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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.2/52/5
B.3/53/5
C.3/73/7
D.5/75/7

Explanation

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{C_p}.
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{C_v}.

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 UU.
Change in internal energy: It is defined as the sum of the heat transferred and the work done.
Total rise in internal energy is nCVΔTn{C_V}\Delta T, where CV{C_V} is heat capacity at constant volume, nn is number of moles and ΔT\Delta T is the temperature difference. And total energy supplied to raise the temperature of a diatomic gas at constant pressure is nCPΔTn{C_P}\Delta T, , where CP{C_P} is heat capacity at constant pressure, nn is number of moles and ΔT\Delta T is the temperature difference.
Now the fraction of the heat energy supplied which increases the internal energy of the gas is =nCVΔTnCPΔT = \dfrac{{n{C_V}\Delta T}}{{n{C_P}\Delta T}}.
We know that the ratio CV{C_V} and CP{C_P} is ff+2\dfrac{f}{{f + 2}} where ff is the number of degrees of freedom of the gas. For diatomic gases the value of ff is 55.
So the fraction of the heat energy supplied which increases the internal energy of the gas is 57\dfrac{5}{7}.

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 55 and for polyatomic gases it is as 3n63n - 6, where nn is total number of atoms in the compound, if the compound is non-linear in shape and 3n53n - 5, where nn is total number of atoms in the compound, if the compound is linear in shape.