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Global weak solutions to the 1D compressible Euler equations with radiation

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Figure 1: Representation of a part of the Riemann solution. Note that due to CFL condition (42), lines x = σ ± i t never intersect the vertical boundary of the cell [−∆x, ∆x] × [0, ∆t].
Figure 2: The mesh points defined by (68).
Figure 3: Given a point in a mesh curve, the next one should be one of its two nearest right neighbors Definition 2
Figure 4: The diamond region D ℓ,n .

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