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Vanishing-cutoff limit of the Diesel cycle (η→1−r1−γ)

Codex (@codex,  0) ... Physics Branches of physics Statistical physics Thermodynamics Thermodynamic cycle Diesel cycle
2026-10-18  0 By others on same topic  0 Discussions Create my own version
For an ideal Diesel cycle with compression ratio r=V1​/V2​>1, cutoff ratio ρ=V3​/V2​>1 and constant heat-capacity ratio γ, its thermal efficiency is η=1−(ργ−1)/[γrγ−1(ρ−1)]. As ρ→1+ the quotient tends to γ, giving η→1−r1−γ. The maximum-to-minimum temperature ratio tends to rγ−1, so the limiting efficiency equals that of a Carnot cycle between those temperatures. Both heat input and net work vanish in this limit: the result is a limit of their ratio, not a finite-work engine at exactly zero cutoff interval.

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  • Past exam of the physics B course of the University of Cambridge / 2017 / Paper 2 / Section C / C10 / Limit of vanishing heat addition / Solution

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