The ratio of work done by an ideal diatomic gas to the heat supplied by the gas in an isobaric process is
57
35
27
53
ΔU=nCVΔT=n52RΔTΔQ=nCVΔT=n72RΔTW=ΔQ−ΔU=n72RΔT=n52RΔT=nRΔTWΔU=27