Sobolev embedding of H₀¹(Ω) in dimension two #
In dimension two the critical exponent of H¹ is infinite and the Gagliardo-Nirenberg-Sobolev
inequality at p = 2 is unavailable, since it asks p < d. On a bounded domain the embedding
into L⁴ still follows from the inequality at p = 3/2 < 2, whose conjugate exponent is 6,
together with Hölder's inequality ‖∇u‖_{L^{3/2}(Ω)} ≤ |Ω|^{1/6} ‖∇u‖_{L²(Ω)}. This is the
remark on n = 2 in the proof of Gilbarg and Trudinger's Theorem 8.1, where any exponent above
2 serves.
Main declarations #
EllipticPdes.Embedding.sobolevConstTwo: the constant.EllipticPdes.Embedding.eLpNorm_testGraph_le_two: the estimate on a test function.EllipticPdes.Embedding.eLpNorm_le_of_mem_H01_two: the estimate onH₀¹(Ω).
References #
D. Gilbarg and N. S. Trudinger, Elliptic Partial Differential Equations of Second Order,
§8.1 Theorem 8.1 (p. 180), the remark on n = 2.
The constant of the two-dimensional embedding into L⁴: Mathlib's constant at p = 3/2,
q = 4, times the Hölder factor |Ω|^{1/6}.
Equations
- EllipticPdes.Embedding.sobolevConstTwo Ω = MeasureTheory.eLpNormLESNormFDerivOfLeConst ℝ MeasureTheory.volume Ω (3 / 2) 4 * (MeasureTheory.volume Ω).toNNReal ^ (1 / 6)
Instances For
A function supported in Ω has the same Lᵖ seminorm over Ω as over the whole space,
for functions into any normed group.
Two-dimensional Sobolev inequality on a test function: the L⁴(Ω) seminorm of the
function coordinate is bounded by the sum of the L²(Ω) norms of the gradient coordinates.
Sobolev estimate on H₀¹(Ω) in dimension two, into L⁴(Ω).