Cantera
3.0.0
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Base class for transport property managers. More...
#include <Transport.h>
Base class for transport property managers.
All classes that compute transport properties for a single phase derive from this class. Class Transport is meant to be used as a base class only. It is possible to instantiate it, but its methods throw exceptions if called.
This section describes how calculations are carried out within the Transport class. The Transport class and derived classes of the the Transport class necessarily use the ThermoPhase class to obtain the list of species and the thermodynamic state of the phase.
No state information is stored within Transport classes. Queries to the underlying ThermoPhase object must be made to obtain the state of the system.
An exception to this however is the state information concerning the the gradients of variables. This information is not stored within the ThermoPhase objects. It may be collected within the Transport objects. In fact, the meaning of const operations within the Transport class refers to calculations which do not change the state of the system nor the state of the first order gradients of the system.
When a const operation is evoked within the Transport class, it is also implicitly assumed that the underlying state within the ThermoPhase object has not changed its values.
The diffusion fluxes must be referenced to a particular reference fluid velocity. Most typical is to reference the diffusion fluxes to the mass averaged velocity, but referencing to the mole averaged velocity is suitable for some liquid flows, and referencing to a single species is suitable for solid phase transport within a lattice. Currently, the identity of the reference velocity is coded into each transport object as a typedef named VelocityBasis, which is equated to an integer. Negative values of this variable refer to mass or mole-averaged velocities. Zero or positive quantities refers to the reference velocity being referenced to a particular species. Below are the predefined constants for its value.
All transport managers specify a default reference velocity in their default constructors. All gas phase transport managers by default specify the mass- averaged velocity as their reference velocities.
Definition at line 145 of file Transport.h.
Public Member Functions | |
Transport (ThermoPhase *thermo=0, size_t ndim=npos) | |
Constructor. | |
Transport (const Transport &)=delete | |
Transport & | operator= (const Transport &)=delete |
virtual string | transportModel () const |
Identifies the model represented by this Transport object. | |
string | transportType () const |
Identifies the Transport object type. | |
ThermoPhase & | thermo () |
Phase object. | |
bool | ready () |
Returns true if the transport manager is ready for use. | |
void | setNDim (const int ndim) |
Set the number of dimensions to be expected in flux expressions. | |
size_t | nDim () const |
Return the number of dimensions in flux expressions. | |
void | checkSpeciesIndex (size_t k) const |
Check that the specified species index is in range. | |
void | checkSpeciesArraySize (size_t kk) const |
Check that an array size is at least nSpecies(). | |
virtual double | getElectricConduct () |
Compute the mixture electrical conductivity (S m-1) at the current conditions of the phase (Siemens m-1) | |
virtual void | getElectricCurrent (int ndim, const double *grad_T, int ldx, const double *grad_X, int ldf, const double *grad_V, double *current) |
Compute the electric current density in A/m^2. | |
virtual void | getSpeciesFluxes (size_t ndim, const double *const grad_T, size_t ldx, const double *const grad_X, size_t ldf, double *const fluxes) |
Get the species diffusive mass fluxes wrt to the specified solution averaged velocity, given the gradients in mole fraction and temperature. | |
virtual void | getSpeciesFluxesES (size_t ndim, const double *grad_T, size_t ldx, const double *grad_X, size_t ldf, const double *grad_Phi, double *fluxes) |
Get the species diffusive mass fluxes wrt to the mass averaged velocity, given the gradients in mole fraction, temperature and electrostatic potential. | |
virtual void | getSpeciesVdiff (size_t ndim, const double *grad_T, int ldx, const double *grad_X, int ldf, double *Vdiff) |
Get the species diffusive velocities wrt to the mass averaged velocity, given the gradients in mole fraction and temperature. | |
virtual void | getSpeciesVdiffES (size_t ndim, const double *grad_T, int ldx, const double *grad_X, int ldf, const double *grad_Phi, double *Vdiff) |
Get the species diffusive velocities wrt to the mass averaged velocity, given the gradients in mole fraction, temperature, and electrostatic potential. | |
virtual void | getMolarFluxes (const double *const state1, const double *const state2, const double delta, double *const cfluxes) |
Get the molar fluxes [kmol/m^2/s], given the thermodynamic state at two nearby points. | |
virtual void | getMassFluxes (const double *state1, const double *state2, double delta, double *mfluxes) |
Get the mass fluxes [kg/m^2/s], given the thermodynamic state at two nearby points. | |
virtual void | getThermalDiffCoeffs (double *const dt) |
Return a vector of Thermal diffusion coefficients [kg/m/sec]. | |
virtual void | getBinaryDiffCoeffs (const size_t ld, double *const d) |
Returns the matrix of binary diffusion coefficients [m^2/s]. | |
virtual void | getMultiDiffCoeffs (const size_t ld, double *const d) |
Return the Multicomponent diffusion coefficients. Units: [m^2/s]. | |
virtual void | getMixDiffCoeffs (double *const d) |
Returns a vector of mixture averaged diffusion coefficients. | |
virtual void | getMixDiffCoeffsMole (double *const d) |
Returns a vector of mixture averaged diffusion coefficients. | |
virtual void | getMixDiffCoeffsMass (double *const d) |
Returns a vector of mixture averaged diffusion coefficients. | |
virtual void | getViscosityPolynomial (size_t i, double *coeffs) const |
Return the polynomial fits to the viscosity of species i. | |
virtual void | getConductivityPolynomial (size_t i, double *coeffs) const |
Return the temperature fits of the heat conductivity of species i. | |
virtual void | getBinDiffusivityPolynomial (size_t i, size_t j, double *coeffs) const |
Return the polynomial fits to the binary diffusivity of species pair (i, j) | |
virtual void | getCollisionIntegralPolynomial (size_t i, size_t j, double *astar_coeffs, double *bstar_coeffs, double *cstar_coeffs) const |
Return the polynomial fits to the collision integral of species pair (i, j) | |
virtual void | setViscosityPolynomial (size_t i, double *coeffs) |
Modify the polynomial fits to the viscosity of species i. | |
virtual void | setConductivityPolynomial (size_t i, double *coeffs) |
Modify the temperature fits of the heat conductivity of species i. | |
virtual void | setBinDiffusivityPolynomial (size_t i, size_t j, double *coeffs) |
Modify the polynomial fits to the binary diffusivity of species pair (i, j) | |
virtual void | setCollisionIntegralPolynomial (size_t i, size_t j, double *astar_coeffs, double *bstar_coeffs, double *cstar_coeffs, bool flag) |
Modify the polynomial fits to the collision integral of species pair (i, j) | |
virtual void | setParameters (const int type, const int k, const double *const p) |
Set model parameters for derived classes. | |
AnyMap | parameters () const |
Return the parameters for a phase definition which are needed to reconstruct an identical object using the newTransport function. | |
void | setVelocityBasis (VelocityBasis ivb) |
Sets the velocity basis. | |
VelocityBasis | getVelocityBasis () const |
Gets the velocity basis. | |
Transport Properties | |
virtual double | viscosity () |
The viscosity in Pa-s. | |
virtual void | getSpeciesViscosities (double *const visc) |
Returns the pure species viscosities. | |
virtual double | bulkViscosity () |
The bulk viscosity in Pa-s. | |
virtual double | ionConductivity () |
The ionic conductivity in 1/ohm/m. | |
virtual void | getSpeciesIonConductivity (double *const ionCond) |
Returns the pure species ionic conductivity. | |
virtual void | mobilityRatio (double *mobRat) |
Returns the pointer to the mobility ratios of the species in the phase. | |
virtual void | getSpeciesMobilityRatio (double **mobRat) |
Returns the pure species limit of the mobility ratios. | |
virtual double | thermalConductivity () |
Returns the mixture thermal conductivity in W/m/K. | |
virtual double | electricalConductivity () |
The electrical conductivity (Siemens/m). | |
virtual void | getMobilities (double *const mobil_e) |
Get the Electrical mobilities (m^2/V/s). | |
virtual void | getFluidMobilities (double *const mobil_f) |
Get the fluid mobilities (s kmol/kg). | |
Protected Attributes | |
ThermoPhase * | m_thermo |
pointer to the object representing the phase | |
bool | m_ready = false |
true if finalize has been called | |
size_t | m_nsp = 0 |
Number of species. | |
size_t | m_nDim |
Number of dimensions used in flux expressions. | |
int | m_velocityBasis = VB_MASSAVG |
Velocity basis from which diffusion velocities are computed. | |
std::weak_ptr< Solution > | m_root |
reference to Solution | |
Transport manager construction | |
These methods are used during construction. | |
virtual void | init (ThermoPhase *thermo, int mode=0, int log_level=0) |
Initialize a transport manager. | |
virtual void | setThermo (ThermoPhase &thermo) |
Specifies the ThermoPhase object. | |
virtual void | setRoot (shared_ptr< Solution > root) |
Set root Solution holding all phase information. | |
virtual bool | CKMode () const |
Boolean indicating the form of the transport properties polynomial fits. | |
void | finalize () |
Enable the transport object for use. | |
Transport | ( | ThermoPhase * | thermo = 0 , |
size_t | ndim = npos |
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Constructor.
New transport managers should be created using TransportFactory, not by calling the constructor directly.
thermo | Pointer to the ThermoPhase class representing this phase. |
ndim | Dimension of the flux vector used in the calculation. |
thermo
and ndim
parameters will be removed after Cantera 3.0. The ThermoPhase object should be specifed when calling the init
method.Definition at line 15 of file Transport.cpp.
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Definition at line 163 of file Transport.h.
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Identifies the model represented by this Transport object.
Each derived class should override this method to return a meaningful identifier.
Reimplemented in DustyGasTransport, HighPressureGasTransport, IonGasTransport, MixTransport, MultiTransport, UnityLewisTransport, and WaterTransport.
Definition at line 173 of file Transport.h.
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Identifies the Transport object type.
Each derived class should override this method to return a meaningful identifier.
Definition at line 180 of file Transport.h.
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Phase object.
Every transport manager is designed to compute properties for a specific phase of a mixture, which might be a liquid solution, a gas mixture, a surface, etc. This method returns a reference to the object representing the phase itself.
Definition at line 192 of file Transport.h.
bool ready | ( | ) |
Returns true if the transport manager is ready for use.
Definition at line 32 of file Transport.cpp.
void setNDim | ( | const int | ndim | ) |
Set the number of dimensions to be expected in flux expressions.
ndim | Number of dimensions in flux expressions |
Definition at line 38 of file Transport.cpp.
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Return the number of dimensions in flux expressions.
Definition at line 211 of file Transport.h.
void checkSpeciesIndex | ( | size_t | k | ) | const |
Check that the specified species index is in range.
Throws an exception if k is greater than nSpecies()
Definition at line 44 of file Transport.cpp.
void checkSpeciesArraySize | ( | size_t | kk | ) | const |
Check that an array size is at least nSpecies().
Throws an exception if kk is less than nSpecies(). Used before calls which take an array pointer.
Definition at line 51 of file Transport.cpp.
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The viscosity in Pa-s.
Reimplemented in GasTransport, HighPressureGasTransport, IonGasTransport, and WaterTransport.
Definition at line 230 of file Transport.h.
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Returns the pure species viscosities.
The units are Pa-s and the length is the number of species
visc | Vector of viscosities |
Reimplemented in GasTransport.
Definition at line 241 of file Transport.h.
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The bulk viscosity in Pa-s.
The bulk viscosity is only non-zero in rare cases. Most transport managers either overload this method to return zero, or do not implement it, in which case an exception is thrown if called.
Reimplemented in WaterTransport.
Definition at line 252 of file Transport.h.
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The ionic conductivity in 1/ohm/m.
Definition at line 259 of file Transport.h.
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Returns the pure species ionic conductivity.
The units are 1/ohm/m and the length is the number of species
ionCond | Vector of ionic conductivities |
Definition at line 272 of file Transport.h.
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Returns the pointer to the mobility ratios of the species in the phase.
mobRat | Returns a matrix of mobility ratios for the current problem. The mobility ratio mobRat(i,j) is defined as the ratio of the mobility of species i to species j. |
mobRat(i,j) = mu_i / mu_j
It is returned in fortran-ordering format. That is, it is returned as mobRat[k], where
k = j * nsp + i
The size of mobRat must be at least equal to nsp*nsp
Definition at line 294 of file Transport.h.
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Returns the pure species limit of the mobility ratios.
The value is dimensionless and the length is the number of species
mobRat | Vector of mobility ratios |
Definition at line 307 of file Transport.h.
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Returns the mixture thermal conductivity in W/m/K.
Units are in W / m K or equivalently kg m / s3 K
Reimplemented in HighPressureGasTransport, IonGasTransport, MixTransport, MultiTransport, and WaterTransport.
Definition at line 318 of file Transport.h.
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The electrical conductivity (Siemens/m).
Reimplemented in IonGasTransport.
Definition at line 324 of file Transport.h.
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Get the Electrical mobilities (m^2/V/s).
This function returns the mobilities. In some formulations this is equal to the normal mobility multiplied by Faraday's constant.
Frequently, but not always, the mobility is calculated from the diffusion coefficient using the Einstein relation
\[ \mu^e_k = \frac{F D_k}{R T} \]
mobil_e | Returns the mobilities of the species in array mobil_e . The array must be dimensioned at least as large as the number of species. |
Reimplemented in IonGasTransport, and MixTransport.
Definition at line 345 of file Transport.h.
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Get the fluid mobilities (s kmol/kg).
This function returns the fluid mobilities. Usually, you have to multiply Faraday's constant into the resulting expression to general a species flux expression.
Frequently, but not always, the mobility is calculated from the diffusion coefficient using the Einstein relation
\[ \mu^f_k = \frac{D_k}{R T} \]
mobil_f | Returns the mobilities of the species in array mobil . The array must be dimensioned at least as large as the number of species. |
Definition at line 369 of file Transport.h.
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Compute the mixture electrical conductivity (S m-1) at the current conditions of the phase (Siemens m-1)
The electrical conductivity, \( \sigma \), relates the electric current density, J, to the electric field, E.
\[ \vec{J} = \sigma \vec{E} \]
We assume here that the mixture electrical conductivity is an isotropic quantity, at this stage. Tensors may be included at a later time.
The conductivity is the reciprocal of the resistivity.
The units are Siemens m-1, where 1 S = 1 A / volt = 1 s^3 A^2 /kg /m^2
Definition at line 395 of file Transport.h.
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Compute the electric current density in A/m^2.
Calculates the electric current density as a vector, given the gradients of the field variables.
ndim | The number of spatial dimensions (1, 2, or 3). |
grad_T | The temperature gradient (ignored in this model). |
ldx | Leading dimension of the grad_X array. |
grad_X | The gradient of the mole fraction |
ldf | Leading dimension of the grad_V and current vectors. |
grad_V | The electrostatic potential gradient. |
current | The electric current in A/m^2. This is a vector of length ndim |
Definition at line 415 of file Transport.h.
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Get the species diffusive mass fluxes wrt to the specified solution averaged velocity, given the gradients in mole fraction and temperature.
Units for the returned fluxes are kg m-2 s-1.
Usually the specified solution average velocity is the mass averaged velocity. This is changed in some subclasses, however.
ndim | Number of dimensions in the flux expressions |
grad_T | Gradient of the temperature (length = ndim) |
ldx | Leading dimension of the grad_X array (usually equal to m_nsp but not always) |
grad_X | Gradients of the mole fraction Flat vector with the m_nsp in the inner loop. length = ldx * ndim |
ldf | Leading dimension of the fluxes array (usually equal to m_nsp but not always) |
fluxes | Output of the diffusive mass fluxes. Flat vector with the m_nsp in the inner loop. length = ldx * ndim |
Reimplemented in MixTransport, and MultiTransport.
Definition at line 445 of file Transport.h.
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Get the species diffusive mass fluxes wrt to the mass averaged velocity, given the gradients in mole fraction, temperature and electrostatic potential.
Units for the returned fluxes are kg m-2 s-1.
[in] | ndim | Number of dimensions in the flux expressions |
[in] | grad_T | Gradient of the temperature. (length = ndim) |
[in] | ldx | Leading dimension of the grad_X array (usually equal to m_nsp but not always) |
[in] | grad_X | Gradients of the mole fraction. Flat vector with the m_nsp in the inner loop. length = ldx * ndim. |
[in] | ldf | Leading dimension of the fluxes array (usually equal to m_nsp but not always). |
[in] | grad_Phi | Gradients of the electrostatic potential (length = ndim) |
[out] | fluxes | The diffusive mass fluxes. Flat vector with the m_nsp in the inner loop. length = ldx * ndim. |
Definition at line 472 of file Transport.h.
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Get the species diffusive velocities wrt to the mass averaged velocity, given the gradients in mole fraction and temperature.
[in] | ndim | Number of dimensions in the flux expressions |
[in] | grad_T | Gradient of the temperature (length = ndim) |
[in] | ldx | Leading dimension of the grad_X array (usually equal to m_nsp but not always) |
[in] | grad_X | Gradients of the mole fraction. Flat vector with the m_nsp in the inner loop. length = ldx * ndim |
[in] | ldf | Leading dimension of the fluxes array (usually equal to m_nsp but not always) |
[out] | Vdiff | Diffusive velocities wrt the mass- averaged velocity. Flat vector with the m_nsp in the inner loop. length = ldx * ndim. units are m / s. |
Definition at line 499 of file Transport.h.
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Get the species diffusive velocities wrt to the mass averaged velocity, given the gradients in mole fraction, temperature, and electrostatic potential.
[in] | ndim | Number of dimensions in the flux expressions |
[in] | grad_T | Gradient of the temperature (length = ndim) |
[in] | ldx | Leading dimension of the grad_X array (usually equal to m_nsp but not always) |
[in] | grad_X | Gradients of the mole fraction. Flat vector with the m_nsp in the inner loop. length = ldx * ndim. |
[in] | ldf | Leading dimension of the fluxes array (usually equal to m_nsp but not always) |
[in] | grad_Phi | Gradients of the electrostatic potential (length = ndim) |
[out] | Vdiff | Diffusive velocities wrt the mass-averaged velocity. Flat vector with the m_nsp in the inner loop. length = ldx
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Definition at line 529 of file Transport.h.
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Get the molar fluxes [kmol/m^2/s], given the thermodynamic state at two nearby points.
[in] | state1 | Array of temperature, density, and mass fractions for state 1. |
[in] | state2 | Array of temperature, density, and mass fractions for state 2. |
[in] | delta | Distance from state 1 to state 2 (m). |
[out] | cfluxes | Output array containing the diffusive molar fluxes of species from state1 to state2. This is a flat vector with m_nsp in the inner loop. length = ldx * ndim. Units are [kmol/m^2/s]. |
Reimplemented in DustyGasTransport, and MultiTransport.
Definition at line 552 of file Transport.h.
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Get the mass fluxes [kg/m^2/s], given the thermodynamic state at two nearby points.
[in] | state1 | Array of temperature, density, and mass fractions for state 1. |
[in] | state2 | Array of temperature, density, and mass fractions for state 2. |
[in] | delta | Distance from state 1 to state 2 (m). |
[out] | mfluxes | Output array containing the diffusive mass fluxes of species from state1 to state2. This is a flat vector with m_nsp in the inner loop. length = ldx * ndim. Units are [kg/m^2/s]. |
Reimplemented in MultiTransport.
Definition at line 572 of file Transport.h.
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Return a vector of Thermal diffusion coefficients [kg/m/sec].
The thermal diffusion coefficient \( D^T_k \) is defined so that the diffusive mass flux of species k induced by the local temperature gradient is given by the following formula:
\[ M_k J_k = -D^T_k \nabla \ln T. \]
The thermal diffusion coefficient can be either positive or negative.
dt | On return, dt will contain the species thermal diffusion coefficients. Dimension dt at least as large as the number of species. Units are kg/m/s. |
Reimplemented in HighPressureGasTransport, MixTransport, and MultiTransport.
Definition at line 595 of file Transport.h.
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Returns the matrix of binary diffusion coefficients [m^2/s].
[in] | ld | Inner stride for writing the two dimension diffusion coefficients into a one dimensional vector |
[out] | d | Diffusion coefficient matrix (must be at least m_k * m_k in length. |
Reimplemented in GasTransport, and HighPressureGasTransport.
Definition at line 607 of file Transport.h.
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Return the Multicomponent diffusion coefficients. Units: [m^2/s].
If the transport manager implements a multicomponent diffusion model, then this method returns the array of multicomponent diffusion coefficients. Otherwise it throws an exception.
[in] | ld | The dimension of the inner loop of d (usually equal to m_nsp) |
[out] | d | flat vector of diffusion coefficients, fortran ordering. d[ld*j+i] is the D_ij diffusion coefficient (the diffusion coefficient for species i due to concentration gradients in species j). Units: m^2/s |
Reimplemented in DustyGasTransport, HighPressureGasTransport, and MultiTransport.
Definition at line 624 of file Transport.h.
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Returns a vector of mixture averaged diffusion coefficients.
Mixture-averaged diffusion coefficients [m^2/s]. If the transport manager implements a mixture-averaged diffusion model, then this method returns the array of mixture-averaged diffusion coefficients. Otherwise it throws an exception.
d | Return vector of mixture averaged diffusion coefficients Units = m2/s. Length = n_sp |
Reimplemented in GasTransport, IonGasTransport, and UnityLewisTransport.
Definition at line 639 of file Transport.h.
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Returns a vector of mixture averaged diffusion coefficients.
Reimplemented in GasTransport, and UnityLewisTransport.
Definition at line 645 of file Transport.h.
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Returns a vector of mixture averaged diffusion coefficients.
Reimplemented in GasTransport, and UnityLewisTransport.
Definition at line 651 of file Transport.h.
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Return the polynomial fits to the viscosity of species i.
Reimplemented in GasTransport.
Definition at line 657 of file Transport.h.
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Return the temperature fits of the heat conductivity of species i.
Reimplemented in GasTransport.
Definition at line 663 of file Transport.h.
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Return the polynomial fits to the binary diffusivity of species pair (i, j)
Reimplemented in GasTransport.
Definition at line 669 of file Transport.h.
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Return the polynomial fits to the collision integral of species pair (i, j)
Reimplemented in GasTransport.
Definition at line 675 of file Transport.h.
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Modify the polynomial fits to the viscosity of species i.
Reimplemented in GasTransport.
Definition at line 684 of file Transport.h.
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Modify the temperature fits of the heat conductivity of species i.
Reimplemented in GasTransport.
Definition at line 690 of file Transport.h.
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Modify the polynomial fits to the binary diffusivity of species pair (i, j)
Reimplemented in GasTransport.
Definition at line 696 of file Transport.h.
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Modify the polynomial fits to the collision integral of species pair (i, j)
Reimplemented in GasTransport.
Definition at line 702 of file Transport.h.
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Set model parameters for derived classes.
This method may be derived in subclasses to set model-specific parameters. The primary use of this class is to set parameters while in the middle of a calculation without actually having to dynamically cast the base Transport pointer.
type | Specifies the type of parameters to set 0 : Diffusion coefficient 1 : Thermal Conductivity The rest are currently unused. |
k | Species index to set the parameters on |
p | Vector of parameters. The length of the vector varies with the parameterization |
Definition at line 726 of file Transport.h.
AnyMap parameters | ( | ) | const |
Return the parameters for a phase definition which are needed to reconstruct an identical object using the newTransport function.
This excludes the individual species transport properties, which are handled separately.
Definition at line 58 of file Transport.cpp.
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Sets the velocity basis.
What the transport object does with this parameter is up to the individual operator. Currently, this is not functional for most transport operators including all of the gas-phase operators.
ivb | Species the velocity basis |
Definition at line 746 of file Transport.h.
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Gets the velocity basis.
What the transport object does with this parameter is up to the individual operator. Currently, this is not functional for most transport operators including all of the gas-phase operators.
Definition at line 759 of file Transport.h.
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Initialize a transport manager.
This routine sets up a transport manager. It calculates the collision integrals and populates species-dependent data structures.
thermo | Pointer to the ThermoPhase object |
mode | Chemkin compatible mode or not. This alters the specification of the collision integrals. defaults to no. |
log_level | Defaults to zero, no logging |
Reimplemented in IonGasTransport, GasTransport, MixTransport, MultiTransport, and WaterTransport.
Definition at line 778 of file Transport.h.
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Specifies the ThermoPhase object.
We have relaxed this operation so that it will succeed when the underlying old and new ThermoPhase objects have the same number of species and the same names of the species in the same order. The idea here is to allow copy constructors and duplicators to work. In order for them to work, we need a method to switch the internal pointer within the Transport object after the duplication takes place. Also, different thermodynamic instantiations of the same species should also work.
thermo | Reference to the ThermoPhase object that the transport object will use |
init
. Reimplemented in DustyGasTransport.
Definition at line 68 of file Transport.cpp.
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Set root Solution holding all phase information.
Definition at line 95 of file Transport.cpp.
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Boolean indicating the form of the transport properties polynomial fits.
Returns true if the Chemkin form is used.
Reimplemented in GasTransport.
Definition at line 803 of file Transport.h.
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Enable the transport object for use.
Once finalize() has been called, the transport manager should be ready to compute any supported transport property, and no further modifications to the model parameters should be made.
Definition at line 101 of file Transport.cpp.
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pointer to the object representing the phase
Definition at line 821 of file Transport.h.
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true if finalize has been called
Definition at line 825 of file Transport.h.
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Number of species.
Definition at line 828 of file Transport.h.
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Number of dimensions used in flux expressions.
Definition at line 832 of file Transport.h.
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Velocity basis from which diffusion velocities are computed.
Defaults to the mass averaged basis = -2
Definition at line 837 of file Transport.h.
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reference to Solution
Definition at line 841 of file Transport.h.