Q157 / 200 · MHT CET - Medical 2026 (26 April Shift 1) · Physics
A galvanometer can be converted into a voltmeter of certain range by connecting a resistance of $990\ \Omega$ in series with it. When the resistance of $480\ \Omega$ is connected in series, the range is halved. The resistance of the galvanometer is
- A$20\ \Omega$
- Correct answerB$30\ \Omega$
- C$40\ \Omega$
- D$50\ \Omega$
Solution
Let the resistance of the galvanometer be $G$ and the full-scale deflection current be $I_g$.
When a resistance of $990\ \Omega$ is connected in series, the range of the voltmeter is $V$.
$V = I_g (G + 990)$
When a resistance of $480\ \Omega$ is connected in series, the range is halved, i.e., $\dfrac{V}{2}$.
$\dfrac{V}{2} = I_g (G + 480)$
Dividing the first equation by the second equation:
$\dfrac{V}{\dfrac{V}{2}} = \dfrac{I_g (G + 990)}{I_g (G + 480)}$
$2 = \dfrac{G + 990}{G + 480}$
$2(G + 480) = G + 990$
$2G + 960 = G + 990$
$G = 30\ \Omega$
Answer: $30\ \Omega$
When a resistance of $990\ \Omega$ is connected in series, the range of the voltmeter is $V$.
$V = I_g (G + 990)$
When a resistance of $480\ \Omega$ is connected in series, the range is halved, i.e., $\dfrac{V}{2}$.
$\dfrac{V}{2} = I_g (G + 480)$
Dividing the first equation by the second equation:
$\dfrac{V}{\dfrac{V}{2}} = \dfrac{I_g (G + 990)}{I_g (G + 480)}$
$2 = \dfrac{G + 990}{G + 480}$
$2(G + 480) = G + 990$
$2G + 960 = G + 990$
$G = 30\ \Omega$
Answer: $30\ \Omega$
Hence, the correct answer is option: 'B'.