During warming, θ˙=α(θ1−θ) and θ=θ1−(θ1−θ0)e−αt. During cooling, with τ=t−T, θ˙=−α(θ−θ0) and θ=θ0+(θ1−θ0)(1−e−αT)e−ατ.
N(2T)/N(0)=exp[−∫02Tβ(θ(t))dt].
Evaluation gives the implicit
equationβmax[T−αe−αT(1−e−αT)]=log100.
For
x=αT≪1,
e−x(1−e−x)=x−23x2+O(x3). Hence
23βmaxαT2∼log100 and
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