eBook ISBN: | 978-1-4704-0399-7 |
Product Code: | MEMO/169/801.E |
List Price: | $71.00 |
MAA Member Price: | $63.90 |
AMS Member Price: | $42.60 |
eBook ISBN: | 978-1-4704-0399-7 |
Product Code: | MEMO/169/801.E |
List Price: | $71.00 |
MAA Member Price: | $63.90 |
AMS Member Price: | $42.60 |
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Book DetailsMemoirs of the American Mathematical SocietyVolume: 169; 2004; 170 ppMSC: Primary 35
We consider the Cauchy problem for a strictly hyperbolic \(2\times 2\) system of conservation laws in one space dimension \( u_t+[F(u)]_x=0, u(0,x)=\bar u(x),\) which is neither linearly degenerate nor genuinely non-linear. We make the following assumption on the characteristic fields. If \(r_i(u), \ i=1,2,\) denotes the \(i\)-th right eigenvector of \(DF(u)\) and \(\lambda_i(u)\) the corresponding eigenvalue, then the set \(\{u : \nabla \lambda_i \cdot r_i (u) = 0\}\) is a smooth curve in the \(u\)-plane that is transversal to the vector field \(r_i(u)\).
Systems of conservation laws that fulfill such assumptions arise in studying elastodynamics or rigid heat conductors at low temperature.
For such systems we prove the existence of a closed domain \(\mathcal{D} \subset L^1,\) containing all functions with sufficiently small total variation, and of a uniformly Lipschitz continuous semigroup \(S:\mathcal{D} \times [0,+\infty)\rightarrow \mathcal{D}\) with the following properties. Each trajectory \(t \mapsto S_t \bar u\) of \(S\) is a weak solution of (1). Vice versa, if a piecewise Lipschitz, entropic solution \(u= u(t,x)\) of (1) exists for \(t \in [0,T],\) then it coincides with the trajectory of \(S\), i.e. \(u(t,\cdot) = S_t \bar u.\)
This result yields the uniqueness and continuous dependence of weak, entropy-admissible solutions of the Cauchy problem (1) with small initial data, for systems satisfying the above assumption.
ReadershipGraduate students and research mathematicians interested in partial differential equations.
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Table of Contents
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Chapters
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1. Introduction
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2. Preliminaries
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3. Outline of the proof
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4. The algorithm
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5. Basic interaction estimates
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6. Bounds on the total variation and on the interaction potential
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7. Estimates on the number of discontinuities
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8. Estimates on shift differentials
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9. Completion of the proof
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10. Conclusion
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We consider the Cauchy problem for a strictly hyperbolic \(2\times 2\) system of conservation laws in one space dimension \( u_t+[F(u)]_x=0, u(0,x)=\bar u(x),\) which is neither linearly degenerate nor genuinely non-linear. We make the following assumption on the characteristic fields. If \(r_i(u), \ i=1,2,\) denotes the \(i\)-th right eigenvector of \(DF(u)\) and \(\lambda_i(u)\) the corresponding eigenvalue, then the set \(\{u : \nabla \lambda_i \cdot r_i (u) = 0\}\) is a smooth curve in the \(u\)-plane that is transversal to the vector field \(r_i(u)\).
Systems of conservation laws that fulfill such assumptions arise in studying elastodynamics or rigid heat conductors at low temperature.
For such systems we prove the existence of a closed domain \(\mathcal{D} \subset L^1,\) containing all functions with sufficiently small total variation, and of a uniformly Lipschitz continuous semigroup \(S:\mathcal{D} \times [0,+\infty)\rightarrow \mathcal{D}\) with the following properties. Each trajectory \(t \mapsto S_t \bar u\) of \(S\) is a weak solution of (1). Vice versa, if a piecewise Lipschitz, entropic solution \(u= u(t,x)\) of (1) exists for \(t \in [0,T],\) then it coincides with the trajectory of \(S\), i.e. \(u(t,\cdot) = S_t \bar u.\)
This result yields the uniqueness and continuous dependence of weak, entropy-admissible solutions of the Cauchy problem (1) with small initial data, for systems satisfying the above assumption.
Graduate students and research mathematicians interested in partial differential equations.
-
Chapters
-
1. Introduction
-
2. Preliminaries
-
3. Outline of the proof
-
4. The algorithm
-
5. Basic interaction estimates
-
6. Bounds on the total variation and on the interaction potential
-
7. Estimates on the number of discontinuities
-
8. Estimates on shift differentials
-
9. Completion of the proof
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10. Conclusion