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- W1992913018 abstract "p(0) =p’(O) = 0, and p’ > 0,p” > 0 in P > 0. (4 For example, one can take p(p) = py, y > 1. By definition, a vacuum state is any portion of the x t plane in which p = 0. In Section 2 we show that a vacuum state must be bounded by rarefaction waves. We then study the ways in which it is possible to go from a nonvacuum to a vacuum state (see [IS]). There are, in fact two distinct types of vacuums which we call compression and rarefaction vacuums; the compression vacuums differ from the rarefaction vacuums in that they give rise to compression waves which eventually form shock" @default.
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- W1992913018 date "1980-12-01" @default.
- W1992913018 modified "2023-09-29" @default.
- W1992913018 title "On the vacuum state for the isentropic gas dynamics equations" @default.
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- W1992913018 doi "https://doi.org/10.1016/0196-8858(80)90016-0" @default.
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