期刊
NONLINEARITY
卷 35, 期 2, 页码 954-997出版社
IOP Publishing Ltd
DOI: 10.1088/1361-6544/ac4151
关键词
shock formation; shock curve; entropy condition; Rankine-Hugoniot condition; hyperbolic conservation law
资金
- NSFC [11571177, 11731007, 12001162]
The paper investigates the shock formation and regularities of shock curves for hyperbolic conservation laws. It shows that under certain conditions, a weak entropy solution and shock curve can be locally constructed. When these conditions are violated, the study focuses on the optimal regularities of the shock curve and behavior of the solution near the blowup point.
The study on the shock formation and the regularities of the resulting shock surfaces for hyperbolic conservation laws is a basic problem in the nonlinear partial differential equations. In this paper, we are concerned with the shock formation and the optimal regularities of the resulting shock curves for the 1D conservation law partial derivative(t)u +partial derivative(x)f (u) = 0 with the smooth initial data u(0, x) = u(0)(x). If u(0)(x) is an element of C-1(R) and f (u) is an element of C-2(R), it is well-known that the solution u will blow up on the time T* = - 1/min g'(x) when min g'(x) < 0 holds for g(x) = f'(u(0)(x)). Let x(0) be a local minimum point of g'(x) such that g'(x(0)) = min g'(x) < 0 and g ''(x(0)) = 0, g((3))(x(0)) > 0 (which is called the generic nondegenerate condition), then by theorem 2 of Lebaud (1994 J. Math. Pures Appl. 9 523-565), a weak entropy solution u together with the shock curve x = phi(t)is an element of C-2[T-*, T-* + epsilon) starting from the blowup point (T-*, x(*) = x(0) + g(x(0))T-*) can be locally constructed. When the generic nondegenerate condition is violated, namely, when x(0) is a local minimum point of g'(x) such that g ''(x(0)) = g((3))(x(0)) =... = g((2k0))(x(0)) = 0 but g((2k0+1))(x(0)) > 0 for some k(0) is an element of N with k(0) >= 2; or g((k))(x(0)) = 0 for any k is an element of N and k >= 2, we will study the shock formation and the optimal regularity of the shock curve x =phi(t), meanwhile, some precise descriptions on the behaviors of u near the blowup point (T-*, x(*)) are given. Our main aims are to show that: around the blowup point, the shock really appears whether the initial data are degenerate with finite orders or with infinite orders; the optimal regularities of the shock solution and the resulting shock curve have the explicit relations with the degenerate degrees of the initial data.
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