A galvanometer is transformed into an ammeter by connecting a shunt resistance \( R_s \) in parallel. This parallel connection enables the ammeter to measure substantial currents without risking damage to the galvanometer. The total current entering the circuit divides between the galvanometer and the shunt, with the galvanometer's portion of the current dictated by its resistance.Applying the formula for parallel resistances yields:\[I = \frac{V}{R_g + R_s},\]Here, \( R_g \) denotes the galvanometer's resistance, and \( R_s \) is the shunt resistance. Consequently, the combined resistance of the ammeter configuration is the sum \( R_g + R_s \).