_potential_unique = true
using_offset = false
position_units = ${dom0Scale}
Additional_Outputs = 'ElectronTemperature Current EField'
[]
[]
#The Kernels supply the sources terms
[Kernels]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
[x_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[emRate]
order = CONSTANT
family = MONOMIAL
[]
[exRate]
order = CONSTANT
family = MONOMIAL
[]
[swRate]
order = CONSTANT
family = MONOMIAL
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
[]
[quRate]
order = CONSTANT
family = MONOMIAL
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
[]
[]
[AuxKernels]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
preset = false
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
preset = false
[]
#New Boundary conditions for electons, same as in paper
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#emission_coeffs = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#emission_coeffs = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 100
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = '0.100 * (25.4e-3 - x)'
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log(3./2.) + log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 3e-7
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
dtmin = 1e-14
l_max_its = 20
scheme = bdf2
dt = 1e-9
[]
[Outputs]
file_base = 'RF_out'
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/Conference_Syntax_Tests/Lymberopoulos_with_argon_metastables.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = kV
use_moles = true
[]
[Mesh]
[file]
type = FileMeshGenerator
file = 'Lymberopoulos.msh'
[]
[left]
type = SideSetsFromNormalsGenerator
normals = '-1 0 0'
new_boundary = 'left'
input = file
[]
[right]
type = SideSetsFromNormalsGenerator
normals = '1 0 0'
new_boundary = 'right'
input = left
[]
[]
[Problem]
type = FEProblem
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
[]
[AuxVariables]
#[emDeBug]
#[]
#[Ar+_DeBug]
#[]
#[Ar*_DeBug]
#[]
#[mean_enDeBug]
#[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efield]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 0
[]
[]
[AuxKernels]
#[emDeBug]
# type = DebugResidualAux
# variable = emDeBug
# debug_variable = em
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[Ar+_DeBug]
# type = DebugResidualAux
# variable = Ar+_DeBug
# debug_variable = Ar+
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[mean_enDeBug]
# type = DebugResidualAux
# variable = mean_enDeBug
# debug_variable = mean_en
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
#[Ar*_DeBug]
# type = DebugResidualAux
# variable = Ar*_DeBug
# debug_variable = Ar*
# #execute_on = 'LINEAR NONLINEAR TIMESTEP_BEGIN'
#[]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e22
value = -2.928623
execute_on = INITIAL
[]
[Efield_calc]
type = Efield
component = 0
potential = potential
variable = Efield
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 0
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_left]
type = FunctionDirichletBC
variable = potential
boundary = 'left'
function = potential_bc_func
[]
[potential_dirichlet_right]
type = DirichletBC
variable = potential
boundary = 'right'
value = 0
[]
#New Boundary conditions for electons, same as in paper
[em_physical_right]
type = LymberopoulosElectronBC
variable = em
boundary = 'right'
emission_coeffs = 0.01
#emission_coeffs = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
[em_physical_left]
type = LymberopoulosElectronBC
variable = em
boundary = 'left'
emission_coeffs = 0.01
#emission_coeffs = 1
ks = 1.19e5
#ks = 0.0
ions = Ar+
potential = potential
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_right_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'right'
position_units = ${dom0Scale}
[]
[Ar+_physical_left_advection]
type = LymberopoulosIonBC
variable = Ar+
potential = potential
boundary = 'left'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_right_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'right'
value = 100
[]
[Ar*_physical_left_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'left'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_right]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'right'
[]
[mean_en_physical_left]
type = ElectronTemperatureDirichletBC
variable = mean_en
electrons = em
value = 0.5
boundary = 'left'
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_bc_func]
type = ParsedFunction
expression = '0.100*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = '0.100 * (25.4e-3 - x)'
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log(3./2.) + log((1e13 + 1e15 * (1-x/1)^2 * (x/1)^2)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = false
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_electron_mobility = 30.0
user_electron_diffusion_coeff = 119.8757763975
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 0.144409938
diffusivity = 6.428571e-3
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-3
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_0]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
reaction = 'em + Ar* -> em + Ar'
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
reaction = 'em + Ar* -> em + em + Ar+'
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
end_time = 0.00737463126
#end_time = 3e-7
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-08
#nl_abs_tol = 7.6e-5 #Commit out do to test falure on Mac
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
[TimeSteppers]
[Postprocessor]
type = PostprocessorDT
postprocessor = InversePlasmaFreq
[]
[]
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]
(test/tests/Lymberopoulos_rf_discharge/Lymberopoulos_with_argon_metastables_2D_At100mTorr_CoarseMesh.i)
dom0Scale = 25.4e-3
[GlobalParams]
potential_units = V
use_moles = true
[]
[Mesh]
type = FileMesh
file = 'GEC_mesh_coarse.msh'
coord_type = RZ
rz_coord_axis = Y
[]
[Variables]
[em]
[]
[Ar+]
[]
[Ar*]
[]
[mean_en]
[]
[potential]
[]
[potential_ion]
[]
[]
[Kernels]
#Electron Equations (Same as in paper)
#Time Derivative term of electron
[em_time_deriv]
type = ElectronTimeDerivative
variable = em
[]
#Advection term of electron
[em_advection]
type = EFieldAdvection
variable = em
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons
[em_diffusion]
type = CoeffDiffusion
variable = em
position_units = ${dom0Scale}
[]
#Net electron production from ionization
[em_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from step-wise ionization
[em_stepwise_ionization]
type = EEDFReactionLog
variable = em
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net electron production from metastable pooling
[em_pooling]
type = ReactionSecondOrderLog
variable = em
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Ion Equations (Same as in paper)
#Time Derivative term of the ions
[Ar+_time_deriv]
type = ElectronTimeDerivative
variable = Ar+
[]
#Advection term of ions
[Ar+_advection]
type = EFieldAdvection
variable = Ar+
potential = potential_ion
position_units = ${dom0Scale}
[]
[Ar+_diffusion]
type = CoeffDiffusion
variable = Ar+
position_units = ${dom0Scale}
[]
#Net ion production from ionization
[Ar+_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from step-wise ionization
[Ar+_stepwise_ionization]
type = EEDFReactionLog
variable = Ar+
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = 1
[]
#Net ion production from metastable pooling
[Ar+_pooling]
type = ReactionSecondOrderLog
variable = Ar+
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = 1
[]
#Argon Excited Equations (Same as in paper)
#Time Derivative term of excited Argon
[Ar*_time_deriv]
type = ElectronTimeDerivative
variable = Ar*
[]
#Diffusion term of excited Argon
[Ar*_diffusion]
type = CoeffDiffusion
variable = Ar*
position_units = ${dom0Scale}
[]
#Net excited Argon production from excitation
[Ar*_excitation]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar
mean_energy = mean_en
reaction = 'em + Ar -> em + Ar*'
coefficient = 1
[]
#Net excited Argon loss from step-wise ionization
[Ar*_stepwise_ionization]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + em + Ar+'
coefficient = -1
[]
#Net excited Argon loss from superelastic collisions
[Ar*_collisions]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar'
coefficient = -1
[]
#Net excited Argon loss from quenching to resonant
[Ar*_quenching]
type = EEDFReactionLog
variable = Ar*
electrons = em
target = Ar*
mean_energy = mean_en
reaction = 'em + Ar* -> em + Ar_r'
coefficient = -1
[]
#Net excited Argon loss from metastable pooling
[Ar*_pooling]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
coefficient = -2
_v_eq_u = true
_w_eq_u = true
[]
#Net excited Argon loss from two-body quenching
[Ar*_2B_quenching]
type = ReactionSecondOrderLog
variable = Ar*
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
coefficient = -1
_v_eq_u = true
[]
#Net excited Argon loss from three-body quenching
[Ar*_3B_quenching]
type = ReactionThirdOrderLog
variable = Ar*
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
coefficient = -1
_v_eq_u = true
[]
#Voltage Equations (Same as in paper)
#Voltage term in Poissons Eqaution
[potential_diffusion_dom0]
type = CoeffDiffusionLin
variable = potential
position_units = ${dom0Scale}
[]
#Ion term in Poissons Equation
[Ar+_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = Ar+
[]
#Electron term in Poissons Equation
[em_charge_source]
type = ChargeSourceMoles_KV
variable = potential
charged = em
[]
#Since the paper uses electron temperature as a variable, the energy equation is in
#a different form but should be the same physics
#Time Derivative term of electron energy
[mean_en_time_deriv]
type = ElectronTimeDerivative
variable = mean_en
[]
#Advection term of electron energy
[mean_en_advection]
type = EFieldAdvection
variable = mean_en
potential = potential
position_units = ${dom0Scale}
[]
#Diffusion term of electrons energy
[mean_en_diffusion]
type = CoeffDiffusion
variable = mean_en
position_units = ${dom0Scale}
[]
#Joule Heating term
[mean_en_joule_heating]
type = JouleHeating
variable = mean_en
potential = potential
em = em
position_units = ${dom0Scale}
[]
#Energy loss from ionization
[Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + em + Ar+'
threshold_energy = -15.7
[]
#Energy loss from excitation
[Excitation_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar*'
threshold_energy = -11.56
[]
#Energy loss from step-wise ionization
[Stepwise_Ionization_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
threshold_energy = -4.14
[]
#Energy gain from superelastic collisions
[Collisions_Loss]
type = EEDFEnergyLog
variable = mean_en
electrons = em
target = Ar*
reaction = 'em + Ar* -> em + Ar'
threshold_energy = 11.56
[]
# Energy loss from elastic collisions
[Elastic_loss]
type = EEDFElasticLog
variable = mean_en
electrons = em
target = Ar
reaction = 'em + Ar -> em + Ar'
[]
#Effective potential for the Ions
[Ion_potential_time_deriv]
type = TimeDerivative
variable = potential_ion
[]
[Ion_potential_reaction]
type = ScaledReaction
variable = potential_ion
collision_freq = 1283370.875
[]
[Ion_potential_coupled_force]
type = CoupledForce
variable = potential_ion
v = potential
coef = 1283370.875
[]
[]
[AuxVariables]
[emDeBug]
[]
[Ar+_DeBug]
[]
[Ar*_DeBug]
[]
[mean_enDeBug]
[]
[potential_DeBug]
[]
[Te]
order = CONSTANT
family = MONOMIAL
[]
[x]
order = CONSTANT
family = MONOMIAL
[]
[x_node]
[]
[y]
order = CONSTANT
family = MONOMIAL
[]
[y_node]
[]
[rho]
order = CONSTANT
family = MONOMIAL
[]
[em_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar+_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar*_lin]
order = CONSTANT
family = MONOMIAL
[]
[Ar]
[]
[Efieldx]
order = CONSTANT
family = MONOMIAL
[]
[Efieldy]
order = CONSTANT
family = MONOMIAL
[]
[Current_em]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[Current_Ar]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[emRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[exRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[swRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[deexRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[quRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[poolRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[TwoBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[ThreeBRate]
order = CONSTANT
family = MONOMIAL
block = 'plasma'
[]
[]
[AuxKernels]
#[emDeBug]
# type = DebugResidualAux
# variable = emDeBug
# debug_variable = em
#[]
#[Ar+_DeBug]
# type = DebugResidualAux
# variable = Ar+_DeBug
# debug_variable = Ar+
#[]
#[mean_enDeBug]
# type = DebugResidualAux
# variable = mean_enDeBug
# debug_variable = mean_en
#[]
#[Ar*_DeBug]
# type = DebugResidualAux
# variable = Ar*_DeBug
# debug_variable = Ar*
#[]
#[Potential_DeBug]
# type = DebugResidualAux
# variable = potential_DeBug
# debug_variable = potential
#[]
[emRate]
type = ProcRateForRateCoeff
variable = emRate
v = em
w = Ar
reaction = 'em + Ar -> em + em + Ar+'
[]
[exRate]
type = ProcRateForRateCoeff
variable = exRate
v = em
w = Ar*
reaction = 'em + Ar -> em + Ar*'
[]
[swRate]
type = ProcRateForRateCoeff
variable = swRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + em + Ar+'
[]
[deexRate]
type = ProcRateForRateCoeff
variable = deexRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar'
[]
[quRate]
type = ProcRateForRateCoeff
variable = quRate
v = em
w = Ar*
reaction = 'em + Ar* -> em + Ar_r'
[]
[poolRate]
type = ProcRateForRateCoeff
variable = poolRate
v = Ar*
w = Ar*
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
[]
[TwoBRate]
type = ProcRateForRateCoeff
variable = TwoBRate
v = Ar*
w = Ar
reaction = 'Ar* + Ar -> Ar + Ar'
[]
[ThreeBRate]
type = ProcRateForRateCoeffThreeBody
variable = ThreeBRate
v = Ar*
w = Ar
x = Ar
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
[]
[Te]
type = ElectronTemperature
variable = Te
electron_density = em
mean_en = mean_en
[]
[x_g]
type = Position
variable = x
position_units = ${dom0Scale}
[]
[x_ng]
type = Position
variable = x_node
position_units = ${dom0Scale}
[]
[y_g]
type = Position
variable = y
position_units = ${dom0Scale}
[]
[y_ng]
type = Position
variable = y_node
position_units = ${dom0Scale}
[]
[em_lin]
type = DensityMoles
variable = em_lin
density_log = em
[]
[Ar+_lin]
type = DensityMoles
variable = Ar+_lin
density_log = Ar+
[]
[Ar*_lin]
type = DensityMoles
variable = Ar*_lin
density_log = Ar*
[]
[Ar_val]
type = ConstantAux
variable = Ar
# value = 3.22e2
value = -5.231208
execute_on = INITIAL
[]
[Efieldx_calc]
type = Efield
component = 0
potential = potential
variable = Efieldx
position_units = ${dom0Scale}
[]
[Efieldy_calc]
type = Efield
component = 1
potential = potential
variable = Efieldy
position_units = ${dom0Scale}
[]
[Current_em]
type = ADCurrent
potential = potential
density_log = em
variable = Current_em
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[Current_Ar]
type = ADCurrent
potential = potential_ion
density_log = Ar+
variable = Current_Ar
art_diff = false
block = 'plasma'
position_units = ${dom0Scale}
[]
[]
[BCs]
#Voltage Boundary Condition, same as in paper
[potential_top_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Top_Electrode'
function = potential_top_bc_func
preset = false
[]
[potential_bottom_plate]
type = FunctionDirichletBC
variable = potential
boundary = 'Bottom_Electrode'
function = potential_bottom_bc_func
preset = false
[]
[potential_dirichlet_bottom_plate]
type = DirichletBC
variable = potential
boundary = 'Walls'
value = 0
preset = false
[]
[potential_Dielectric]
type = EconomouDielectricBC
variable = potential
boundary = 'Top_Insulator Bottom_Insulator'
electrons = em
ions = Ar+
ion_potentials = potential_ion
electron_energy = mean_en
dielectric_constant = 1.859382e-11
thickness = 0.0127
emission_coeffs = 0.01
position_units = ${dom0Scale}
[]
#New Boundary conditions for electons, same as in paper
[em_physical_diffusion]
type = SakiyamaElectronDiffusionBC
variable = em
electron_energy = mean_en
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[em_Ar+_second_emissions]
type = SakiyamaSecondaryElectronBC
variable = em
potential = potential_ion
ions = Ar+
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
[Ar+_physical_advection]
type = SakiyamaIonAdvectionBC
variable = Ar+
potential = potential_ion
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
#New Boundary conditions for ions, should be the same as in paper
#(except the metastables are not set to zero, since Zapdos uses log form)
[Ar*_physical_diffusion]
type = LogDensityDirichletBC
variable = Ar*
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
value = 100
[]
#New Boundary conditions for mean energy, should be the same as in paper
[mean_en_physical_diffusion]
type = SakiyamaEnergyDiffusionBC
variable = mean_en
electrons = em
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[mean_en_Ar+_second_emissions]
type = SakiyamaEnergySecondaryElectronBC
variable = mean_en
electrons = em
ions = Ar+
potential = potential_ion
Tse_equal_Te = true
emission_coeffs = 0.01
boundary = 'Top_Electrode Bottom_Electrode Top_Insulator Bottom_Insulator Walls'
position_units = ${dom0Scale}
[]
[]
[ICs]
[em_ic]
type = FunctionIC
variable = em
function = density_ic_func
[]
[Ar+_ic]
type = FunctionIC
variable = Ar+
function = density_ic_func
[]
[Ar*_ic]
type = FunctionIC
variable = Ar*
function = meta_density_ic_func
[]
[mean_en_ic]
type = FunctionIC
variable = mean_en
function = energy_density_ic_func
[]
[potential_ic]
type = FunctionIC
variable = potential
function = potential_ic_func
[]
[]
[Functions]
[potential_top_bc_func]
type = ParsedFunction
expression = '50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_bottom_bc_func]
type = ParsedFunction
expression = '-50*sin(2*3.1415926*13.56e6*t)'
[]
[potential_ic_func]
type = ParsedFunction
expression = 0
[]
[density_ic_func]
type = ParsedFunction
expression = 'log((1e14)/6.022e23)'
[]
[meta_density_ic_func]
type = ParsedFunction
expression = 'log((1e16)/6.022e23)'
[]
[energy_density_ic_func]
type = ParsedFunction
expression = 'log((3./2.) * 4) + log((1e14)/6.022e23)'
[]
[]
[Materials]
[GasBasics]
type = GasElectronMoments
interp_trans_coeffs = true
interp_elastic_coeff = false
ramp_trans_coeffs = false
user_p_gas = 133.322
em = em
potential = potential
mean_en = mean_en
user_se_coeff = 0.00
property_tables_file = Argon_reactions_paper_RateCoefficients/electron_moments.txt
[]
[gas_species_0]
type = ADHeavySpecies
heavy_species_name = Ar+
heavy_species_mass = 6.64e-26
heavy_species_charge = 1.0
mobility = 1.44409938
diffusivity = 6.428571e-2
[]
[gas_species_1]
type = ADHeavySpecies
heavy_species_name = Ar*
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
diffusivity = 7.515528e-2
[]
[gas_species_2]
type = ADHeavySpecies
heavy_species_name = Ar
heavy_species_mass = 6.64e-26
heavy_species_charge = 0.0
[]
[reaction_00]
type = ZapdosEEDFRateConstant
mean_energy = mean_en
property_file = 'Argon_reactions_paper_RateCoefficients/ar_elastic.txt'
reaction = 'em + Ar -> em + Ar'
electrons = em
[]
[reaction_0]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excitation.txt'
reaction = 'em + Ar -> em + Ar*'
mean_energy = mean_en
electrons = em
[]
[reaction_1]
type = ZapdosEEDFRateConstant
property_file = 'Argon_reactions_paper_RateCoefficients/ar_ionization.txt'
reaction = 'em + Ar -> em + em + Ar+'
mean_energy = mean_en
electrons = em
[]
[reaction_2]
type = ZapdosEEDFRateConstant
reaction = 'em + Ar* -> em + Ar'
property_file = 'Argon_reactions_paper_RateCoefficients/ar_deexcitation.txt'
mean_energy = mean_en
electrons = em
[]
[reaction_3]
type = ZapdosEEDFRateConstant
reaction = 'em + Ar* -> em + em + Ar+'
property_file = 'Argon_reactions_paper_RateCoefficients/ar_excited_ionization.txt'
mean_energy = mean_en
electrons = em
[]
[reaction_4]
type = GenericRateConstant
reaction = 'em + Ar* -> em + Ar_r'
#reaction_rate_value = 2e-13
reaction_rate_value = 1.2044e11
[]
[reaction_5]
type = GenericRateConstant
reaction = 'Ar* + Ar* -> Ar+ + Ar + em'
#reaction_rate_value = 6.2e-16
reaction_rate_value = 373364000
[]
[reaction_6]
type = GenericRateConstant
reaction = 'Ar* + Ar -> Ar + Ar'
#reaction_rate_value = 3e-21
reaction_rate_value = 1806.6
[]
[reaction_7]
type = GenericRateConstant
reaction = 'Ar* + Ar + Ar -> Ar_2 + Ar'
#reaction_rate_value = 1.1e-42
reaction_rate_value = 398909.324
[]
[]
#New postprocessor that calculates the inverse of the plasma frequency
[Postprocessors]
[InversePlasmaFreq]
type = PlasmaFrequencyInverse
variable = em
use_moles = true
execute_on = 'INITIAL TIMESTEP_BEGIN'
[]
[]
[Preconditioning]
active = 'smp'
[smp]
type = SMP
full = true
[]
[fdp]
type = FDP
full = true
[]
[]
[Executioner]
type = Transient
#end_time = 7.4e-3
end_time = 1e-7
dtmax = 1e-9
petsc_options = '-snes_converged_reason -snes_linesearch_monitor'
solve_type = NEWTON
petsc_options_iname = '-pc_type -pc_factor_shift_type -pc_factor_shift_amount -ksp_type -snes_linesearch_minlambda'
petsc_options_value = 'lu NONZERO 1.e-10 fgmres 1e-3'
nl_rel_tol = 1e-12
#nl_abs_tol = 7.6e-5
dtmin = 1e-14
l_max_its = 20
#Time steps based on the inverse of the plasma frequency
#[TimeSteppers]
# [Postprocessor]
# type = PostprocessorDT
# postprocessor = InversePlasmaFreq
# scale = 0.1
# []
#[]
[]
[Outputs]
perf_graph = true
[out]
type = Exodus
[]
[]