To convert a galvanometer into an ammeter, a shunt resistance \( R_s \) is placed in parallel with the galvanometer. This allows the ammeter to measure large currents without damaging the galvanometer. The total current through the circuit is shared between the galvanometer and the shunt, with the galvanometer current determined by its resistance.
Using the relation for parallel resistances:
\[
I = \frac{V}{R_g + R_s},
\]
where \( R_g \) is the resistance of the galvanometer, and \( R_s \) is the shunt resistance. Thus, the total resistance of the system is the sum \( R_g + R_s \).