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rizer.cantera_ext
C++ Cantera 1-D plasma extension (custom Domain1D models and solvers)
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| constexpr double | e = 1.602'176'634e-19 |
| Elementary charge [C]. Exact (CODATA). | |
| constexpr double | k_b = 1.380'649e-23 |
| Boltzmann constant [J/K]. Exact (CODATA). | |
| constexpr double | N_a = 6.022'140'76e23 |
| Avogadro's number [1/mol]. Exact (CODATA). | |
| constexpr double | c = 299'792'458.0 |
| Speed of light [m/s]. Exact (CODATA). | |
| constexpr double | h = 6.626'070'15e-34 |
| Planck constant [J s]. Exact (CODATA). | |
| constexpr double | m_e = 9.109'383'713'9e-31 |
| Electron mass [kg] (CODATA 2022). | |
| constexpr double | M_e = m_e * N_a |
| Electron molar mass [kg/mol]. | |
| constexpr double | Da = 1.660'539'068'92e-27 |
| Dalton / atomic mass constant [kg] (CODATA 2022). | |
| constexpr double | epsilon_0 = 8.854'187'818'8e-12 |
| Vacuum permittivity [F/m] (CODATA 2022). | |
| constexpr double | stefan_boltzmann = 5.670'374'419e-8 |
| Stefan-Boltzmann constant [W/(m^2 K^4)] (CODATA). | |
| constexpr double | bohr_radius_m = 5.291'772'105'44e-11 |
| Bohr radius [m] (CODATA). | |
| constexpr double | rydberg_energy_eV = 13.605'693'122'990 |
| Rydberg energy [eV] (CODATA). | |
| constexpr double | pi = 3.141'592'653'589'793'238'46 |
| pi (matches numpy's np.pi used in units.py). | |
| constexpr double | hbar = h / (2.0 * pi) |
| Reduced Planck constant [J s]. | |
| constexpr double | R = k_b * N_a |
| Ideal gas constant [J/(mol K)]. | |
| constexpr double | R_kmol = R * 1e3 |
| Ideal gas constant [J/(kmol K)] (matches Cantera's GasConstant). | |
| constexpr double | m_N2 = 28.013'4 * Da |
| N2 mass [kg]. | |
| constexpr double | P_1_bar = 1e5 |
| 1 bar [Pa]. | |
| constexpr double | eV_to_K = e / k_b |
| eV -> K. | |
| constexpr double | K_to_eV = k_b / e |
| K -> eV. | |
| constexpr double | eV_to_J = e |
| eV -> J. | |
| constexpr double | J_to_eV = 1.0 / e |
| J -> eV. | |
| constexpr double | K_to_J = k_b |
| K -> J. | |
| constexpr double | J_to_K = 1.0 / k_b |
| J -> K. | |
| constexpr double | kJ_per_mol_to_J_per_particle = 1e3 / N_a |
| kJ/mol -> J/particle. | |
| constexpr double | invcm_to_joule = h * c * 100.0 |
| inverse cm -> J. | |
| const double | spitzer_constant |
| Spitzer conductivity constant [Ohm^-1 m^-1 K^-3/2]: | |
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Spitzer conductivity constant [Ohm^-1 m^-1 K^-3/2]:
\[ \sigma = \text{spitzer\_constant} \cdot T_e^{3/2} / \ln\Lambda. \]
Same expression as units.py (cannot be constexpr: uses pow/sqrt).