Step 1: Understand the given condition for null points.
The bar magnet is placed along the north-south direction.
The angle of dip is
\[
0^\circ
\]
So the earth's magnetic field is horizontal and is denoted by
\[
B
\]
Null points are found on the axial line of the magnet at a distance
\[
r=20\ \text{cm}
\]
At a null point, the magnetic field due to the magnet is equal in magnitude and opposite in direction to the earth's magnetic field.
Therefore, on the axial line,
\[
B_{\text{axial}}=B
\]
Step 2: Use the relation between axial and equatorial magnetic fields.
For a short bar magnet, the magnetic field on the axial line is
\[
B_{\text{axial}}=\frac{\mu_0}{4\pi}\frac{2M}{r^3}
\]
The magnetic field on the equatorial line or normal bisector is
\[
B_{\text{equatorial}}=\frac{\mu_0}{4\pi}\frac{M}{r^3}
\]
Hence,
\[
B_{\text{axial}}=2B_{\text{equatorial}}
\]
Therefore,
\[
B_{\text{equatorial}}=\frac{B_{\text{axial}}}{2}
\]
Since
\[
B_{\text{axial}}=B
\]
we get
\[
B_{\text{equatorial}}=\frac{B}{2}
\]
Step 3: Find the total magnetic field on the normal bisector.
On the normal bisector, the field due to the magnet is opposite to the magnetic moment direction.
The earth's magnetic field and the magnetic field due to the magnet act in the same line, so the resultant field is
\[
B_{\text{total}}=B+B_{\text{equatorial}}
\]
Substituting
\[
B_{\text{equatorial}}=\frac{B}{2}
\]
we get
\[
B_{\text{total}}=B+\frac{B}{2}
\]
\[
B_{\text{total}}=\frac{3B}{2}
\]
Given,
\[
B_{\text{total}}=0.6\ \text{G}
\]
Thus,
\[
\frac{3B}{2}=0.6
\]
Step 4: Calculate the value of \(B\).
\[
B=0.6\times\frac{2}{3}
\]
\[
B=0.4\ \text{G}
\]
Step 5: Final conclusion.
Therefore, the magnitude of earth's magnetic field is
\[
\boxed{0.4\ \text{G}}
\]