Chapter
1.2 Gas dynamics in lagrangian variables
Criticism of the change of variables
1.3 The equation of road traffic
1.5 Magneto-hydrodynamics
A simplified model of waves
1.6 Hyperelastic materials
1.7 Singular limits of dispersive equations
2 Scalar equations in dimension d = 1
2.1 Classical solutions of the Cauchy problem
Non-linear case. The method of characteristics
2.2 Weak solutions, non-uniqueness
The Rankine–Hugoniot condition
Non-uniqueness for the Cauchy problem
2.3 Entropy solutions, the Kružkov existence theorem
Approximate solutions; entropy inequalities
Existence and uniqueness for the Cauchy problem
Application: admissible discontinuities
Piecewise smooth entropy solutions
Self-similar solutions. Rarefactions
The solution of the Riemann problem
2.5 The case of f convex. The Lax formula
The Hamilton–Jacobi equation
2.6 Proof of Theorem 2.3.5: existence
The approach by semi-groups
2.7 Proof of Theorem 2.3.5: uniqueness
An inequality for two entropy solutions
Integration of the inequality (2.19)
End of the proof of Proposition 2.3.6
Initial datum with bounded total variation
Uniqueness: the duality method
3 Linear and quasi-linear systems
3.1 Linear hyperbolic systems
Geometric conditions of hyperbolicity
3.2 Quasi-linear hyperbolic systems
3.4 Entropies, convexity and hyperbolicity
3.5 Weak solutions and entropy solutions
The Rankine–Hugoniot condition
3.6 Local existence of smooth solutions
Indications about the proof
Convergence of the iterative scheme
4 Dimension d = 1, the Riemann problem
4.1 Generalities on the Riemann problem
Local description of the Hugoniot locus
Proof of Lemmas 4.3.2 and 4.3.3
Genuinely non-linear characteristic fields
4.4 Contact discontinuities
4.5 Rarefaction waves. Wave curves
Parametrisation of wave curves
The form of the solution of the Riemann problem
Local existence of the solution of the Riemann problem
4.7 The solution of the Riemann problem for the p-system
The solution of the Riemann problem
4.8 The solution of the Riemann problem for gas dynamics
Parametrisation of shock curves
The solution of the Riemann problem
The case of a perfect gas
5.1 Functions of bounded variation
5.2 Description of the scheme
Supplements apropos of the local Riemann problem
5.6 The example of Nishida
The isothermal model of gas dynamics
5.7 2 × 2 Systems with diminishing total variation
5.9 Supplementary remarks
‘Continuous’ Glimm functional
6 Second order perturbations
6.1 Dissipation by viscosity
Dissipation or production of entropy
Partially hyperbolic systems
6.2 Global existence in the strictly dissipative case
Estimate of the derivatives
Extension of the solution…
Existence with a small diffusion
6.3 Smooth convergence as…
Two most favourable cases
Uniformity of the existence times
6.4 Scalar case. Accuracy of approximation
7 Viscosity profiles for shock waves
7.1 Typical example of a limit of viscosity solutions
Profiles vs. Lax’s entropy condition
Profile vs. Lax’s shock condition
7.2 Existence of the viscosity profile for a weak shock
The case of weak shocks with B = b(u)I
Extensions of Theorem 7.2.1…
7.3 Profiles for gas dynamics
Isentropic fluid with viscosity
Generalities on the stability of profiles
7.5 Stability of the profile for a Lax shock
Non-linear diffusion waves
Calculation of the diffusion waves
7.6 Influence of the diffusion tensor
7.7 Case of over-compressive shocks
Instability of the over-compressive shock