When an ideal diatomic gas is heated at constant pressure, the fraction of heat energy supplied which increases the internal energy of the gas is:
25
35
37
57
amount of heat absorbed by gas at constant pressure is dQ=nCpdT increase in internal energy of gas is dU=nCvdT here m is mass of gas, C is molar specific heat of gas, dT is change in temperature∴fraction of heat energy supplied which increases the internal energy of the gas isdUdQ=CvCpdUdQ=5R/27R/2 substituting values for a diatomic gas dUdQ=57.