∑ajk∂2jku=f
the theory of weak solutions in Sobolev spaces cannot be employed when the coefficient a is not differentiable because in this case the intergration-by-parts formula is not available. In the course we will explore an alternative solution theory based on the notion of viscosity solutions.cyan=lecture |
yellow=discussion of a problem sheet (and possibly lecture) |
magenta=self-study |
grey=no class |
Week | Friday | Exercises | Syllabus | References |
---|---|---|---|---|
42 | 18 Oct | definition of viscosity solutions | [G] §1 and §4 | |
43 | 25 Oct | jets and semicontinuous envelopes | [G] §5 | |
44 | 1 Nov | jet closures; Dirichlet problem | [G] Defs. 2.32, 2.38, 2.39 | |
45 | 8 Nov | Sheet 1 | ||
46 | 15 Nov | Sheet 2 | ||
47 | 22 Nov | comparison principle, Perron's method | [G] §6 | |
48 | 29 Nov | |||
49 | 6 Dec | |||
50 | 13 Dec 8-10 | Lecture | ||
50 | 13 Dec 10-12 | Exercise class | ||
51 | no class; shifted to week 50 | |||
2 | 10 Jan | |||
3 | 17 Jan | |||
4 | 24 Jan | |||
5 | 31 Jan | |||
6 | 7 Feb |