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Global existence for one-dimensional motion of non-isentropic viscous fluids

✍ Scribed by Shigenori Yanagi


Publisher
John Wiley and Sons
Year
1993
Tongue
English
Weight
470 KB
Volume
16
Category
Article
ISSN
0170-4214

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✦ Synopsis


Abstract

We study the p‐system with viscosity given by v~t~ βˆ’ u~x~ = 0, u~t~ + p(v)~x~ = (k(v)u~x~)~x~ + f(∫ v__d__x, t), with the initial and the boundary conditions (v(x, 0), u(x,0)) = (v~0~, u~0~(x)), u(0,t) = u(X,t) = 0. To describe the motion of the fluid more realistically, many equations of state, namely the function p(v) have been proposed. In this paper, we adopt Planck's equation, which is defined only for v > b(> 0) and not a monotonic function of v, and prove the global existence of the smooth solution. The essential point of the proof is to obtain the bound of v of the form b < h(T) β©½ v(x, t) β©½ H(T) < ∞ for some constants h(T) and H(T).


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