To transform a galvanometer into an ammeter, a low-resistance component known as a "shunt" is connected in parallel. This shunt resistor redirects the majority of the current, enabling the ammeter to measure significantly larger current values than the galvanometer alone could handle.
Provided Information:
The current passing through the shunt resistor, \(I_s\), is calculated as:
\(I_s = I - I_g\)
Substituting the given values:
\(I_s = 20 \times 10^{-3} - 20 \times 10^{-6} = 19.98 \times 10^{-3} \, A\)
Since the voltage across the galvanometer and the shunt is identical, the following relationship holds:
\(I_g \times R_g = I_s \times R_s\)
Rearranging this equation to determine the shunt resistance, \(R_s\):
\(R_s = \frac{I_g \times R_g}{I_s}\)
Substituting the known values into the equation:
\(R_s = \frac{20 \times 10^{-6} \times 200}{19.98 \times 10^{-3}}\)
The calculated shunt resistance is:
\(R_s = \frac{4 \times 10^{-3}}{19.98 \times 10^{-3}} \approx 0.20 \, \Omega\)
Consequently, a resistance of \(0.20 \, \Omega\) must be added for the galvanometer to function as an ammeter with a range of 0-20 mA.
The determined value is: \(0.20 \, \Omega\).
Assertion (A): The deflection in a galvanometer is directly proportional to the current passing through it.
Reason (R): The coil of a galvanometer is suspended in a uniform radial magnetic field.