Two small equal point charges of magnitude q are suspended from a common point O the ceiling by insulating massless strings of equal lengths. They come to equilibrium with each string making angle θ from the vertical. If the mass of each charge is m, then the electrostatic potential at the center of line joining them will be (14πϵ0=K)
In equilibrium, the expressions are given as,
F=Tsinθ (1)
mg=Tcosθ (2)
From above equations, it can be written as,
tanθ=Fmg (3)
The electric force is given as,
F=q24πε0x2
Substitute the value of F in equation (3), we get
tanθ=q24πε0mgx2
x=√q24πε0mgtanθ
x=√kq2mgtanθ
The electric potential is given as,
V=kqx2+kqx2
V=4kqx
V=4√kmgtanθ
Thus, the electric potential at the centre of the line is 4√kmgtanθ.