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Proof of Chain Rule for One-Dimensional Derivatives

lemmalem:chain-rule-1d-2026a
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Reason: Proof of lem:chain-rule-1d-2026a by the increment (Caratheodory) function of g at gamma(t_0), which makes the factorization of the difference quotient valid with no case split on whether gamma attains gamma(t_0) nearby. Exposure-clean.

Proof

Throughout, βˆ£β‹…βˆ£|\cdot| is the absolute value on R\mathbb{R}. Write s0=Ξ³(t0)s_0=\gamma(t_0), A=gβ€²(s0)A=g'(s_0) and B=Ξ³β€²(t0)B=\gamma'(t_0), the derivatives supplied by the hypotheses.

Step 0 (two elementary facts).

(a) If 0≀c0\le c and p≀qp\le q then cp≀cqcp\le cq. If c=0c=0 both products are 00; if 0<c0<c and p=qp=q they are equal; and if 0<c0<c and p<qp<q then cp<cqcp<cq by claim 10 of Elementary Order Arithmetic in an Ordered Field.

(b) For every x∈Rx\in\mathbb{R} one has 0<∣x∣+10<|x|+1, the inverse (∣x∣+1)βˆ’1(|x|+1)^{-1} exists and is positive, and ∣xβˆ£β€‰(∣x∣+1)βˆ’1≀1|x|\,(|x|+1)^{-1}\le 1. By claim 1 of Properties of the Absolute Value in an Ordered Field, 0β‰€βˆ£x∣0\le|x|, and 0<10<1 by claim 6 of Elementary Order Arithmetic in an Ordered Field; claim 3 of that lemma, applied to the strict inequality 0<10<1 and the inequality 0β‰€βˆ£x∣0\le|x|, gives 0<1+∣x∣=∣x∣+10<1+|x|=|x|+1, so claim 7 supplies the positive inverse. Claim 1 of that lemma turns 0<10<1 into ∣x∣<∣x∣+1|x|<|x|+1, and fact (a) with c=(∣x∣+1)βˆ’1c=(|x|+1)^{-1} gives ∣xβˆ£β€‰(∣x∣+1)βˆ’1≀(∣x∣+1)(∣x∣+1)βˆ’1=1|x|\,(|x|+1)^{-1}\le(|x|+1)(|x|+1)^{-1}=1.

Step 1 (the increment function of gg). Define Φ:J→R\Phi:J\to\mathbb{R} by

Ξ¦(s)=(g(s)βˆ’g(s0))(sβˆ’s0)βˆ’1forΒ s∈JΒ withΒ sβ‰ s0,Ξ¦(s0)=A,\Phi(s)=\bigl(g(s)-g(s_0)\bigr)(s-s_0)^{-1}\quad\text{for } s\in J \text{ with } s\ne s_0,\qquad \Phi(s_0)=A,

the inverse existing because sβ‰ s0s\ne s_0 gives sβˆ’s0β‰ 0s-s_0\ne0.

(1a) For every s∈Js\in J, g(s)βˆ’g(s0)=Ξ¦(s) (sβˆ’s0)g(s)-g(s_0)=\Phi(s)\,(s-s_0). For sβ‰ s0s\ne s_0 this is field arithmetic, using (sβˆ’s0)βˆ’1(sβˆ’s0)=1(s-s_0)^{-1}(s-s_0)=1; for s=s0s=s_0 both sides are 00.

(1b) For every Ρ∈R\varepsilon\in\mathbb{R} with 0<Ξ΅0<\varepsilon there is η∈R\eta\in\mathbb{R} with 0<Ξ·0<\eta such that every s∈Js\in J with ∣sβˆ’s0∣<Ξ·|s-s_0|<\eta satisfies ∣Φ(s)βˆ’A∣<Ξ΅|\Phi(s)-A|<\varepsilon. By hypothesis s0s_0 is an interior point of JJ at which gg is differentiable with derivative AA, so the definition of the derivative supplies Ξ·\eta with 0<Ξ·0<\eta such that every k∈Rk\in\mathbb{R} with 0<∣k∣<Ξ·0<|k|<\eta and s0+k∈Js_0+k\in J satisfies

∣(g(s0+k)βˆ’g(s0))kβˆ’1βˆ’A∣<Ξ΅.\Bigl|\bigl(g(s_0+k)-g(s_0)\bigr)k^{-1}-A\Bigr|<\varepsilon .

Let s∈Js\in J with ∣sβˆ’s0∣<Ξ·|s-s_0|<\eta. If s=s0s=s_0 then Ξ¦(s)βˆ’A=Aβˆ’A=0\Phi(s)-A=A-A=0, and ∣0∣=0<Ξ΅|0|=0<\varepsilon by claim 1 of Properties of the Absolute Value in an Ordered Field. Otherwise sβˆ’s0β‰ 0s-s_0\ne0, hence 0<∣sβˆ’s0∣0<|s-s_0| by claim 1 of that lemma; taking k=sβˆ’s0k=s-s_0, for which s0+k=s∈Js_0+k=s\in J, the displayed estimate is exactly ∣Φ(s)βˆ’A∣<Ξ΅|\Phi(s)-A|<\varepsilon.

Step 2 (a bound on the difference quotients of Ξ³\gamma). For h∈Rh\in\mathbb{R} with hβ‰ 0h\ne0 and t0+h∈It_0+h\in I set

Q(h)=(Ξ³(t0+h)βˆ’Ξ³(t0))hβˆ’1,soΒ thatΞ³(t0+h)βˆ’Ξ³(t0)=h Q(h).Q(h)=\bigl(\gamma(t_0+h)-\gamma(t_0)\bigr)h^{-1},\qquad\text{so that}\qquad \gamma(t_0+h)-\gamma(t_0)=h\,Q(h).

Since 0<10<1 by claim 6 of Elementary Order Arithmetic in an Ordered Field, differentiability of Ξ³\gamma at t0t_0 with derivative BB supplies Ξ΄1\delta_1 with 0<Ξ΄10<\delta_1 such that every hh with 0<∣h∣<Ξ΄10<|h|<\delta_1 and t0+h∈It_0+h\in I satisfies ∣Q(h)βˆ’B∣<1|Q(h)-B|<1. For such hh, claim 3 of Properties of the Absolute Value in an Ordered Field gives ∣Q(h)βˆ£βˆ’βˆ£Bβˆ£β‰€βˆ£βˆ£Q(h)βˆ£βˆ’βˆ£B∣∣|Q(h)|-|B|\le\bigl||Q(h)|-|B|\bigr|, which is at most ∣Q(h)βˆ’B∣|Q(h)-B| by claim 7 of that lemma; so ∣Q(h)βˆ£βˆ’βˆ£B∣<1|Q(h)|-|B|<1 by claim 2 of Elementary Order Arithmetic in an Ordered Field, and adding ∣B∣|B| to both sides, by claim 1 of that lemma,

∣Q(h)∣<∣B∣+1.|Q(h)|<|B|+1 .

Step 3 (the estimate). Let Ρ∈R\varepsilon\in\mathbb{R} with 0<Ξ΅0<\varepsilon. By claim 8 of Elementary Order Arithmetic in an Ordered Field, 0<Ξ΅β‹…2βˆ’10<\varepsilon\cdot2^{-1} and Ξ΅β‹…2βˆ’1+Ξ΅β‹…2βˆ’1=Ξ΅\varepsilon\cdot2^{-1}+\varepsilon\cdot2^{-1}=\varepsilon. By Step 0 (b) the inverses (∣B∣+1)βˆ’1(|B|+1)^{-1} and (∣A∣+1)βˆ’1(|A|+1)^{-1} exist and are positive, so by claim 5 of that lemma the numbers

Ξ΅1=Ξ΅β‹…2βˆ’1 (∣B∣+1)βˆ’1,Ξ΅2=Ξ΅β‹…2βˆ’1 (∣A∣+1)βˆ’1\varepsilon_1=\varepsilon\cdot2^{-1}\,(|B|+1)^{-1},\qquad \varepsilon_2=\varepsilon\cdot2^{-1}\,(|A|+1)^{-1}

are positive.

Let Ξ·\eta be as in Step 1 (1b) for Ξ΅1\varepsilon_1. Differentiability of Ξ³\gamma at t0t_0 supplies Ξ΄2\delta_2 with 0<Ξ΄20<\delta_2 such that every hh with 0<∣h∣<Ξ΄20<|h|<\delta_2 and t0+h∈It_0+h\in I satisfies ∣Q(h)βˆ’B∣<Ξ΅2|Q(h)-B|<\varepsilon_2. The number η (∣B∣+1)βˆ’1\eta\,(|B|+1)^{-1} is positive by claim 5. Applying claim 9 twice, let Ξ΄\delta be a least element among Ξ΄1\delta_1, Ξ΄2\delta_2 and η (∣B∣+1)βˆ’1\eta\,(|B|+1)^{-1}; since Ξ΄\delta equals one of them, 0<Ξ΄0<\delta.

Let h∈Rh\in\mathbb{R} with 0<∣h∣<Ξ΄0<|h|<\delta and t0+h∈It_0+h\in I, and put s=Ξ³(t0+h)s=\gamma(t_0+h), an element of JJ by hypothesis. By claim 2 of Elementary Order Arithmetic in an Ordered Field we have ∣h∣<Ξ΄1|h|<\delta_1, ∣h∣<Ξ΄2|h|<\delta_2 and ∣h∣<η (∣B∣+1)βˆ’1|h|<\eta\,(|B|+1)^{-1}.

First, sβˆ’s0=h Q(h)s-s_0=h\,Q(h), so ∣sβˆ’s0∣=∣hβˆ£β€‰βˆ£Q(h)∣|s-s_0|=|h|\,|Q(h)| by claim 4 of Properties of the Absolute Value in an Ordered Field. Since hβ‰ 0h\ne0, claim 1 of that lemma gives 0<∣h∣0<|h|; so Step 2 and claim 10 of Elementary Order Arithmetic in an Ordered Field give ∣hβˆ£β€‰βˆ£Q(h)∣<∣hβˆ£β€‰(∣B∣+1)|h|\,|Q(h)|<|h|\,(|B|+1), and claim 10 again, with the positive multiplier ∣B∣+1|B|+1, gives ∣hβˆ£β€‰(∣B∣+1)<η (∣B∣+1)βˆ’1(∣B∣+1)=Ξ·|h|\,(|B|+1)<\eta\,(|B|+1)^{-1}(|B|+1)=\eta. By claim 2 we conclude ∣sβˆ’s0∣<Ξ·|s-s_0|<\eta, so Step 1 (1b) yields

∣Φ(s)βˆ’A∣<Ξ΅1.|\Phi(s)-A|<\varepsilon_1 .

Second, by Step 1 (1a), the identity sβˆ’s0=h Q(h)s-s_0=h\,Q(h) and hβˆ’1h=1h^{-1}h=1,

((g∘γ)(t0+h)βˆ’(g∘γ)(t0))hβˆ’1=(g(s)βˆ’g(s0))hβˆ’1=Ξ¦(s) (sβˆ’s0) hβˆ’1=Ξ¦(s) Q(h).\bigl((g\circ\gamma)(t_0+h)-(g\circ\gamma)(t_0)\bigr)h^{-1}=\bigl(g(s)-g(s_0)\bigr)h^{-1}=\Phi(s)\,(s-s_0)\,h^{-1}=\Phi(s)\,Q(h).

By field arithmetic,

Ξ¦(s) Q(h)βˆ’AB=(Ξ¦(s)βˆ’A)Q(h)+A(Q(h)βˆ’B),\Phi(s)\,Q(h)-AB=\bigl(\Phi(s)-A\bigr)Q(h)+A\bigl(Q(h)-B\bigr),

so by claims 5 and 4 of Properties of the Absolute Value in an Ordered Field,

∣Φ(s)Q(h)βˆ’ABβˆ£β‰€βˆ£Ξ¦(s)βˆ’Aβˆ£β€‰βˆ£Q(h)∣+∣Aβˆ£β€‰βˆ£Q(h)βˆ’B∣.\bigl|\Phi(s)Q(h)-AB\bigr|\le\bigl|\Phi(s)-A\bigr|\,\bigl|Q(h)\bigr|+|A|\,\bigl|Q(h)-B\bigr| .

For the first summand, Step 0 (a) with c=∣Φ(s)βˆ’A∣c=|\Phi(s)-A|, which is nonnegative by claim 1 of Properties of the Absolute Value in an Ordered Field, together with ∣Q(h)βˆ£β‰€βˆ£B∣+1|Q(h)|\le|B|+1 from Step 2, gives ∣Φ(s)βˆ’Aβˆ£β€‰βˆ£Q(h)βˆ£β‰€βˆ£Ξ¦(s)βˆ’Aβˆ£β€‰(∣B∣+1)|\Phi(s)-A|\,|Q(h)|\le|\Phi(s)-A|\,(|B|+1); and claim 10 of Elementary Order Arithmetic in an Ordered Field, with the positive multiplier ∣B∣+1|B|+1, turns ∣Φ(s)βˆ’A∣<Ξ΅1|\Phi(s)-A|<\varepsilon_1 into ∣Φ(s)βˆ’Aβˆ£β€‰(∣B∣+1)<Ξ΅1(∣B∣+1)=Ξ΅β‹…2βˆ’1|\Phi(s)-A|\,(|B|+1)<\varepsilon_1(|B|+1)=\varepsilon\cdot2^{-1}. By claim 2 the first summand is smaller than Ξ΅β‹…2βˆ’1\varepsilon\cdot2^{-1}. For the second summand, Step 0 (a) with c=∣A∣c=|A| gives ∣Aβˆ£β€‰βˆ£Q(h)βˆ’Bβˆ£β‰€βˆ£Aβˆ£β€‰Ξ΅2=(∣Aβˆ£β€‰(∣A∣+1)βˆ’1) Ρ⋅2βˆ’1|A|\,|Q(h)-B|\le|A|\,\varepsilon_2=\bigl(|A|\,(|A|+1)^{-1}\bigr)\,\varepsilon\cdot2^{-1}, and Step 0 (b) with Step 0 (a) applied with c=Ξ΅β‹…2βˆ’1c=\varepsilon\cdot2^{-1} bounds this by Ξ΅β‹…2βˆ’1\varepsilon\cdot2^{-1}.

Adding the two bounds by claim 3 of Elementary Order Arithmetic in an Ordered Field, and using claim 2 of that lemma with the displayed triangle-inequality bound,

∣((g∘γ)(t0+h)βˆ’(g∘γ)(t0))hβˆ’1βˆ’AB∣<Ξ΅β‹…2βˆ’1+Ξ΅β‹…2βˆ’1=Ξ΅.\Bigl|\bigl((g\circ\gamma)(t_0+h)-(g\circ\gamma)(t_0)\bigr)h^{-1}-AB\Bigr|<\varepsilon\cdot2^{-1}+\varepsilon\cdot2^{-1}=\varepsilon .

Since Ξ΅\varepsilon was an arbitrary positive real number and t0t_0 is an interior point of II, the real number ABAB witnesses the definition of the derivative of g∘γg\circ\gamma at t0t_0. Hence g∘γg\circ\gamma is differentiable at t0t_0 and (g∘γ)β€²(t0)=AB=gβ€²(Ξ³(t0)) γ′(t0)(g\circ\gamma)'(t_0)=AB=g'\bigl(\gamma(t_0)\bigr)\,\gamma'(t_0). β– \blacksquare

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