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

Two identical positive charges are placed at $x =\, -a$ and $x = a$ . The correct variation of potential $V$ along the $x-$ axis is given by

Consider two points $1$ and $2$ in a region outside a charged sphere. Two points are not very far away from the sphere. If $E$ and $V$ represent the electric field vector and the electric potential, which of the following is not possible

Two insulated charged conducting spheres of radii $20\,cm$ and $15\,cm$ respectively and having an equal charge of $10\,C$ are connected by a copper wire and then they are separated. Then

A conducting sphere of radius $R$ is given a charge $Q.$ The electric potential and the electric field at the centre of the sphere respectively are

  • [AIPMT 2014]

The electric potential at the centre of two concentric half rings of radii $R_1$ and $R_2$, having same linear charge density $\lambda$ is

  • [JEE MAIN 2023]