TheoremBase

Checks the values of the reflection by direct computation and verifies continuity and the derivative from the epsilon-delta definitions.

Proof

Computations with real numbers are those of The Real Numbers as a Type (vi).

Proof of (i). Let u∈[a,b]u\in[a,b], so a≀u≀ba\le u\le b. Then a=a+bβˆ’b≀a+bβˆ’u≀a+bβˆ’a=ba=a+b-b\le a+b-u\le a+b-a=b, so a+bβˆ’u∈[a,b]a+b-u\in[a,b]. Hence (Values, Restriction and Equality of a Map, and the Map u↦t(u)u\mapsto t(u) as a Defined Set Symbol (v), with [a,b][a,b] for AA and BB and the expression a+bβˆ’ua+b-u for tt) there is a map ψ:[a,b]β†’[a,b]\psi:[a,b]\to[a,b] with ψ(u)=a+bβˆ’u\psi(u)=a+b-u for every u∈[a,b]u\in[a,b], and it is the only one, by Values, Restriction and Equality of a Map, and the Map u↦t(u)u\mapsto t(u) as a Defined Set Symbol (iv).

Proof of (ii) and (iii). For u,v∈[a,b]u,v\in[a,b], ψ(ψ(u))=a+bβˆ’(a+bβˆ’u)=u\psi(\psi(u))=a+b-(a+b-u)=u and ψ(u)βˆ’Οˆ(v)=vβˆ’u\psi(u)-\psi(v)=v-u, so ∣ψ(u)βˆ’Οˆ(v)∣=∣vβˆ’u∣=∣uβˆ’v∣|\psi(u)-\psi(v)|=|v-u|=|u-v|.

Proof of (iv). Since [a,b]βŠ†R[a,b]\subseteq\mathbb{R}, ψ\psi is also a map [a,b]β†’R[a,b]\to\mathbb{R}, by Functions, Values of a Function, and Functions from One Class to Another (iii). Let s∈[a,b]s\in[a,b] and let Ξ΅>0\varepsilon>0 be real; put Ξ΄=Ξ΅\delta=\varepsilon. Every t∈[a,b]t\in[a,b] with ∣tβˆ’s∣<Ξ΄|t-s|<\delta satisfies ∣ψ(t)βˆ’Οˆ(s)∣=∣tβˆ’s∣<Ξ΅|\psi(t)-\psi(s)|=|t-s|<\varepsilon, by (iii). By the Ξ΅\varepsilon-Ξ΄\delta form of continuity in The Real Line: Standing Notation and Background for Calculus on Intervals (vi), ψ\psi is continuous at ss relative to [a,b][a,b]; as ss was arbitrary, ψ\psi is continuous on [a,b][a,b], by Continuous Map Between Metric Spaces (ii).

Proof of (v). As in the proof of (iv), ψ\psi is a map [a,b]β†’R[a,b]\to\mathbb{R}. Let s∈[a,b]s\in[a,b] and let Ξ΅>0\varepsilon>0 be real; put Ξ΄=1\delta=1. For every t∈[a,b]t\in[a,b] with 0<∣tβˆ’s∣<Ξ΄0<|t-s|<\delta we have tβˆ’sβ‰ 0t-s\neq0 and ψ(t)βˆ’Οˆ(s)=sβˆ’t=βˆ’(tβˆ’s)\psi(t)-\psi(s)=s-t=-(t-s), so

∣ψ(t)βˆ’Οˆ(s)tβˆ’sβˆ’(βˆ’1)∣=∣(βˆ’1)βˆ’(βˆ’1)∣=0<Ξ΅.\Bigl|\frac{\psi(t)-\psi(s)}{t-s}-(-1)\Bigr|=|(-1)-(-1)|=0<\varepsilon .

So βˆ’1-1 is a derivative of ψ\psi at ss, by Derivative of a Real Function on an Interval (i) with [a,b][a,b] for II; hence ψ\psi is differentiable at ss and Οˆβ€²(s)=βˆ’1\psi'(s)=-1, by Derivative of a Real Function on an Interval (ii). As s∈[a,b]s\in[a,b] was arbitrary, ψ\psi is differentiable, by Derivative of a Real Function on an Interval (iii).

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