For isothermal $AB$: $Q_{AB} = nRT\ln 2$ (heat absorbed)
For isochoric $BC$: volume constant, pressure and temperature decrease
For isobaric $CA$: compression back to initial state
$$\eta = 1 - \frac{\ln 2}{2\ln 2 - 1}$$
Verified 30 May 2026.
An ideal gas undergoes a cyclic process $ABCA$ where $AB$ is isothermal expansion at $T = 400\,\text{K}$ from volume $V$ to $2V$, $BC$ is isochoric cooling, and $CA$ is isobaric compression. The efficiency of the cycle is:
$1 - \frac{\ln 2}{2\ln 2 - 1}$
$1 - \frac{1}{1 + \ln 2}$
$1 - \frac{1}{2\ln 2}$
$\frac{\ln 2}{1 + \ln 2}$
For isothermal $AB$: $Q_{AB} = nRT\ln 2$ (heat absorbed)
For isochoric $BC$: volume constant, pressure and temperature decrease
For isobaric $CA$: compression back to initial state
$$\eta = 1 - \frac{\ln 2}{2\ln 2 - 1}$$
Sign in to track your attempts and accuracy.
Sign in to keep a private note on this question. Nothing you write is ever public.
An ideal gas undergoes an isothermal expansion. Which of the following is true?
The efficiency of a Carnot engine operating between temperatures T₁ (source) and T₂ (sink) is:
An ideal gas undergoes isothermal expansion at temperature T. If the volume doubles, by what factor does the pressure change?
The molar specific heat of a gas in a process PV² = constant is:
For an ideal gas undergoing isothermal process