When an ideal diatomic gas is heated at constant pressure , the fraction of heat energy supplies which is used in doing work to maintain pressure constant is:
Fraction of heat energy supplied which increases the internal energy
We know that,
Number of moles the gas =n
Specific heat at constant volume =cv
Specific heat at constant pressure =cp
Change in temperature =dT
Ratio of specific heats of gas =γ
Now,
ΔUΔQ=ncvdTncpdT
ΔUΔQ=cvcp
ΔUΔQ=1γ
For diatomic gas γ=75
So,
ΔUΔQ=1γ
ΔUΔQ=57
The fraction of heat energy supplied is 57.