Electrostatics
12.0 Electric Potential
12.1 Properties
12.2 Use of Potential
12.3 Potential Due to Point Charge
12.4 Potential due to a Ring
12.5 Potential Due to Uniformly charged Disc
12.6 Potential Due To Uniformly Charged Spherical Shell
12.7 Potential Due to Uniformly Charged Solid Sphere
12.0 Electric Potential
12.2 Use of Potential
12.3 Potential Due to Point Charge
12.4 Potential due to a Ring
12.5 Potential Due to Uniformly charged Disc
12.6 Potential Due To Uniformly Charged Spherical Shell
12.7 Potential Due to Uniformly Charged Solid Sphere
In electrostatics field, the electric potential (due to some source charges) at a point $P$ is defined as the work done by external agent in taking a unit point positive charge from a reference charge point (generally taken at infinity) to that point $P$ without changing its kinetic energy..
Mathematical representation :
If ${{{\left( {{W_{\infty \; \to P}}} \right)}_{ext}}}$ is the work required in moving a point charge $q$ from infinity to a point $P,$ the electric potential of the point $P$ is $${\left. {{V_P}\frac{{{{\left( {{W_{\infty \; \to P}}} \right)}_{ext}}}}{q}} \right]_{\Delta K = 0}} = \frac{{{{\left( { - {W_{elc}}} \right)}_{\infty \; \to P}}}}{q}$$ Note:
(I) ${{{\left( {{W_{\infty \; \to P}}} \right)}_{ext}}}$ can also be called as the work done by external agent against the electric force on a unit positive charge due to the source charge.
(II) Write both $W$ and $q$ with proper sign.