When an ideal gas $(\gamma = \frac{5}{3})$ is heated under constant pressure, then what percentage of given heat energy will be utilised in doing external work?
Show Hint
For heating at constant pressure:
\[
\frac{W}{Q}=\frac{R}{C_P}
\]
So first find \(C_P\) from \(\gamma\), then directly calculate the fraction.
Concept:
At constant pressure:
\[
Q=nC_P\Delta T
\]
and work done is:
\[
W=P\Delta V=nR\Delta T
\]
So the fraction of heat used in external work is:
\[
\frac{W}{Q}=\frac{nR\Delta T}{nC_P\Delta T}=\frac{R}{C_P}
\]
ip
Step 1: Relate \(C_P\) with \(\gamma\).
We know:
\[
\gamma=\frac{C_P}{C_V}=\frac{5}{3}
\]
and
\[
C_P-C_V=R
\]
Also,
\[
C_P=\frac{\gamma R}{\gamma-1}
\]
Substitute \(\gamma=\frac53\):
\[
C_P=\frac{\frac53 R}{\frac53-1}
=\frac{\frac53 R}{\frac23}
=\frac52 R
\]
ip
Step 2: Find the fraction of heat used as work.
\[
\frac{W}{Q}=\frac{R}{C_P}
=\frac{R}{\frac52 R}
=\frac{2}{5}
\]
\[
\frac{W}{Q}=0.4
\]
ip
Step 3: Convert into percentage.
\[
0.4\times 100 = 40%
\]
ip
Hence, the correct answer is:
\[
\boxed{(D)\ 40%}
\]