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・ Shockley Semiconductor Laboratory
・ Shockley Shoemake
・ Shockley–Queisser limit
・ Shockley–Ramo theorem
・ Shockmain Davis
・ Shockman
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Shocks and discontinuities (magnetohydrodynamics)
・ Shocks Mills Bridge
・ Shocks the conscience
・ Shockscape
・ Shocksteady
・ Shocktoberfest
・ Shocktrauma
・ Shockwave (2000 yacht)
・ Shockwave (Canada's Wonderland)
・ Shockwave (comics)
・ Shockwave (disambiguation)
・ Shockwave (Drayton Manor)
・ Shockwave (Dreamworld)
・ Shockwave (G.I. Joe)
・ Shockwave (game portal)


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Shocks and discontinuities (magnetohydrodynamics) : ウィキペディア英語版
Shocks and discontinuities (magnetohydrodynamics)
Shocks and discontinuities are transition layers where the plasma properties change from one equilibrium state to another. The relation between the plasma properties on both sides of a shock or a discontinuity can be obtained from the conservative form of the magnetohydrodynamic (MHD) equations, assuming conservation of mass, momentum, energy and of \nabla \cdot \mathbf .
==Rankine-Hugoniot jump conditions for MHD==
The jump conditions across a time-independent MHD shock or discontinuity are referred as the Rankine-Hugoniot equations for MHD. In the frame moving with the shock/discontinuity, those jump conditions can be written:
: \rho_1 v_ = \rho_2 v_,
: B_ = B_,
: \rho_1 v_^2+ p_1 + \frac=\rho_2 v_^2+ p_2 + \frac,
: \rho_1 v_ \mathbf}B_}= \rho_2 v_ \mathbf}B_},
: \left(\frac\frac+\frac\right)\rho_1 v_+\frac^2}-\frac}\cdot \mathbf=\left(\frac\frac+\frac\right)\rho_2 v_+\frac^2}-\frac}\cdot \mathbf,
: (\mathbf \times \mathbf)_ = (\mathbf \times \mathbf)_,
where \rho, v, p, B are the plasma density, velocity, (thermal) pressure and magnetic field respectively. The subscripts t and n refer to the tangential and normal components of a vector (with respect to the shock/discontinuity front). The subscripts 1 and 2 refer to the two states of the plasma on each side of the shock/discontinuity

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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