First-order Sobolev space Created 2026-09-24 Updated 2026-09-24
For an open set and , the first-order Sobolev space iswhere each is a weak derivative. Its standard norm is .
One-dimensional Sobolev representative Created 2026-09-24 Updated 2026-09-24
Every element of for has an absolutely continuous representative. Its ordinary derivative exists almost everywhere, equals its weak derivative, and belongs to .
Past exam of the mathematics course of the University of Cambridge 2025 iii Paper 105 1 d Solution Created 2026-09-24 Updated 2026-09-24
Testing the weak formulation with the constant function proves the necessary compatibility conditionAssume first that is connected and this condition holds. On the mean-zero Sobolev spaceuse the norm . To prove the needed Poincare-Wirtinger inequality, suppose it failed. There would be with and . The Rellich-Kondrachov compactness theorem gives a subsequence converging strongly in and weakly in to a function . Its weak derivative vanishes, so connectedness makes constant; its zero mean makes it zero. This contradicts . Hence is an equivalent Hilbert space norm on .
DefineBoundedness of makes a bounded bilinear form, while uniform ellipticity givesso it is a coercive bilinear form. The Cauchy-Schwarz inequality and the Poincare-Wirtinger inequality make a bounded linear functional. The Lax-Milgram theorem supplies a unique satisfying for every mean-zero . For arbitrary , subtract its mean; the omitted constant contributes zero on both sides because and . Thus solves the original problem.
If two solutions exist, their difference satisfies , so uniform ellipticity gives . It is therefore constant on . The solution is unique up to an additive constant, and its mean-zero representative is unique. If is disconnected, the precise condition is on every connected component , and one independent additive constant remains on each component.
Past exam of the mathematics course of the University of Cambridge 2025 iii Paper 105 2 a Solution Created 2026-09-24 Updated 2026-09-24
For , the function is the th weak derivative whenfor every test function . This is the integration by parts identity with no boundary term and agrees with the ordinary derivative whenever is classically differentiable.
For , the first-order Sobolev space iswith norm, for example,Functions equal almost everywhere represent the same Sobolev element.
Past exam of the mathematics course of the University of Cambridge 2025 iii Paper 105 2 b Solution Created 2026-09-24 Updated 2026-09-24
Let be the weak derivative and defineThe fundamental theorem of calculus for Lebesgue integration makes an absolutely continuous function, differentiable almost everywhere, with almost everywhere. The distributional derivative of is zero. A locally integrable function with zero distributional derivative on a connected interval is equal almost everywhere to a constant . Consequentlyis an absolutely continuous representative of , and almost everywhere.
Past exam of the mathematics course of the University of Cambridge 2025 iii Paper 105 2 c Solution Created 2026-09-24 Updated 2026-09-24
Write points of as with . For , translate into the domain byContinuity of translations in applied to givesas . Choose a standard mollifier supported in a ball of radius . For , the convolutiononly samples points with first coordinate greater than , so it is well-defined and smooth throughout . The approximation-to-the-identity theorem, applied also to each weak derivative, allows to be chosen so thatTaking and using the triangle inequality proves the density of smooth functions in a Sobolev space.