| WARPXM v1.10.0
    | 
| Classes | |
| class | CustomMaxwell | 
| class | DivergenceError | 
| Divergence Error Calculation This calculates the divergence error for diagnostic purposes THIS IS NOT MEANT TO BE AN INITIAL CONDITION PsiE = 1/(omega_p tau)^2 * (L / dp) * Div(E) - rho_c PsiB = Div(B)  More... | |
| class | EinICEM | 
| Class to set IC on EM fields in 5-moment problem.  More... | |
| class | FieldZpinch1d | 
| class | FieldZpinch1dCar | 
| class | FieldZpinch2d | 
| class | FieldZpinchTest1d | 
| class | FlowInitEM | 
| Class to set IC for electromagnetic fields in a simple flow problem.  More... | |
| class | GEM | 
| class | GEM1D | 
| class | HarrisCurrentSheet | 
| class | HartmannField | 
| class | KH_Instability | 
| Initialization and boundary conditions for electromagnetic Rayleigh-Taylor and Kelvin-Helmholtz instability defined using piecewise discontinuous values.  More... | |
| class | KH_Instability_Analytic | 
| Initialization and boundary conditions for electromagnetic Rayleigh-Taylor and Kelvin-Helmholtz instability defined using analytic functions described in Vogman PoP 2020 Eq.  More... | |
| class | KHInstability2d2vKineticSetup | 
| 2D2V Kelvin-Helmholtz Instability for Fields Based on calculated kinetic equilibrium Should be consistent with 2d2v_kh_instability.h/cc in function_evaluators/kinetics  More... | |
| class | Kinetics1d1vLandauDampingField | 
| 1D1V Landau Damping Initial Condition for the Fields This is an Ex (1D Electric) Field consistent with a Maxwellian distribution with sinusoidally-varying spatial variation with a uniformly-distributed opposite chage: E_x(x) = +Z_i n_0 (omega_p tau)^2 (delta_p/L) (alpha/k) sin(kx) See the paper: Physics-Based-Adaptive Plasma Model for High-Fidelity Numerical Simulations https://www.frontiersin.org/articles/10.3389/fphy.2018.00105/full Equation 121  More... | |
| class | Kinetics2d2vLandauDampingField | 
| 2D2V Landau Damping Initial Condition for the Fields This is an (Ex, Ey) (2D Electric) Field consistent with a Maxwellian distribution with sinusoidally-varying spatial variation with a uniformly-distributed opposite charge: E_x(x) = +Z_i n_0 (omega_p tau)^2 (delta_p/L) (alpha_x/k_x) sin(k_x * x) E_y(y) = +Z_i n_0 (omega_p tau)^2 (delta_p/L) (alpha_y/k_y) sin(k_y * y)  More... | |
| class | LangmuirDispersionField | 
| class | PlasmaSwitchFields | 
| Initialize the EM fields for the simplified 2D plasma switch problem with a normalized Poynting vector [1,0,0].  More... | |
| class | RTI_Instability | 
| Field setup for combination of hydrodynamic Rayleigh-Taylor and Kelvin-Helmholtz instabilities??  More... | |
| class | SincField | 
| class | SincField2d | 
| class | SineField | 
| class | UniformMaxwell | 
| Input uniform field values.  More... | |