INGENIA

MEC-04

Carnot efficiency

η = 1 − Tc/Th between two thermal reservoirs.

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Heat enginesCarnot 1824

Governing equation

η=1−TcTh\eta = 1-\dfrac{T_c}{T_h}

Th∈[300,2000]T_h \in \left[300, 2000\right]

where

T_h
Hot reservoir (K)
T_c
Cold reservoir (K)
\eta
Carnot efficiency (—)

The figure, part by part

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MEC-04 · phase
00:0 / 00:08
①

Governing law — red

η=1−TcTh\eta = 1-\dfrac{T_c}{T_h}

Th∈[300,2000]T_h \in \left[300, 2000\right]

Th=300T_h = 300η=0\eta = 0

②

Domain of the variable — blue

T_h_{\min} = 300,\quad T_h_{\max} = 2000

Th∈[300,2000]T_h \in \left[300, 2000\right]

Th=300T_h = 300Th=300T_h = 300

③

Response curve — green

η=1−TcTh\eta = 1-\dfrac{T_c}{T_h}

Th∈[300,2000]T_h \in \left[300, 2000\right]

Th=300T_h = 300η=0\eta = 0

④

Rate of change — amber

dηdTh\frac{\mathrm{d}\eta}{\mathrm{d}T_h}

Th∈[300,2000]T_h \in \left[300, 2000\right]

Th=310.7T_h = 310.7η′=0.003\eta^{\prime} = 0.003

Lecture brief

Historical brief

Machine design grew from Coulomb torsion and Hertz contact (1881) through Soderberg fatigue and the heat-engine cycle. The lab writes shaft, bearing, contact and thermodynamic limits in SI. This sheet (MEC-04 — Carnot efficiency) is the form associated with Carnot 1824. Working symbols: ThT_h, TcT_c →\rightarrow η\eta. Carnot proved that no engine between two temperatures can beat the reversible ratio 1−Tc/Th, the bound of the second law.

Purpose

Purpose: compute η\eta from ThT_h, TcT_c in Mechanical via η=1−TcTh\eta = 1-\dfrac{T_c}{T_h} η = 1 − Tc/Th between two thermal reservoirs. Use it when a real mechanical question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given Th=800.000 KT_h = 800.000\,\mathrm{K}, Tc=300.000 KT_c = 300.000\,\mathrm{K}, the governing relation η=1−TcTh\eta = 1-\dfrac{T_c}{T_h} yields η=0.6250 —\eta = 0.6250\,\mathrm{—}. Ideal reversible cycle, Kelvin temperatures. Move a slider: the numbers are this situation, not a canned story.

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Outputs

  • Carnot efficiency \eta0.6250 —
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MEC-04 · phase
00:0 / 00:08

Narration of this film

Ideal reversible cycle, Kelvin temperatures.

Carnot proved that no engine between two temperatures can beat the reversible ratio 1−Tc/Th, the bound of the second law.

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Watch on YouTube