The vessel contains an ideal monoatomic gas which expands at constant pressure when heat is given when then work done in expansion is
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considering the isobaric process
we already know that
Q=nΔT
W=nRΔT
for isobaric process=γRγ-1
=γRγ-1
Here γRγ denotes the adiabatic index or heat capacity ratio.
For the mono atomic gases γ=53
⇒ΔWΔQ=R=γ-1γ
=53-153=0.4
=40%
Finally It is the fraction of heat supplied for external work or energy.
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