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Impulsive acceleration of strongly magnetized relativistic flows

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Figure

Figure 1. The self-similar rarefaction wave solution atare the magnetic field t = 1, using units ofl0 = 1, ρ0 = 1 and c = 1
Figure 2. Propagation of a highly magnetized cold shell of plasma. Theof total energy (solid line), magnetic energy (dashed line) and kinetic energy(dot–dashed line) as measured in the wall frame (bottom right-hand panel).The front of secondary rarefaction
Figure 3.⟨�⟩∗) and σ (region (thick lines), as well as their values at the head of the secondaryrarefaction wave (indicating a slower convergence in the limit(weighted by energy – equation B1) ofdashed and solid lines, respectively
Figure 4. Numerical and self-similar solutions for shell’s ‘tail’. The left-
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