The moving-coil instrument acts as a basic galvanometer with internal resistance $R_g = 5\ \Omega$ and full-scale deflection current $I_g = 1\ \text{mA}$.
A shunt resistor $R_s = 0.55\ \Omega$ is connected in parallel to extend the range.
The maximum current $I$ it can now measure is given by:
\[
I = I_g \left(1 + \frac{R_g}{R_s} \right)
\]
Substituting values:
\[
I = 1\ \text{mA} \left(1 + \frac{5}{0.55} \right) = 1\ \text{mA} \left(1 + 9.09 \right) = 10.09\ \text{mA}
\]
Approximately, the instrument can now measure up to 10 mA.