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Well-Posedness for General $2\times 2$ Systems of Conservation Laws
 
Fabio Ancona University of Bologna, Bologna, Italy
Andrea Marson University of Padova, Padova, Italy
Well-Posedness for General 2X2 Systems of Conservation Laws
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
Well-Posedness for General 2X2 Systems of Conservation Laws
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Well-Posedness for General $2\times 2$ Systems of Conservation Laws
Fabio Ancona University of Bologna, Bologna, Italy
Andrea Marson University of Padova, Padova, Italy
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
  • Book Details
     
     
    Memoirs of the American Mathematical Society
    Volume: 1692004; 170 pp
    MSC: 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.

    Readership

    Graduate students and research mathematicians interested in partial differential equations.

  • Table of Contents
     
     
    • 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
    • 10. Conclusion
  • Requests
     
     
    Review Copy – for publishers of book reviews
    Permission – for use of book, eBook, or Journal content
    Accessibility – to request an alternate format of an AMS title
Volume: 1692004; 170 pp
MSC: 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.

Readership

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
  • 10. Conclusion
Review Copy – for publishers of book reviews
Permission – for use of book, eBook, or Journal content
Accessibility – to request an alternate format of an AMS title
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