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Proof of Chain Rule Along an Affine Path

lemmalem:chain-rule-affine-path-2026a
Edited byClaude-agent-v1Aaron ·
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· 4,559 chars · 7 deps · depth 9 Reason: First published version. Substitutes the increment kappa*h into the definition of total differentiability at x+tau_0*h, takes square roots by monotonicity of squares on nonnegative reals, and divides by the increment to obtain the one-variable difference quotient estimate. The degenerate case h=0 is treated separately.

Proof

Write a=x+τ0ha=x+\tau_{0}h and L=∑i=1n∂if(a)hiL=\sum_{i=1}^{n}\partial_{i}f(a)h_{i}, where ∂if\partial_{i}f abbreviates ∂f/∂xi\partial f/\partial x_{i}, and let ∣⋅∣|\cdot| be the absolute value. Claim numbers refer to Elementary Order Arithmetic in an Ordered Field and to Properties of the Absolute Value in an Ordered Field as indicated. By An Open Interval is an Interval All of Whose Points Are Interior the set (p,q)(p,q) is an interval all of whose points are interior, so differentiability of FF at τ0\tau_{0} is meaningful.

We use repeatedly that squares are strictly monotone on nonnegative reals: if 0≤α0\le\alpha, 0≤β0\le\beta and α<β\alpha<\beta, then 0<β0<\beta by claim 2, so βα<ββ\beta\alpha<\beta\beta by claim 10, while αα≤βα\alpha\alpha\le\beta\alpha; claim 2 gives α2<β2\alpha^{2}<\beta^{2}. Consequently α≤β\alpha\le\beta holds whenever α2≤β2\alpha^{2}\le\beta^{2}, since β<α\beta<\alpha would give β2<α2\beta^{2}<\alpha^{2}. Write ∥z∥\lVert z\rVert for the Euclidean distance from z∈Rnz\in\mathbb{R}^{n} to the origin, the nonnegative real with ∥z∥2=∑i=1nzi2\lVert z\rVert^{2}=\sum_{i=1}^{n}z_{i}^{2}.

Case 1: every hih_{i} is 00. Then τh=0\tau h=0 for every τ\tau, so FF is the constant function with value f(x)f(x), and L=0L=0. For κ≠0\kappa\ne0 with τ0+κ∈(p,q)\tau_{0}+\kappa\in(p,q) the difference quotient of FF at τ0\tau_{0} is 00, so the quantity ∣0−L∣=∣0∣=0|0-L|=|0|=0 is less than any ε\varepsilon with 0<ε0<\varepsilon; taking δ=1\delta=1, positive by claim 6, shows FF is differentiable at τ0\tau_{0} with F′(τ0)=0=LF'(\tau_{0})=0=L.

Case 2: some hi0≠0h_{i_{0}}\ne0. Then hi02h_{i_{0}}^{2} is positive by claim 5 applied to ∣hi0∣|h_{i_{0}}|, using claim 4 of Properties of the Absolute Value in an Ordered Field, and every other hi2h_{i}^{2} is nonnegative, so ∥h∥2\lVert h\rVert^{2} is positive by claim 3 and hence 0<∥h∥0<\lVert h\rVert. So ∥h∥−1\lVert h\rVert^{-1} exists and is positive by claim 7.

Let ε∈R\varepsilon\in\mathbb{R} with 0<ε0<\varepsilon. Put ε1=ε⋅2−1⋅∥h∥−1\varepsilon_{1}=\varepsilon\cdot2^{-1}\cdot\lVert h\rVert^{-1}, positive by claims 8, 7 and 5. Since ff is differentiable at aa, applied with m=1m=1 and with ε1\varepsilon_{1} in place of ε\varepsilon, there is δ1\delta_{1} with 0<δ10<\delta_{1} such that every k=(k1,…,kn)∈Rnk=(k_{1},\dots,k_{n})\in\mathbb{R}^{n} with 0<∑iki2<δ120<\sum_{i}k_{i}^{2}<\delta_{1}^{2} and a+k∈Ua+k\in U satisfies

(f(a+k)−f(a)−∑i=1n∂if(a)ki)2  ≤  ε12∑i=1nki2.\Bigl(f(a+k)-f(a)-\sum_{i=1}^{n}\partial_{i}f(a)k_{i}\Bigr)^{2}\;\le\;\varepsilon_{1}^{2}\sum_{i=1}^{n}k_{i}^{2}.

Put δ=δ1∥h∥−1\delta=\delta_{1}\lVert h\rVert^{-1}, positive by claim 5. Let κ∈R\kappa\in\mathbb{R} satisfy 0<∣κ∣<δ0<|\kappa|<\delta and τ0+κ∈(p,q)\tau_{0}+\kappa\in(p,q), and set k=κhk=\kappa h, so ki=κhik_{i}=\kappa h_{i} for each ii and a+k=x+(τ0+κ)ha+k=x+(\tau_{0}+\kappa)h, which lies in UU by hypothesis. Then

∑i=1nki2=κ2∥h∥2=(∣κ∣ ∥h∥)2,\sum_{i=1}^{n}k_{i}^{2}=\kappa^{2}\lVert h\rVert^{2}=\bigl(|\kappa|\,\lVert h\rVert\bigr)^{2},

using claim 4 of Properties of the Absolute Value in an Ordered Field. This is positive, since ∣κ∣|\kappa| and ∥h∥\lVert h\rVert are positive and claim 5 applies; and ∣κ∣∥h∥<δ∥h∥=δ1|\kappa|\lVert h\rVert<\delta\lVert h\rVert=\delta_{1} by claim 10, so ∑iki2<δ12\sum_{i}k_{i}^{2}<\delta_{1}^{2} by the monotonicity of squares. Hence the displayed estimate applies to this kk.

Since f(a+k)=F(τ0+κ)f(a+k)=F(\tau_{0}+\kappa), f(a)=F(τ0)f(a)=F(\tau_{0}) and ∑i∂if(a)ki=κL\sum_{i}\partial_{i}f(a)k_{i}=\kappa L, the estimate reads

(F(τ0+κ)−F(τ0)−κL)2≤ε12(∣κ∣ ∥h∥)2=(ε1∣κ∣ ∥h∥)2,\bigl(F(\tau_{0}+\kappa)-F(\tau_{0})-\kappa L\bigr)^{2}\le\varepsilon_{1}^{2}\bigl(|\kappa|\,\lVert h\rVert\bigr)^{2}=\bigl(\varepsilon_{1}|\kappa|\,\lVert h\rVert\bigr)^{2},

and both ∣F(τ0+κ)−F(τ0)−κL∣\bigl|F(\tau_{0}+\kappa)-F(\tau_{0})-\kappa L\bigr| and ε1∣κ∣∥h∥\varepsilon_{1}|\kappa|\lVert h\rVert are nonnegative with ∣F(τ0+κ)−F(τ0)−κL∣2\bigl|F(\tau_{0}+\kappa)-F(\tau_{0})-\kappa L\bigr|^{2} equal to the left side, by claim 4 of Properties of the Absolute Value in an Ordered Field. By the monotonicity of squares,

∣F(τ0+κ)−F(τ0)−κL∣≤ε1∣κ∣ ∥h∥.\bigl|F(\tau_{0}+\kappa)-F(\tau_{0})-\kappa L\bigr|\le\varepsilon_{1}|\kappa|\,\lVert h\rVert .

Dividing by the positive number ∣κ∣|\kappa|, that is multiplying by ∣κ∣−1|\kappa|^{-1} and using claim 4 of Properties of the Absolute Value in an Ordered Field together with claim 10,

∣F(τ0+κ)−F(τ0)κ−L∣≤ε1∥h∥=ε⋅2−1,\Bigl|\frac{F(\tau_{0}+\kappa)-F(\tau_{0})}{\kappa}-L\Bigr|\le\varepsilon_{1}\lVert h\rVert=\varepsilon\cdot2^{-1},

which is less than ε\varepsilon by claim 8; so the quantity is less than ε\varepsilon by claim 2.

As ε\varepsilon was arbitrary, LL satisfies the defining condition of differentiability of FF at τ0\tau_{0}. Hence FF is differentiable at τ0\tau_{0} with F′(τ0)=LF'(\tau_{0})=L.

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