When an ideal diatomic gas is heated at constant pressure then the fraction of heat energy which is used to increase the internal energy of gas system, is
A
37
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B
35
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C
57
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D
25
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Solution
The correct option is C57 Heat at constant pressure,
ΔQ=nCPΔT. . . . . . .(1)
where, n= no. of moles
CP= molar heat capacity at constant pressure
for diatomic gas, CP=7R2, CV=5R2
So, ΔQ=n(7R2)ΔT. . . . . .(2)
Change in internal energy at constant volume,
ΔU=nCVΔT
ΔU=n(5R2)ΔT. . . . .(3)
ratio, ΔUΔQ=n5R2ΔTn7R2ΔT=57
Hence, 5/7 part of heat supplied is used to increase the internal energy