Two charges $5 \times 10^{-8} \;C$ and $-3 \times 10^{-8}\; C$ are located $16\; cm$ apart. At what point $(s)$ on the line joining the two charges is the electric potential zero? Take the potential at infinity to be zero.

Vedclass pdf generator app on play store
Vedclass iOS app on app store

There are two charges,

$q_{1}=5 \times 10^{-8} \,C$

$q_{2}=-3 \times 10^{-8} \,C$

Distance between the two charges, $d =16 \,cm =0.16 \,m$

Consider a point $P$ on the line joining the two charges, as shown in the given figure.

$r=$ Distance of point $P$ from charge $q_{1}$ Let the electric potential $(V)$ at point $P$ be zero. Potential at point $P$ is the sum of potentials caused by charges $q_{1}$ and $q_{2}$ respectively.

Where, $\therefore V=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{1}}{r}+\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{2}}{(d-r)} \dots(i)$

$\varepsilon_{0}=$ Permittivity of free space For $V =0,$ equation $(i)$ reduces to $0=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{1}}{r}+\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{2}}{(d-r)}$

$\Rightarrow \frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{1}}{r}=-\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{2}}{(d-r)}$

$\Rightarrow \frac{q_{1}}{r}=-\frac{q_{2}}{(d-r)}$

$\Rightarrow \frac{5 \times 10^{-8}}{r}=-\frac{\left(-3 \times 10^{-8}\right)}{(0.16-r)}$

$\Rightarrow 5(0.16-r)=3 r$

$\Rightarrow 0.8=8 r \Rightarrow r=0.1 \,m =10 \,cm$

Therefore, the potential is zero at a distance of $10 \;cm$ from the positive charge between the charges. Suppose point $P$ is outside the system of two charges at a distance s from the negative charge, where potential is zero, as shown in the following figure.

For this arrangement, potential is given by,

Where, $V=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{1}}{s}+\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{2}}{(s-d)} \ldots (ii)$

$\varepsilon_{0}=$ Permittivity of free space For $V=0,$ equation (ii) reduces to $0=\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{1}}{s}+\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{2}}{(s-d)}$

$\Rightarrow \frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{1}}{s}=-\frac{1}{4 \pi \varepsilon_{0}} \cdot \frac{q_{2}}{(s-d)}$

$\Rightarrow \frac{q_{1}}{s}=-\frac{q_{2}}{(s-d)}$

$\Rightarrow \frac{5 \times 10^{-8}}{s}=-\frac{\left(-3 \times 10^{-8}\right)}{(s-0.16)}$

$\Rightarrow 5(s-0.16)=3 \,s$

$\Rightarrow 0.8=2 \,s \Rightarrow s=0.4 \,m =40\, cm$

Therefore, the potential is zero at a distance of $40 \,cm$ from the positive charge outside the system of charges.

898-s11

Similar Questions

Find the potential $V$ of an electrostatic field $\vec E = a\left( {y\hat i + x\hat j} \right)$, where $a$ is a constant.

Charges of $ + \frac{{10}}{3} \times {10^{ - 9}}C$ are placed at each of the four corners of a square of side $8\,cm$. The potential at the intersection of the diagonals is

Charge is uniformly distributed on the surface of a hollow hemisphere. Let $O$ and $A$ be two points on the base of the hemisphere and $V_0$ and $V_A$ be the electric potentials at $O$ and $A$ respectively. Then,

A hollow metallic sphere of radius $10 \;cm$ is charged such that potential of its surface is $80\; V$. The potential at the centre of the sphere would be

  • [AIPMT 1994]

The figure shows a nonconducting ring which has positive and negative charge non uniformly distributed on it such that the total charge is zero. Which of the following statements is true?