In 1949, Lars Onsager in his famous note on statistical hydrodynamics conjectured
that weak solutions to the 3-D incompressible Euler equations belonging to Hölder
spaces with Hölder exponent greater than 1/3 conserve kinetic energy; conversely, he
conjectured the existence of solutions belonging to any Hölder space with exponent less
than 1/3 which do not conserve kinetic energy. The first part, relating to conservation
of kinetic energy, has since been confirmed (cf. [Eyi94, CWT94]). The second part,
relating to the existence of non-conservative solutions, remains an open conjecture and
is the subject of this dissertation.
In groundbreaking work of De Lellis and Székelyhidi Jr. [DLSJ12a, DLSJ12b], the
authors constructed the first examples of non-conservative Hölder continuous weak solutions to the Euler equations. The construction was subsequently improved by Isett
[Ise12, Ise13a], introducing many novel ideas in order to construct 1/5 − ε Hölder continuous weak solutions with compact support in time.
Adhering more closely to the original scheme of De Lellis and Székelyhidi Jr., we
present a comparatively simpler construction of 1/5 − ε Hölder continuous nonconservative weak solutions which may in addition be made to obey a prescribed kinetic
energy profile.¹ Furthermore, we extend this scheme in order to construct weak nonconservative solutions to the Euler equations whose Hölder 1/3 − ε norm is Lebesgue
integrable in time.
The dissertation will be primarily based on three papers: [BDLSJ13], [Buc13] and
[BDLS14] – the first and third paper being in collaboration with De Lellis and Székelyhidi Jr.
Author(s): Tristan Buckmaster
Series: PhD thesis
Publisher: Universität Leipzig
Year: 2014
Language: English
Pages: 105
City: Leipzig
Introduction
The Euler Equation
The Onsager Conjecture
References and Remarks
Outline of Convex Integration Scheme
Convex Integration and the Approach of De Lellis and Székelyhidi Jr. to Onsager's Conjecture
The Convex Integration Scheme of Isett
An Examination of Scales
Convergence of the Energy
References and Remarks
Cancellation of low frequency error
Beltrami Flows
The Operator R
References and Remarks
Minimisation of Transport Error
The Principal Transport Error
Transport Error of Previous Reynolds Stress
Transport Estimates
References and Remarks
Perturbation estimates
Additional Notation and Parameter Orderings
Estimates on Components of Perturbation
References and Remarks
Reynolds Stress Estimates
Reynolds Stress Estimates
References and Remarks
Proof of Theorem 1.2.2
Estimates on the Energy
Main Proposition and Choice of Parameters
Conclusion of Proof of Theorem 1.2.2
References and Remarks
Proof of Theorem 1.2.3
Bookkeeping, Partitioning and Parameter Choice
Main Proposition and Parameter Inequalities
Conclusion of the Proof of Theorem 1.2.3
References and Remarks
Appendix
Hölder spaces
Linear Partial Differential Equation Theory
References