Question
Question: When an ideal diatomic gas is heated at constant pressure, the fraction of the heat energy supplied ...
When an ideal diatomic gas is heated at constant pressure, the fraction of the heat energy supplied which increases the internal energy of the gas is?
A.2/5
B.3/5
C.3/7
D.5/7
Solution
Heat capacity at constant pressure: It is defined as the amount of heat energy absorbed or released by the substance with the change in temperature at constant pressure. It is represented as Cp.
Heat capacity at constant volume: It is defined as the amount of heat energy absorbed or released by the substance with the change in temperature at constant volume. It is represented as Cv.
Complete step by step answer:
Internal energy of a system: It is defined as the energy associated with the random movement of the molecules, is known as the internal energy of a system. It is represented by the symbol U.
Change in internal energy: It is defined as the sum of the heat transferred and the work done.
Total rise in internal energy is nCVΔT, where CV is heat capacity at constant volume, n is number of moles and ΔT is the temperature difference. And total energy supplied to raise the temperature of a diatomic gas at constant pressure is nCPΔT, , where CP is heat capacity at constant pressure, n is number of moles and ΔT is the temperature difference.
Now the fraction of the heat energy supplied which increases the internal energy of the gas is =nCPΔTnCVΔT.
We know that the ratio CV and CP is f+2f where f is the number of degrees of freedom of the gas. For diatomic gases the value of f is 5.
So the fraction of the heat energy supplied which increases the internal energy of the gas is 75.
Hence option D is correct.
Note:
Number of degrees of freedom of the gas is defined as the dimensions of the phase space. For diatomic gases the number of degree of freedom is 5 and for polyatomic gases it is as 3n−6, where n is total number of atoms in the compound, if the compound is non-linear in shape and 3n−5, where n is total number of atoms in the compound, if the compound is linear in shape.