Functions
double	R ()
	Universal gas constant, $R_{} = 8.314462176 \quad \left[ \frac{\text{J}}{\text{mol K}} \right]$ . More...

double	F ()
	Faraday constant, $F_{} = 9.648533992 \cdot 10^4 \quad \left[ \frac{\text{C}}{\text{mol}} \right]$ . More...

double	Pi ()
	$\pi_{} = 3.141592654$ . More...

double	E0 ()
	Permittivity of free space, $\epsilon_0^{} = 8.854187818 \cdot 10^{-12} \quad \left[ \frac{\text{F}}{\text{m}} \right]$ . More...

double	K ()
	Boltzmann constant, $k_{} = 8.617332478 \cdot 10^{-5} \quad \left[ \frac{\text{eV}}{\text{K}} \right]$ . More...

double	K_SI ()
	Boltzmann constant in SI units, $k_{} = 1.3806488 \cdot 10^{-23} \quad \left[ \frac{\text{J}}{\text{K}} \right]$ . More...

double	N_A ()
	Avogadro's constant, $N_A = 6.022140857 \cdot 10^{23} \quad \left[ \frac{\text{molecules}}{\text{mol}} \right]$ . More...

const dealii::Tensor< 1, dim >	gravity_acceleration ()
	Gravitational acceleration, $\mathbf{g} = \{ g_{\alpha} \}_{\alpha = 1}^d \quad \text{such that} \quad \forall \alpha \neq d : \quad g_{\alpha} = 0 \quad \left[ \frac{\text{m}}{\text{sec}^2} \right] \quad \text{and} \quad g_d = -9.81 \quad \left[ \frac{\text{m}}{\text{sec}^2} \right]$ . More...

const dealii::SymmetricTensor < 2, dim >	unit_tensor ()
	Unit tensor, $\hat{ \mathbf{I} } = \{ \delta_{\alpha \beta} \}_{\alpha,\beta = 1}^d$ . More...

double	A_vk ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity). More...

double	B_vk ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity). More...

double	C_vk ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity). More...

double	D_vk ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity). More...

double	E_vk ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity). More...

double	F_vk ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity). More...

double	A_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	B_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	C_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	D_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	E_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	F_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	G_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	H_diff ()
	Coefficient of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity). More...

double	b_0 ()
	Coefficient of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula. More...

double	b_1 ()
	Coefficient $b_1 = 2.9530 \cdot 10^{-2}$ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula. More...

double	b_2 ()
	Coefficient $b_2 = -9.1837 \cdot 10^{-5}$ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula. More...

double	b_3 ()
	Coefficient $b_3 = 1.4454 \cdot 10^{-7}$ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula. More...

double	A11_visc_R1 ()
	Coefficient $A_{} = 1.340794$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	B11_visc_R1 ()
	Coefficient $B_{} = 0.326244;$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	C11_visc_R1 ()
	Coefficient $C_{} = 1.546648$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	D11_visc_R1 ()
	Coefficient $D_{} = 2.768179$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	A11_visc_R2 ()
	Coefficient $A_{} = 1.066993$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	B11_visc_R2 ()
	Coefficient $B_{} = 0.157384;$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	C11_visc_R2 ()
	Coefficient $C_{} = 0.424013$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	D11_visc_R2 ()
	Coefficient $D_{} = 0.698873$ for the $\Omega^{(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	A22_visc_R1 ()
	Coefficient $A_{} = 26.425725$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	B22_visc_R1 ()
	Coefficient $B_{} = 0.045563;$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	C22_visc_R1 ()
	Coefficient $C_{} = -25.232304$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	D22_visc_R1 ()
	Coefficient $D_{} = 0.016075$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^ < 2.5$ . More...

double	A22_visc_R2 ()
	Coefficient $A_{} = 1.151508$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	B22_visc_R2 ()
	Coefficient $B_{} = 0.145812;$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	C22_visc_R2 ()
	Coefficient $C_{} = 0.437374$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

double	D22_visc_R2 ()
	Coefficient $D_{} = 0.670219$ for the $\Omega^{(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^ < 400$ . More...

Function Documentation

double Constants::A11_visc_R1 ( )

inline

Coefficient $A_{} = 1.340794$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::A11_visc_R2 ( )

inline

Coefficient $A_{} = 1.066993$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::A22_visc_R1 ( )

inline

Coefficient $A_{} = 26.425725$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::A22_visc_R2 ( )

inline

Coefficient $A_{} = 1.151508$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::A_diff ( )

inline

Coefficient $ A = 1.06036 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::A_vk ( )

inline

Coefficient $ A = 1.16145 $ of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::B11_visc_R1 ( )

inline

Coefficient $B_{} = 0.326244;$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::B11_visc_R2 ( )

inline

Coefficient $B_{} = 0.157384;$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::B22_visc_R1 ( )

inline

Coefficient $B_{} = 0.045563;$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::B22_visc_R2 ( )

inline

Coefficient $B_{} = 0.145812;$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::b_0 ( )

inline

Coefficient $ b_0 = -2.1794 $ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula.

double Constants::b_1 ( )

inline

Coefficient $b_1 = 2.9530 \cdot 10^{-2}$ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula.

double Constants::b_2 ( )

inline

Coefficient $b_2 = -9.1837 \cdot 10^{-5}$ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula.

double Constants::b_3 ( )

inline

Coefficient $b_3 = 1.4454 \cdot 10^{-7}$ of the Springer-Zawodzinski-Gottesfeld water vapor saturation pressure formula.

double Constants::B_diff ( )

inline

Coefficient $ B = 0.15610 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::B_vk ( )

inline

Coefficient $ B = 0.14874 $ of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::C11_visc_R1 ( )

inline

Coefficient $C_{} = 1.546648$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::C11_visc_R2 ( )

inline

Coefficient $C_{} = 0.424013$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::C22_visc_R1 ( )

inline

Coefficient $C_{} = -25.232304$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::C22_visc_R2 ( )

inline

Coefficient $C_{} = 0.437374$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::C_diff ( )

inline

Coefficient $ C = 0.19300 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::C_vk ( )

inline

Coefficient $ C = 0.52487 $ of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::D11_visc_R1 ( )

inline

Coefficient $D_{} = 2.768179$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::D11_visc_R2 ( )

inline

Coefficient $D_{} = 0.698873$ for the $\Omega^{*(1,1)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::D22_visc_R1 ( )

inline

Coefficient $D_{} = 0.016075$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $0.3 \leq T^* < 2.5$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::D22_visc_R2 ( )

inline

Coefficient $D_{} = 0.670219$ for the $\Omega^{*(2,2)}_{}$ integrals formula (viscosity) between $2.5 \leq T^* < 400$ .

Kerkhof, Piet JAM, and Marcel AM Geboers. "Toward a unified theory of isotropic molecular transport phenomena." AIChE journal 51.1 (2005): 79-121.
Hirschfelder, Joseph O., et al. Molecular theory of gases and liquids. New York: Wiley, 1964.

double Constants::D_diff ( )

inline

Coefficient $ D = 0.47635 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::D_vk ( )

inline

Coefficient $ D = 0.77320 $ of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::E0 ( )

inline

Permittivity of free space, $\epsilon_0^{} = 8.854187818 \cdot 10^{-12} \quad \left[ \frac{\text{F}}{\text{m}} \right]$ .

Referenced by FuelCellShop::MicroScale::AgglomerateBase::AgglomerateBase().

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double Constants::E_diff ( )

inline

Coefficient $ E = 1.03587 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::E_vk ( )

inline

Coefficient $ E = 2.16178 $ of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::F ( )

inline

Faraday constant, $F_{} = 9.648533992 \cdot 10^4 \quad \left[ \frac{\text{C}}{\text{mol}} \right]$ .

Referenced by FuelCellShop::MicroScale::AgglomerateBase::AgglomerateBase(), FuelCellShop::Kinetics::BaseKinetics::BaseKinetics(), and FuelCellShop::Equation::ReactionHeat::initialize_factors().

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double Constants::F_diff ( )

inline

Coefficient $ F = 1.52996 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::F_vk ( )

inline

Coefficient $ F = 2.43787 $ of the Neufeld-Jansen-Aziz collision integrals formula (viscosity and thermal conductivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::G_diff ( )

inline

Coefficient $ G = 1.76474 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

const dealii::Tensor<1,dim> Constants::gravity_acceleration ( )

inline

Gravitational acceleration, $\mathbf{g} = \{ g_{\alpha} \}_{\alpha = 1}^d \quad \text{such that} \quad \forall \alpha \neq d : \quad g_{\alpha} = 0 \quad \left[ \frac{\text{m}}{\text{sec}^2} \right] \quad \text{and} \quad g_d = -9.81 \quad \left[ \frac{\text{m}}{\text{sec}^2} \right]$ .

References dim.

double Constants::H_diff ( )

inline

Coefficient $ H = 3.89411 $ of the Neufeld-Jansen-Aziz collision integrals formula (diffusivity).

Neufeld, Philip D., A. R. Janzen, and R. A. Aziz. "Empirical Equations to Calculate 16 of the Transport Collision Integrals Ω (l, s)* for the Lennard‐Jones (12–6) Potential." The Journal of Chemical Physics 57.3 (1972): 1100-1102.

double Constants::K ( )

inline

Boltzmann constant, $k_{} = 8.617332478 \cdot 10^{-5} \quad \left[ \frac{\text{eV}}{\text{K}} \right]$ .

Referenced by FuelCellShop::Kinetics::BaseKinetics::BaseKinetics().

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double Constants::K_SI ( )

inline

Boltzmann constant in SI units, $k_{} = 1.3806488 \cdot 10^{-23} \quad \left[ \frac{\text{J}}{\text{K}} \right]$ .

double Constants::N_A ( )

inline

Avogadro's constant, $N_A = 6.022140857 \cdot 10^{23} \quad \left[ \frac{\text{molecules}}{\text{mol}} \right]$ .

double Constants::Pi ( )

inline

$\pi_{} = 3.141592654$ .

Referenced by FuelCellShop::MicroScale::SphericalAgglomerateGeometry::SphericalAgglomerateGeometry().

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double Constants::R ( )

inline

Universal gas constant, $R_{} = 8.314462176 \quad \left[ \frac{\text{J}}{\text{mol K}} \right]$ .

Referenced by FuelCellShop::MicroScale::AgglomerateBase::AgglomerateBase(), FuelCellShop::Kinetics::BaseKinetics::BaseKinetics(), FuelCell::OperatingConditions::get_anode_gas_density(), FuelCell::OperatingConditions::get_cathode_gas_density(), and FuelCellShop::Equation::LiquidSourceEquation< dim >::get_temp_related_parameters().

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const dealii::SymmetricTensor<2,dim> Constants::unit_tensor ( )

inline

Unit tensor, $\hat{ \mathbf{I} } = \{ \delta_{\alpha \beta} \}_{\alpha,\beta = 1}^d$ .

References dim.

Functions

Function Documentation