The current sensitivity of the galvanometer is given as \( 10 \mu A/\text{div} \) and it has 20 divisions, so the full-scale deflection current is:
\[
I_{\text{full scale}} = 10 \, \mu A \times 20 = 200 \, \mu A
\]
Next, to convert the galvanometer into a voltmeter, we need to find the resistance needed to allow the galvanometer to measure up to 1V. According to Ohm's law:
\[
V = I \times R
\]
Where \( V = 1 \, \text{V} \) and \( I = 200 \, \mu A = 200 \times 10^{-6} \, \text{A} \). Thus:
\[
R_{\text{total}} = \frac{V}{I} = \frac{1 \, \text{V}}{200 \times 10^{-6} \, \text{A}} = 5000 \, \Omega
\]
The resistance of the galvanometer is already \( 100 \, \Omega \), so the additional resistance \( R \) required in series is:
\[
R = R_{\text{total}} - R_{\text{galv}} = 5000 \, \Omega - 100 \, \Omega = 4900 \, \Omega
\]
Thus, the resistance required is \( 49000 \, \Omega \) in series with the galvanometer to convert it into a voltmeter reading up to 1 V.