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
The barrel of a bicycle pump holds 3.00×10−4m3 of air at 1.00×105Pa and 290K. The outlet is blocked and the air is compressed quasistatically and adiabatically to one fifth of its volume, with no friction at the piston. Treat the air as an ideal diatomic gas with constant heat capacities, CV=25NkB and γ=7/5. Use ΔU=Q+W with W the work done on the gas, and kB=1.381×10−23JK−1.
((a)) Find the temperature of the air at the end of the compression.
((b)) Find the work done on the air during the compression.
((c)) This compression is now used as the adiabatic compression leg of a Carnot cycle running between 290K and the temperature found in (a). Find the efficiency of that cycle.
((d)) In the cycle, the isothermal expansion at the hot temperature takes the gas from 6.00×10−5m3 to 1.20×10−4m3. Find the heat taken in on that leg and the net work delivered per cycle.