A Carnot engine uses atoms of helium

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · The laws of thermodynamics · The laws of thermodynamics

Thermal Physics, Ch Heat engines, refrigerators and the Carnot cycle

Problem

A Carnot engine uses N=2.00×1022N = 2.00\times10^{22} atoms of helium, treated as an ideal monatomic gas with CV=32NkBC_V = \tfrac32 Nk_B and γ=5/3\gamma = 5/3, between reservoirs at 450 K450\,\mathrm{K} and 280 K280\,\mathrm{K}. The isothermal expansion at 450 K450\,\mathrm{K} triples the volume. All four legs are quasistatic and frictionless, and heat crosses only between bodies at the same temperature. Take kB=1.381×10−23 J K−1k_B = 1.381\times10^{-23}\,\mathrm{J\,K^{-1}}, and use ΔU=Q+W\Delta U = Q + W with WW the work done on the gas. ((a)) Find the heat QhQ_h absorbed on the hot isotherm. ((b)) Find the work done on the gas during the adiabatic expansion from 450 K450\,\mathrm{K} to 280 K280\,\mathrm{K}. ((c)) Show that the two adiabatic legs contribute no net work to the cycle, and find the net work delivered per cycle. ((d)) Find the efficiency, once from the two heats and once from the two temperatures.

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