Concept:
A galvanometer can be converted into an ammeter by connecting a low resistance called a shunt in parallel with the galvanometer. The shunt allows most of the current to bypass the galvanometer so that only a small fraction of the total current flows through it.
If
\(G\) = resistance of the galvanometer,
\(S\) = shunt resistance,
\(I_g\) = current through the galvanometer,
\(I\) = total current.
Since the galvanometer and shunt are connected in parallel, the potential difference across them is the same.
\[
I_g G = I_s S
\]
where \(I_s\) is the current through the shunt.
Step 1: Express galvanometer current as a fraction of total current.
\[
I_g = 8\% \, \text{of} \, I
\]
\[
I_g = 0.08I
\]
Step 2: Determine the current through the shunt.
\[
I_s = I - I_g
\]
\[
I_s = I - 0.08I
\]
\[
I_s = 0.92I
\]
Step 3: Use the parallel branch relation.
\[
I_g G = I_s S
\]
Substitute the values:
\[
0.08I \cdot G = 0.92I \cdot S
\]
Step 4: Solve for shunt resistance.
Cancel \(I\) from both sides:
\[
0.08G = 0.92S
\]
\[
S = \frac{0.08}{0.92}G
\]
\[
S = \frac{8}{92}G
\]
\[
S = \frac{2G}{23}
\]
Step 5: Final result.
\[
\boxed{S = \frac{2G}{23}}
\]