Abstract
Let σ be a stationary surface of discontinuity and n be a unit normal of σ (Figure 3.1). We take a rectangular volume Ω for which σ cuts across Ω as shown in the figure. Let S + denote the surface of Ω which lies in the positive side of σ, S − that lies in the negative side, and S l denote the lateral surfaces of Ω.
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Hui, WH., Xu, K. (2012). Review of Eulerian Computation for 1-D Inviscid Flow. In: Computational Fluid Dynamics Based on the Unified Coordinates. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-25896-1_3
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