$2=20\left(1-{e}^{-t / {RC}}\right)$
$\frac{1}{10}=1-{e}^{-t / {RC}}$
${e}^{-t / R C}=\frac{9}{10}$
${e}^{{t} / {RC}}=\frac{10}{9}$
$\frac{{t}}{{RC}}=\ln \left(\frac{10}{9}\right) \Rightarrow {C}=\frac{{t}}{{R} \ell {n}\left(\frac{10}{9}\right)}$
${C}=\frac{10^{-6}}{10 \times .105}=.95\,\mu {F}$

$(A)$ $\frac{E_1}{E_2}=1$ $(B)$ $\frac{E_1}{E_2}=\frac{1}{K}$ $(C)$ $\frac{Q_1}{Q_2}=\frac{3}{K}$ $(D)$ $\frac{ C }{ C _1}=\frac{2+ K }{ K }$

$K(x) = K_0 + \lambda x$ ( $\lambda =$ constant)
The capacitance $C,$ of the capacitor, would be related to its vacuum capacitance $C_0$ for the relation