(d) For conversion of galvanometer (of resistance) into voltmeter, a resistance $R$ is connected in series
$\therefore i_{g} = \frac{V_{1}}{R + G}$ and $i_{g} = \frac{V_{2}}{2R + G}$
$\Rightarrow \frac{V_{1}}{R + G} = \frac{V_{2}}{2R + G} \Rightarrow \frac{V_{2}}{V_{1}} = \frac{2R + G}{R + G} = \frac{2(R + G) - G}{(R + G)}$
$= 2 - \frac{G}{(R + G)} \Rightarrow V_{2} = 2V_{1} - \frac{V_{1}G}{(R + G)} \Rightarrow V_{2} < 2V_{1}$