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Test 3: Ryu & Jones 3b shock tube problem at t = 0.1. We show the numerical solution for ρ, vx and magnetic field By (points) compared with the exact solution (line). 

Test 3: Ryu & Jones 3b shock tube problem at t = 0.1. We show the numerical solution for ρ, vx and magnetic field By (points) compared with the exact solution (line). 

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Article
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We present a new code designed to solve the equations of classical ideal magnetohydrodynamics (MHD) in three dimensions, submitted to a constant gravitational field. The purpose of the code centres on the analysis of solar phenomena within the photosphere–corona region. We present 1D and 2D standard tests to demonstrate the quality of the numerical...

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... is a test containing magnetosonic rarefactions waves. The numerical solution shows only two strong and identical magnetosonic rarefractions. Our code was able to capture this structure and the results are shown in Fig. 3. ...
Context 2
... is greater than the magnetic pres- sure, which implies that β > 1. This excites fast and slow magnetoacoustic-gravity waves which are coupled. The ini- tial pulse splits into two propagating waves at time t = 37.5 s shown in Fig. 11 (top). At time t = 100 s, the two mag- netocoustic waves move upwards until z ≈ 1.4 Mm, in the same way as in Fig. 3 of ( Murawski et al. 2013). The waves continue moving until they reach the transition re- gion. This vertical perturbation produces the propagation of magnetoacoustic-gravity waves in a symmetric way, as shown in Fig. 11 at the xz and yz planes. In these two planes the propagation is seen in the same way. We also show the propagation ...

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