Two small spheres of each charge $q$, mass $m$ and material density $d$ are suspended from a fixed point…
- $6 \sqrt{3}$
- $2 \sqrt{5}$
- $5 \sqrt{3}$
- $7 \sqrt{2}$
Solution

$ \begin{aligned} F_e & =\frac{k q^2}{r^2} \\ r & =2 l \cos \theta \\ \tan \theta & =\frac{F_e}{m g} \end{aligned} $ [from Fig.] So, for $\theta=45^{\circ}$ and $\phi=45^{\circ}$ $ \begin{aligned} r & =\frac{2 l}{v^2}=\sqrt{2 l} \Rightarrow F_e=\frac{K q^2}{2 l} \\ \tan 45^{\circ} & =\frac{k q^2}{2 l m g} \quad\left(\because \tan 45^{\circ}=1\right) \end{aligned} $

For, $\theta=30^{\circ}$ and $\phi=60^{\circ}$ $ r=2 l \times \frac{1}{2}=l $ So , $F_e^{\prime}=\frac{k q^2}{l^2} \Rightarrow \tan 30^{\circ}=\frac{k^{\prime} q^2}{l^2-m^{\prime} g}$ As, the sphere is suspended in a liquid of density $\frac{2}{3} d$, then the observed weight of the body, $m^{\prime}=V\left(d-\frac{2 d}{3}\right)=\frac{m}{3} \quad[\because m=V \cdot d]$

So, from Eq. (i) and (ii), we get $ \begin{aligned} 3 \sqrt{3} k^{\prime} & =\frac{k}{2} \Rightarrow k^{\prime}=\frac{1}{4 \pi \varepsilon_0 \varepsilon_r}, K=\frac{1}{4 \pi \varepsilon_0} \\ \Rightarrow \quad \varepsilon_r & =6 \sqrt{3} \end{aligned} $
Asked in: AP EAMCET 2019 (21 Apr Shift 1)