Physics > Electrostatics > 12.0 Electric Potential

  Electrostatics
    1.0 Introduction
    2.0 Electric charge
    3.0 Coulomb's law
    4.0 Principle of superposition
    5.0 Continuous charge distribution
    6.0 Electric field
    7.0 Electric field lines
    8.0 Insulators and conductors
    9.0 Gauss's law
    10.0 Work done
    11.0 Electric potential energy
    12.0 Electric Potential
    13.0 Electric dipole

12.4 Potential due to a Ring

(i) Potential at the centre of uniformaly charged ring:

Potential due to a small element $dq$ $$dV = \frac{{Kdq}}{R}$$

$\therefore $ Net potential: $V = \int {\frac{{K\;dq}}{R}} $

$\therefore \;V = \frac{K}{R}\;\int {dq = \frac{{Kq}}{R}} $



(ii) For non uniformaly charged ring potential at the center is: $$V = \frac{{K{q_{total}}}}{R}$$



(iii) Potential due to half ring at center is: $$V = \frac{{Kq}}{R}$$



(iv) Potential at the axis of a ring:

Calculation of potential at a point on the axis which is a distance $X$ from center of uniformly charged $($ total charge $Q)$ ring of radius $R.$


consider an element of charge $dq$ on the ring.

Potential at point $P$ due to charge $dq$ will be $$dV = \frac{{K\left( {dq} \right)}}{{\sqrt {{R^2} + {X^2}} }}$$

$\therefore $ Net potential at point $P$ due to all such element will be: $$V = \int {dV} = \frac{{KQ}}{{\sqrt {{R^2} + {X^2}} }}$$


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