Step 1: Use the first case to find spring constant relation.
For block \(A\), volume is
\[
V_A=0.25\;m^3
\]
Let density of iron be \(\rho\).
Mass of block \(A\) is
\[
m_A=\rho V_A=0.25\rho
\]
The spring stretches by
\[
x_A=0.2\;m
\]
At equilibrium,
\[
kx_A=m_Ag
\]
\[
k(0.2)=0.25\rho g
\]
Step 2: Use the second case on inclined plane.
For block \(B\),
\[
V_B=0.75\;m^3
\]
So,
\[
m_B=0.75\rho
\]
On a smooth inclined plane of angle \(30^\circ\), the component of weight along the plane is
\[
m_Bg\sin30^\circ
\]
At equilibrium,
\[
kx_B=m_Bg\sin30^\circ
\]
\[
kx_B=0.75\rho g\cdot \frac12
\]
\[
kx_B=0.375\rho g
\]
Step 3: Find the extension of the spring.
From the first case,
\[
k(0.2)=0.25\rho g
\]
So,
\[
k=\frac{0.25\rho g}{0.2}
\]
Now,
\[
x_B=\frac{0.375\rho g}{k}
\]
Substitute the value of \(k\):
\[
x_B=
\frac{0.375\rho g}{\frac{0.25\rho g}{0.2}}
\]
\[
x_B=\frac{0.375\times 0.2}{0.25}
\]
\[
x_B=0.3\;m
\]
Step 4: Find the distance from the top along the incline.
Unstretched length of the spring is
\[
1.0\;m
\]
Extension is
\[
0.3\;m
\]
Therefore, distance of the block from the top along the incline is
\[
1.0+0.3=1.3\;m
\]
Step 5: Final conclusion.
Hence, the required distance is
\[
\boxed{1.3\;m}
\]