Concept:
At neutral point:
\[
B_{\text{magnet}} = B_H
\]
For axial line:
\[
B = \frac{\mu_0}{4\pi}\frac{2M}{r^3}
\]
Step 1: Equate fields
\[
\frac{\mu_0}{4\pi}\frac{2M}{r^3} = B_H
\]
Step 2: Substitute values
\[
\frac{10^{-7}\cdot 2M}{(0.2)^3} = 0.3\times10^{-4}
\]
\[
\frac{2\times10^{-7}M}{8\times10^{-3}} = 0.3\times10^{-4}
\]
\[
\frac{2M}{8}\times10^{-4} = 0.3\times10^{-4}
\]
\[
\frac{M}{4} = 0.3
\Rightarrow M = 1.2\,A\,m^2
\]
Step 3: Convert units
\[
1\,A\,m^2 = 10^3\,\text{ab-amp}\times\text{cm}^2
\]
\[
M = 1.2\times10^3 = 1200\,\text{ab-amp}\times\text{cm}^2
\]
Conclusion:
\[
1200\,\text{ab-amp}\times\text{cm}^2
\]