TheoremBase

The Chain Rule for Weak Derivatives on the Torus

Composing a class in the Sobolev space of the torus with a continuously differentiable function of bounded derivative again lies in that space, and its weak partial derivatives are given by the classical chain rule formula.

Statement

We work in the setting of The Flat Torus: Standing Notation, used here with a natural number nn satisfying 1≤n1\le n; the cell QQ, the measure space (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}), and the classes Lt(Tn)\mathcal{L}^{t}(\mathbb{T}^{n}) and spaces Lt(Tn)L^{t}(\mathbb{T}^{n}) with the class map [ ⋅ ][\,\cdot\,], for a real number tt with 1≤t1\le t, are the ones fixed there. Let ∥ ⋅ ∥t\lVert\,\cdot\,\rVert_{t} denote the LtL^{t} seminorm of (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}). Weak partial derivatives of classes and the notation ∂jU\partial_{j}U are those of The Weak Partial Derivative on the Torus, and H1(Tn)H^{1}(\mathbb{T}^{n}) is the Sobolev space fixed there. A representative of a class U∈Lt(Tn)U\in L^{t}(\mathbb{T}^{n}) is a member uu of Lt(Tn)\mathcal{L}^{t}(\mathbb{T}^{n}) with [u]=U[u]=U; two representatives of one class agree almost everywhere by The Lebesgue Space Lᵖ(μ) (i).

Let R\mathbb{R} be the real numbers and let ∣⋅∣|\cdot| be the absolute value on R\mathbb{R}. Differentiability of a function from R\mathbb{R} to R\mathbb{R} at a point, and the derivative there, are those of that definition; they apply at every point because by claim 1 of One-Dimensional Derivatives, Partial Derivatives, and Smoothness on the Real Line the set R\mathbb{R} is an interval every point of which is an interior point of it. For ϕ:R→R\phi:\mathbb{R}\to\mathbb{R} differentiable at every point of R\mathbb{R}, ϕ′\phi' denotes the function from R\mathbb{R} to R\mathbb{R} whose value at ss is the derivative of ϕ\phi at ss. We regard R\mathbb{R} also as the Euclidean space R1\mathbb{R}^{1}, which is open in itself by claim 1 of Euclidean Space Is Open in Itself; being of class C1C^{1} on R1\mathbb{R}^{1} is as defined there, and ∂1\partial_{1} denotes the partial derivative with respect to the first variable. For ψ:R→R\psi:\mathbb{R}\to\mathbb{R} and v:Q→Rv:Q\to\mathbb{R}, ψ∘v\psi\circ v denotes the function from QQ to R\mathbb{R} whose value at xx is ψ(v(x))\psi(v(x)), and for v,w:Q→Rv,w:Q\to\mathbb{R} the pointwise product v wv\,w is the function whose value at xx is v(x) w(x)v(x)\,w(x).

Let M∈RM\in\mathbb{R} satisfy 0≤M0\le M and let ϕ:R→R\phi:\mathbb{R}\to\mathbb{R} be of class C1C^{1} on R1\mathbb{R}^{1}; then ϕ\phi is differentiable at every point of R\mathbb{R} and ϕ′(s)=∂1ϕ(s)\phi'(s)=\partial_{1}\phi(s) for every s∈Rs\in\mathbb{R}, by claim 2 of One-Dimensional Derivatives, Partial Derivatives, and Smoothness on the Real Line. Suppose further that

∣ϕ′(s)∣≤Mfor every s∈R.|\phi'(s)|\le M\qquad\text{for every }s\in\mathbb{R}.

Then the following hold.

1. (Lipschitz bound) For all s,t∈Rs,t\in\mathbb{R},

∣ϕ(s)−ϕ(t)∣≤M ∣s−t∣.|\phi(s)-\phi(t)|\le M\,|s-t| .

2. (The composed class) Let U∈L2(Tn)U\in L^{2}(\mathbb{T}^{n}) and let uu be a representative of UU. Then ϕ∘u∈L2(Tn)\phi\circ u\in\mathcal{L}^{2}(\mathbb{T}^{n}); and if u~\tilde{u} is a further representative of UU, then ϕ∘u\phi\circ u and ϕ∘u~\phi\circ\tilde{u} agree almost everywhere, so that the class [ϕ∘u]∈L2(Tn)[\phi\circ u]\in L^{2}(\mathbb{T}^{n}) depends only on UU. We write ϕ(U)\phi(U) for that class.

3. (The chain rule) Let U∈H1(Tn)U\in H^{1}(\mathbb{T}^{n}), let uu be a representative of UU and, for j∈[n]j\in[n], let gjg_{j} be a representative of ∂jU\partial_{j}U. Then for every j∈[n]j\in[n] the pointwise product (ϕ′∘u) gj(\phi'\circ u)\,g_{j} belongs to L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) and

∥(ϕ′∘u) gj∥2≤M ∥gj∥2.\bigl\lVert(\phi'\circ u)\,g_{j}\bigr\rVert_{2}\le M\,\lVert g_{j}\rVert_{2} .

Moreover ϕ(U)∈H1(Tn)\phi(U)\in H^{1}(\mathbb{T}^{n}) and

∂jϕ(U)=[(ϕ′∘u) gj]for every j∈[n].\partial_{j}\phi(U)=\bigl[(\phi'\circ u)\,g_{j}\bigr]\qquad\text{for every }j\in[n].

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