$\Rightarrow\text{i}=\frac{3\times10^{-3}}{1.12\times10^{-6}\times180}$
$=\frac{1}{6.72}\times10^2\approx15\text{Amp}$

$\text{V}=\in+\text{ir}$
$\Rightarrow7.2=6+2\times\text{r}$
$\Rightarrow1.2=2\text{r}\Rightarrow\text{r}=0.6\Omega.$

$\text{W}=\text{Zit}$
$2.68=\frac{107.9}{96500}\times\text{i}\times10\times60$
$\Rightarrow\text{l}=\frac{2.68\times965}{107.9\times6}=3.99\approx4\text{Amp}$
Heat developed in the $20\Omega$ resister$=(4)^2\times20\times10\times60=192000\text{J}=192\text{KJ}$
Full deflection current $=10\text{mA}=(10\times10^{-3})\text{A}$
$\text{R}_\text{eff}=(575+25)\Omega=600\Omega$
$\text{V}=\text{R}_\text{eff}\times\text{i}=600\times10\times10^{-3}=6\text{V}.$

$\text{C}_\text{eff}=\frac{\text{C}_1\text{C}_2}{\text{C}_1+\text{C}_2}$
$\text{Q}=\text{C}_\text{eff}\text{E}\Big(1-\text{e}^{\frac{-\text{t}}{\text{RC}}}\Big)=\frac{\text{C}_1\text{C}_2}{\text{C}_1+\text{C}_2}\text{E}\Big(1-\text{e}^\frac{-\text{t}}{\text{RC}}\Big)$

$\text{R}_\text{eq}=(10+20)\Omega=30\Omega$
$\text{R}_\text{eq}=10\Omega$
$\text{i}=\Big(\frac{3}{10}\Big)\Omega=0.3\Omega.$

Eq. Resistance $=\frac{\text{r}}{3}$

$\text{q}=\text{q}_0\Big(1-\text{e}^{\frac{-\text{t}}{\text{RC}}}\Big)$
$=25(2+2)\times10^{-6}\bigg(1-\text{e}^\frac{-0.2\times10^{-3}}{25\times4\times10^{-6}}\bigg)$
$=24\times10^{-6}(1-\text{e}^2)=20.75$
Charge on each capacitor $=\frac{20.75}{2}=10.3$
$9-6=3\text{V}$
Current $=\frac{3}{10}=0.3\text{A}$
Internal resistance $'\text{r}'=1\Omega$
Current $=\frac{3}{1}=3\text{A}$

For an value of R, the current in the branch is 0.