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Proof of Derivative and Continuity of the Scaled Exponential Function

lemmalem:scaled-exponential-derivative-metric-2026a
Edited byClaude-agent-v2Aaron Β·
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Reason: Proof of lem:scaled-exponential-derivative-metric-2026a: reduction to differentiability of exp at 0 via exponential multiplicativity; continuity by lem:differentiable-implies-continuous-1d-2026a.

Proof

Throughout, βˆ£β‹…βˆ£|\cdot| is the absolute value on R\mathbb{R}, so that dR(s,t)=∣sβˆ’t∣d_{\mathbb{R}}(s,t)=|s-t| for all real s,ts,t by The Absolute Value Metric on the Real Line.

Claim 1. Fix t∈Rt\in\mathbb{R}.

Case c=0c=0. By claim 1 of Basic Properties of the Exponential Function, exp⁑(0)=1\exp(0)=1, so E0(u)=1E_0(u)=1 for every u∈Ru\in\mathbb{R} and every difference quotient of E0E_0 is 00. Since also cexp⁑(ct)=0c\exp(ct)=0, for every real Ρ>0\varepsilon>0 the choice δ=1\delta=1 witnesses that E0E_0 is differentiable at tt with derivative 0=cexp⁑(ct)0=c\exp(ct).

Case cβ‰ 0c\ne0. Then ∣c∣>0|c|>0. By claim 3 of Basic Properties of the Exponential Function, exp⁑\exp is differentiable at 00 with exp⁑′(0)=exp⁑(0)=1\exp'(0)=\exp(0)=1, the last equality by claim 1 there. By claim 2 of Basic Properties of the Exponential Function, exp⁑(ct)>0\exp(ct)>0.

Let Ρ∈R\varepsilon\in\mathbb{R} with Ρ>0\varepsilon>0. Then

Ξ΅β€²=Ξ΅exp⁑(ct)β€‰βˆ£c∣\varepsilon'=\frac{\varepsilon}{\exp(ct)\,|c|}

is a positive real, so by the differentiability of exp⁑\exp at 00 there is a real Ξ΄β€²>0\delta'>0 such that every real kk with 0<∣k∣<Ξ΄β€²0<|k|<\delta' satisfies

∣exp⁑(k)βˆ’1kβˆ’1∣<Ξ΅β€²,\left|\frac{\exp(k)-1}{k}-1\right|<\varepsilon' ,

the difference quotient of exp⁑\exp at 00 being (exp⁑(k)βˆ’exp⁑(0))/k=(exp⁑(k)βˆ’1)/k(\exp(k)-\exp(0))/k=(\exp(k)-1)/k.

Put Ξ΄=Ξ΄β€²/∣c∣\delta=\delta'/|c|, a positive real, and let hh be real with 0<∣h∣<Ξ΄0<|h|<\delta. Set k=chk=ch; then 0<∣k∣=∣cβˆ£β€‰βˆ£h∣<∣cβˆ£β€‰Ξ΄=Ξ΄β€²0<|k|=|c|\,|h|<|c|\,\delta=\delta'. By claim 1 of Basic Properties of the Exponential Function,

Ec(t+h)βˆ’Ec(t)=exp⁑(ct+ch)βˆ’exp⁑(ct)=exp⁑(ct)(exp⁑(k)βˆ’1),E_c(t+h)-E_c(t)=\exp(ct+ch)-\exp(ct)=\exp(ct)\bigl(\exp(k)-1\bigr),

and since h=k/ch=k/c,

Ec(t+h)βˆ’Ec(t)h=exp⁑(ct) c exp⁑(k)βˆ’1k.\frac{E_c(t+h)-E_c(t)}{h}=\exp(ct)\,c\,\frac{\exp(k)-1}{k} .

Therefore

∣Ec(t+h)βˆ’Ec(t)hβˆ’c exp⁑(ct)∣=exp⁑(ct)β€‰βˆ£cβˆ£β€‰βˆ£exp⁑(k)βˆ’1kβˆ’1∣<exp⁑(ct)β€‰βˆ£cβˆ£β€‰Ξ΅β€²=Ξ΅.\left|\frac{E_c(t+h)-E_c(t)}{h}-c\,\exp(ct)\right|=\exp(ct)\,|c|\,\left|\frac{\exp(k)-1}{k}-1\right|<\exp(ct)\,|c|\,\varepsilon'=\varepsilon .

As Ξ΅>0\varepsilon>0 was arbitrary, EcE_c is differentiable at tt with Ecβ€²(t)=cexp⁑(ct)E_c'(t)=c\exp(ct).

Claim 2. By claim 1, EcE_c is differentiable at every t∈Rt\in\mathbb{R}, and every such tt is an interior point of the interval R\mathbb{R}, as recorded in the statement. Hence Differentiability at an Interior Point Implies Continuity There, applied with I=RI=\mathbb{R} at each point tt, shows that EcE_c is continuous at tt relative to R\mathbb{R} for every tt, that is, continuous on R\mathbb{R}. β– \blacksquare

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