Potential due to Point Charge

Physics
NEET UG
Version 1Updated 22 Mar 2026

Electric potential at a point in an electric field is defined as the amount of work done by an external agent in bringing a unit positive test charge from infinity to that point without acceleration. It is a scalar quantity and is measured in Joules per Coulomb (J/C), also known as Volts (V). For a single isolated point charge QQ, the electric potential VV at a distance rr from the charge is gi…

Quick Summary

Electric potential due to a point charge is a fundamental concept in electrostatics, defining the 'electric state' of a point in space. It is a scalar quantity, measured in Volts (V), and represents the work done per unit positive test charge to bring it from infinity to that point without acceleration.

For an isolated point charge QQ, the potential VV at a distance rr is given by V=kQrV = \frac{kQ}{r}, where k=14piepsilon0k = \frac{1}{4piepsilon_0}. The sign of QQ is crucial: positive charges create positive potentials, and negative charges create negative potentials.

Unlike the electric field, which is a vector and varies as 1/r21/r^2, potential is a scalar and varies as 1/r1/r. This scalar nature simplifies calculations for multiple charges, as the total potential at a point is simply the algebraic sum of potentials due to individual charges (superposition principle).

Understanding this concept is vital for comprehending electric potential energy, work done in electric fields, and the behavior of charges in various electrostatic setups.

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Key Concepts

Derivation from Work Done

The potential at a point is derived by calculating the work done by an external agent to move a unit positive…

Superposition Principle for Potential

Since potential is a scalar, the total potential at any point due to a system of point charges is the…

Potential Difference and Work Done

The potential difference DeltaV=VBVADelta V = V_B - V_A between two points A and B is the work done per unit positive…

  • Definition:Work done by external agent to bring unit positive charge from infinity to a point.
  • Formula:V=14πϵ0Qr=kQrV = \frac{1}{4\pi\epsilon_0} \frac{Q}{r} = \frac{kQ}{r}
  • Units:Volt (V) or J/C
  • Nature:Scalar quantity (includes sign of Q)
  • Sign:Positive for +Q, Negative for -Q
  • Dependence:V1/rV \propto 1/r
  • Superposition:Vtotal=Vi=kQiriV_{total} = \sum V_i = \sum \frac{kQ_i}{r_i} (algebraic sum)
  • Work Done:Wext=q(VfinalVinitial)W_{ext} = q(V_{final} - V_{initial})
  • Relationship with E:E=dV/drE = -dV/dr (in 1D), r=V/Er = V/E (for point charge)
  • Equipotential Surfaces:Concentric spheres for point charge; W=0W=0 along them.

To remember the potential formula and its properties:

Very Positive Charges Radiate Potential, Negative Charges Attract Negative Potential.

  • Very: Voltage (Potential)
  • Positive Charges: QQ is positive
  • Radiate Potential: VV is positive
  • Negative Charges: QQ is negative
  • Attract Negative Potential: VV is negative

And for the formula: Very Kool Quick Review: V=kQ/rV = kQ/r

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