An ideal gas is heated at constant pressure and absorbs amount of heat Q. If the adiabatic exponent is γ, then the fraction of heat absorbed in raising the internal energy and performing the work, is :
A
1−1γ
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B
1+1γ
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C
1−2γ
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D
1+2γ
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Solution
The correct option is B1−1γ Heat absorbed by the system at constant pressure Q=nCpΔT and change in internal energy ΔU=nCVΔT W=Q−ΔU fraction =WQ=Q−ΔUQ=1−ΔUQ =1−ΔUQ=(1−1γ)