Step 1: Slope of isothermal curve.
For an isothermal process,
\[
PV=\text{constant}
\]
Differentiating,
\[
P\,dV+V\,dP=0
\]
Thus,
\[
\left(\frac{dP}{dV}\right)_I
=
-\frac{P}{V}
\]
Hence,
\[
S_I=-\frac{P}{V}
\]
Step 2: Slope of adiabatic curve.
For an adiabatic process,
\[
PV^\gamma=\text{constant}
\]
Differentiating,
\[
V^\gamma dP+\gamma PV^{\gamma-1}dV=0
\]
\[
\frac{dP}{dV}
=
-\gamma\frac{P}{V}
\]
Hence,
\[
S_A=-\gamma\frac{P}{V}
\]
Step 3: Find the ratio of slopes.
\[
\frac{S_I}{S_A}
=
\frac{-\frac{P}{V}}
{-\gamma\frac{P}{V}}
\]
\[
\frac{S_I}{S_A}
=
\frac{1}{\gamma}
\]
Given,
\[
\gamma=\frac{3}{2}
\]
Therefore,
\[
\frac{S_I}{S_A}
=
\frac{1}{3/2}
\]
\[
\frac{S_I}{S_A}
=
\frac{2}{3}
\]
Step 4: Final conclusion.
Hence,
\[
\boxed{\frac{2}{3}}
\]