英文摘要 |
Numerical simulation of the plasma propulsion is essential to the Pulsed Plasma Thruster (PPT) fundamental research. By way of coupling the effects among the electric field, magnetic field and flow field in the PPT, a one-dimensional time-dependent model based magnetohydrodynamic (MHD) for PPT has been developed and solved numerically. The system of idealized MHD equations is a conservation system of hydrodynamics and Maxwell's equations with Lorentz force as the driving force of the plasma flow. The shock-tube problem has been used to test numerical stabilities of employed numerical methods. In this research the Riemann problem for a quasilinear hyperbolic system of equations governing the one-dimensional unsteady flow of an inviscid and perfectly conducting compressible fluid, subjected to a transverse magnetic field, is solved numerically. Three different numerical schemes have been employed in this study. The Lax-Wendroff and MacCormack were originally employed for the space discretization of the system of nonlinear equations. Unfortunately, the results showed oscillations at discontinuities even with addition of artificial viscosities for these two methods. For numerical simulations to be effective, a high-order accurate solver that captures MHD shocks monotonically and works reliably for strong magnetic fields is needed. A characteristics-based scheme of Roe's Riemann solver for the MHD equations, with flux limiters to improve spatial accuracy has been developed successfully. The unsteady terms are discretized using fourth order Runge-Kutta integration. The results are compared with other references for validation and show a good agreement with the existed literature. Rarefaction fan, contact discontinuity and a moving shock have been resolved clearly. It has been observed that in contrast to the gasdynamic case, the pressure varies across the contact discontinuity. A full pressure has been introduced to remove the spike caused by the influence of the magnetic field and is continuous across the contact discontinuity. |