Convex integration applied to the multi-dimensional compressible Euler equations [electronic resource] / Simon Markfelder.

Intro
Preface
Contents
Part I The Problem Studied in This Book
1 Introduction
1.1 The Euler Equations
1.2 Weak Solutions and Admissibility
1.3 Overview on Well-Posedness Results
1.4 Structure of This Book
2 Hyperbolic Conservation Laws
2.1 Formulation of a Conservation Law
2.2 Initial Boundary Value Problem
2.3 Hyperbolicity
2.4 Companion Laws and Entropies
2.5 Admissible Weak Solutions
3 The Euler Equations as a Hyperbolic Systemof Conservation Laws
3.1 Barotropic Euler System
3.1.1 Hyperbolicity
3.1.2 Entropies

3.1.3 Admissible Weak Solutions
3.2 Full Euler System
3.2.1 Hyperbolicity
3.2.2 Entropies
3.2.3 Admissible Weak Solutions
Part II Convex Integration
4 Preparation for Applying Convex Integrationto Compressible Euler
4.1 Outline and Preliminaries
4.1.1 Adjusting the Problem
4.1.2 Tartar's Framework
4.1.3 Plane Waves and the Wave Cone
4.1.4 Sketch of the Convex Integration Technique
4.2 -Convex Hulls
4.2.1 Definitions and Basic Facts
4.2.2 The HN-Condition and a Way to Define U
4.2.3 The -Convex Hull of Slices

4.2.4 The -Convex Hull if the Wave Cone is Complete
4.3 The Relaxed Set U Revisited
4.3.1 Definition of U
4.3.2 Computation of U
4.4 Operators
4.4.1 Statement of the Operators
4.4.2 Lemmas for the Proof of Proposition 4.4.1
4.4.3 Proof of Proposition 4.4.1
5 Implementation of Convex Integration
5.1 The Convex-Integration-Theorem
5.1.1 Statement of the Theorem
5.1.2 Functional Setup
5.1.3 The Functionals I0 and the Perturbation Property
5.1.4 Proof of the Convex-Integration-Theorem
5.2 Proof of the Perturbation Property
5.2.1 Lemmas for the Proof

5.2.2 Proof of Lemma 5.2.4
5.2.3 Proof of Lemma 5.2.1 Using Lemmas 5.2.2, 5.2.3and 5.2.4
5.2.4 Proof of the Perturbation Property Using Lemma 5.2.1
5.3 Convex Integration with Fixed Density
5.3.1 A Modified Version of the Convex-Integration-Theorem
5.3.2 Proof the Modified Perturbation Property
Part III Application to Particular Initial (Boundary) Value Problems
6 Infinitely Many Solutions of the Initial Boundary Value Problem for Barotropic Euler
6.1 A Simple Result on Weak Solutions
6.2 Possible Improvements to Obtain Admissible Weak Solutions

6.3 Further Possible Improvements
7 Riemann Initial Data in Two Space Dimensionsfor Isentropic Euler
7.1 One-Dimensional Self-Similar Solution
7.2 Summary of the Results on Non-/Uniqueness
7.3 Non-Uniqueness Proof if the Self-Similar Solution Consists of One Shock and One Rarefaction
7.3.1 Condition for Non-Uniqueness
7.3.2 The Corresponding System of Algebraic Equations and Inequalities
7.3.3 Simplification of the Algebraic System
7.3.4 Solution of the Algebraic System if the Rarefaction is ``Small''
7.3.5 Proof of Theorem 7.3.1 via an Auxiliary State