Electric Potential

Q: What is the difference between electric potential and electric potential energy?

Electric potential ($V$) is a property of the electric field itself at a given point in space, defined as the potential energy per unit positive test charge ($V = U/q_0$). It tells us how much potential energy a unit charge would have if placed at that point. Electric potential energy ($U$), on the other hand, is the actual energy stored in a specific charge ($q$) when it is placed at a point with potential $V$, given by $U = qV$. So, potential is a characteristic of the location, while potential energy is a characteristic of a specific charge at that location.

Updated 22 Mar 2026

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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), which is also known as Volt (V). The concept of electric potential is fundamental to understanding the energy associated with elect…

Quick Summary

Electric potential ( $V$ ) is a scalar quantity representing the work done per unit positive test charge to bring it from infinity to a specific point in an electric field, without acceleration. Its unit is the Volt (V), where $1\,\text{V} = 1\,\text{J/C}$ .

The potential due to a point charge $Q$ at a distance $r$ is $V = \frac{1}{4\pi\epsilon_0} \frac{Q}{r}$ . For a system of charges, the total potential is the algebraic sum of individual potentials. Electric potential difference ( $\Delta V$ ) between two points A and B is the work done by an external agent per unit charge to move it from A to B.

Equipotential surfaces are regions where the potential is constant, and electric field lines are always perpendicular to them. The electric field $\vec{E}$ is the negative gradient of the potential, $\vec{E} = -\nabla V$ .

Electric potential energy ( $U$ ) of a charge $q$ at a potential $V$ is $U = qV$ . For a system of two charges $q_1, q_2$ separated by $r$ , $U = \frac{1}{4\pi\epsilon_0} \frac{q_1 q_2}{r}$ . A dipole $\vec{p}$ in an external field $\vec{E}$ has potential energy $U = -\vec{p} \cdot \vec{E}$ .

Full explanation

Conceptual Foundation of Electric Potential

Electric potential, often denoted by $V$ , is a scalar quantity that describes the potential energy per unit charge at a given location in an electric field. It's a fundamental concept in electrostatics, providing a more convenient way to analyze electric fields and the energy associated with charge configurations than directly using the electric field vector $\vec{E}$ .

The concept arises from the conservative nature of the electrostatic force. Just like gravity, the work done by the electrostatic force in moving a charge between two points is independent of the path taken. This allows us to define a potential energy function, and subsequently, an electric potential.

Potential Difference: More practically, we often talk about electric potential difference, $\Delta V$ , between two points A and B. It is defined as the work done by an external agent in moving a unit positive test charge from point A to point B without acceleration.

V_B - V_A = \frac{W_{ext}(A \to B)}{q_0}

If point A is taken at infinity (

V_A = 0

), then the potential at point B is simply the work done in bringing the unit positive charge from infinity to B.

Key Principles and Laws

Work-Energy Theorem and Potential: — The work done by the electric field in moving a charge

q_0

from A to B is

W_{AB} = -\Delta U = -(U_B - U_A)

. Since

V = U/q_0

, we have

W_{AB} = -q_0(V_B - V_A) = q_0(V_A - V_B)

. Conversely, the work done by an external agent is

W_{ext} = q_0(V_B - V_A)

Electric Potential due to a Point Charge: — Consider a point charge

Q

at the origin. To find the potential at a distance

r

from

Q

, we calculate the work done in bringing a unit positive test charge from infinity to

r

. The electric field due to

Q

E = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2}

. The potential

V(r)

is given by:

V(r) = -\int_{\infty}^{r} \vec{E} \cdot d\vec{l} = -\int_{\infty}^{r} \frac{1}{4\pi\epsilon_0} \frac{Q}{r'^2} dr'

V(r) = \frac{1}{4\pi\epsilon_0} \frac{Q}{r}

This formula shows that potential decreases with distance from a positive charge and increases with distance from a negative charge (becomes less negative). For

Q>0

V>0

. For

Q<0

V<0

Electric Potential due to a System of Point Charges: — Due to the superposition principle, the total electric potential at any point due to a system of point charges is the algebraic sum of the potentials due to individual charges at that point.

V = \sum_{i=1}^{n} V_i = \sum_{i=1}^{n} \frac{1}{4\pi\epsilon_0} \frac{Q_i}{r_i}

Here,

r_i

is the distance of the point from the

i

-th charge

Q_i

. Remember, potential is a scalar, so we just add them algebraically, paying attention to the sign of each charge.

Electric Potential due to an Electric Dipole: — An electric dipole consists of two equal and opposite charges,

+q

and

-q

, separated by a small distance

2a

. The dipole moment is

\vec{p} = q(2\vec{a})

The potential at a point $(r, \theta)$ (in spherical coordinates, with the dipole along the z-axis) is approximately:

V(r, \theta) = \frac{1}{4\pi\epsilon_0} \frac{p \cos\theta}{r^2}

where

r

is the distance from the center of the dipole and

\theta

is the angle between the position vector

\vec{r}

and the dipole moment

\vec{p}

* Along the axial line (where $\theta = 0^{\circ}$ or $180^{\circ}$ ), $V = \pm \frac{1}{4\pi\epsilon_0} \frac{p}{r^2}$ . * Along the equatorial line (where $\theta = 90^{\circ}$ ), $V = 0$ . This is a very important result: the potential is zero everywhere on the equatorial plane of a dipole.

Equipotential Surfaces: — These are surfaces in an electric field where all points on the surface have the same electric potential. No work is done in moving a test charge along an equipotential surface. This implies that the electric field lines are always perpendicular to equipotential surfaces. For a point charge, equipotential surfaces are concentric spheres. For a uniform electric field, they are planes perpendicular to the field lines.

Relation between Electric Field and Electric Potential: — The electric field is the negative gradient of the electric potential.

\vec{E} = -\nabla V

In one dimension,

E_x = -\frac{dV}{dx}

. In three dimensions, this expands to:

E_x = -\frac{\partial V}{\partial x}, \quad E_y = -\frac{\partial V}{\partial y}, \quad E_z = -\frac{\partial V}{\partial z}

This relationship is crucial as it allows us to calculate the electric field from a known potential function, which is often simpler than direct vector summation.

Electric Potential Energy

Electric potential energy ( $U$ ) is the energy stored in a system of charges due to their relative positions in an electric field. It's the work done by an external agent to assemble the charges from infinity to their current configuration.

Potential Energy of a Single Charge in an External Field: — If a charge

q

is placed at a point where the external potential is

V

, its potential energy is

U = qV

. This is the work done to bring

q

from infinity to that point.

Potential Energy of a System of Two Point Charges: — To bring

q_1

from infinity to a point, no work is done initially as there's no field. Then, to bring

q_2

from infinity to a distance

r_{12}

from

q_1

, the work done is

q_2 V_1

, where

V_1 = \frac{1}{4\pi\epsilon_0} \frac{q_1}{r_{12}}

is the potential due to

q_1

at the location of

q_2

. So, the potential energy of the system is:

U = \frac{1}{4\pi\epsilon_0} \frac{q_1 q_2}{r_{12}}

Potential Energy of a System of Multiple Point Charges: — For a system of

n

charges, the total potential energy is the sum of the potential energies for every unique pair of charges:

U = \sum_{i<j} \frac{1}{4\pi\epsilon_0} \frac{q_i q_j}{r_{ij}}

This sum ensures each pair is counted only once.

Potential Energy of a Dipole in an External Electric Field: — When an electric dipole with dipole moment

\vec{p}

is placed in a uniform external electric field

\vec{E}

, it experiences a torque

\vec{\tau} = \vec{p} \times \vec{E}

. The potential energy of the dipole in this field is:

U = -\vec{p} \cdot \vec{E} = -pE \cos\theta

where

\theta

is the angle between

\vec{p}

and

\vec{E}

. The potential energy is minimum (most stable) when

\theta = 0^{\circ}

(dipole aligned with the field) and maximum (least stable) when

\theta = 180^{\circ}

(dipole anti-aligned).

Real-World Applications

Capacitors: — These devices store electric potential energy in an electric field between two conducting plates. The potential difference across the plates is directly related to the stored charge and capacitance.

Batteries: — Batteries create and maintain a potential difference, driving current through circuits. The 'voltage' of a battery is its potential difference.

Particle Accelerators: — High potential differences are used to accelerate charged particles (like electrons or protons) to very high speeds, imparting significant kinetic energy.

Electrostatic Precipitators: — Used to remove particulate matter from industrial exhaust gases. High potential differences create strong electric fields that ionize gas molecules, which then charge the particles, allowing them to be collected on oppositely charged plates.

Nerve Impulses: — The transmission of nerve signals in biological systems involves changes in electric potential across nerve cell membranes.

Common Misconceptions

Potential vs. Potential Energy: — Students often confuse electric potential (

V

) with electric potential energy (

U

). Potential is potential energy per unit charge (

V = U/q

). It's a property of the field at a point, independent of the charge placed there. Potential energy, however, depends on both the potential and the specific charge placed at that point.

Zero Electric Field implies Zero Potential (and vice-versa): — Not necessarily. For example, inside a charged conducting sphere, the electric field is zero, but the potential is constant and non-zero (equal to the potential on its surface). Conversely, at the equatorial plane of an electric dipole, the potential is zero, but the electric field is non-zero.

Potential is a Vector: — Potential is a scalar. Its calculation involves algebraic summation, not vector addition.

Reference Point for Potential: — Potential is always relative. While we often take infinity as the zero potential reference, any point can be chosen. However, potential difference is absolute.

NEET-Specific Angle

For NEET, understanding the definitions, formulas for point charges, systems of charges, and dipoles is paramount. Questions frequently involve calculating potential at specific points, determining work done, or relating potential to electric field.

The concept of equipotential surfaces and their properties (e.g., perpendicularity to E-field lines, no work done) is also a recurring theme. Pay close attention to the signs of charges and the scalar nature of potential.

Problems involving potential energy of charge configurations or dipoles in external fields are also common. Mastering the relationship $\vec{E} = -\nabla V$ is essential for both conceptual and numerical problems.

Key Concepts

Potential due to a System of Point Charges

When multiple point charges are present, the electric potential at any point in space is simply the algebraic…

Relation between Electric Field and Electric Potential

The electric field $\vec{E}$ and electric potential $V$ are intimately linked. The electric field is the…

Electric Potential Energy of a Dipole in an External Electric Field

When an electric dipole with dipole moment $\vec{p}$ is placed in a uniform external electric field…

Often confused with

Side-by-side differences the NEET paper likes to test.

Electric Potential vs Electric Potential Energy

Aspect	Electric Potential	Electric Potential Energy
Definition	Electric Potential (V): Work done per unit positive test charge to bring it from infinity to a point.	Electric Potential Energy (U): Work done to bring a specific charge from infinity to a point in an electric field, or to assemble a system of charges.
Unit	Volt (V) or Joules per Coulomb (J/C)	Joule (J)
Nature	Scalar quantity	Scalar quantity
Dependency	Property of the electric field at a point, independent of the charge placed there.	Depends on the magnitude of the charge and the electric potential at its location ($U=qV$). Also depends on the configuration of charges in a system.
Analogy	Gravitational potential (height) at a point.	Gravitational potential energy (mgh) of an object at that height.

Electric potential is a fundamental characteristic of an electric field at a specific location, representing the potential energy that a unit positive charge would possess if placed there. It's a 'per unit charge' concept.

Electric potential energy, on the other hand, is the actual energy stored within a specific charge or a system of charges due to their positions within an electric field. While both are scalar quantities, potential is independent of the test charge, whereas potential energy directly depends on the magnitude of the charge involved.

Understanding this distinction is crucial for solving problems in electrostatics.

Why it is tested: For NEET, distinguishing between electric potential and electric potential energy is a common source of conceptual questions. Students must clearly understand their definitions, units, and how they relate ($U=qV$). Misconceptions often arise when applying these concepts to work-energy problems, making this a high-yield area for testing fundamental understanding.

Questions students ask

6 answered on this topic.

What is the difference between electric potential and electric potential energy?

Electric potential ( $V$ ) is a property of the electric field itself at a given point in space, defined as the potential energy per unit positive test charge ( $V = U/q_0$ ). It tells us how much potential energy a unit charge would have if placed at that point.

Electric potential energy ( $U$ ), on the other hand, is the actual energy stored in a specific charge ( $q$ ) when it is placed at a point with potential $V$ , given by $U = qV$ . So, potential is a characteristic of the location, while potential energy is a characteristic of a specific charge at that location.

Why is electric potential a scalar quantity while electric field is a vector quantity?

Electric potential is defined based on the work done to move a charge, and work is a scalar quantity (it only has magnitude, not direction). Therefore, electric potential, being work done per unit charge, is also a scalar.

In contrast, the electric field is defined as the force experienced by a unit positive test charge, and force is a vector quantity (having both magnitude and direction). Hence, the electric field is a vector.

This scalar nature of potential often simplifies calculations significantly.

Can electric potential be negative? What does a negative potential signify?

Yes, electric potential can be negative. A negative potential at a point means that an external agent would have to do negative work (or the electric field would do positive work) to bring a unit positive test charge from infinity to that point.

This typically occurs in the vicinity of negative source charges. For instance, near a single negative point charge, the potential is negative. It implies that a positive test charge would be attracted to the source charge, and thus, its potential energy would decrease as it approaches.

What are equipotential surfaces? Give an example.

Equipotential surfaces are imaginary surfaces in an electric field where all points on the surface have the same electric potential. No work is done by the electric field when a charge moves from one point to another on the same equipotential surface.

A key property is that electric field lines are always perpendicular to equipotential surfaces. For example, for an isolated positive point charge, the equipotential surfaces are concentric spheres centered on the charge.

For a uniform electric field, the equipotential surfaces are planes perpendicular to the direction of the field lines.

Is it possible for the electric field to be zero at a point where the electric potential is non-zero, or vice-versa?

Yes, both scenarios are possible. Consider the interior of a charged conducting sphere: the electric field is zero everywhere inside, but the electric potential is constant and equal to the potential on its surface (which is non-zero).

Conversely, consider the equatorial plane of an electric dipole: the electric potential is zero at all points on this plane, but the electric field is definitely non-zero and points perpendicular to the dipole axis.

This highlights that E and V are related but not directly proportional in a simple way.

How is electric potential related to the electric field?

The electric field (a vector) is related to the electric potential (a scalar) through a mathematical operation called the negative gradient. Specifically, $\vec{E} = -\nabla V$ . In simpler terms, the electric field points in the direction of the steepest decrease in electric potential.

The magnitude of the electric field is the rate of change of potential with respect to distance. This relationship is crucial because it allows us to derive the electric field from the potential, which is often easier to calculate due to its scalar nature.

Revise in 30 seconds

Electric Potential (V): — Work done per unit charge from infinity to a point. Scalar quantity. Unit: Volt (V) or J/C.

Potential due to Point Charge: —

V = \frac{1}{4\pi\epsilon_0} \frac{Q}{r} = \frac{kQ}{r}

Potential due to System of Charges: —

V_{total} = \sum V_i = \sum \frac{kQ_i}{r_i}

(algebraic sum).

Potential Difference: —

\Delta V = V_B - V_A = \frac{W_{ext}}{q_0}

Work Done: —

W = q(V_B - V_A)

Electric Potential Energy (U): — Energy of a charge

q

at potential

V

U = qV

. Unit: Joule (J).

Potential Energy of Two Charges: —

U = \frac{1}{4\pi\epsilon_0} \frac{q_1 q_2}{r_{12}} = \frac{kq_1q_2}{r_{12}}

Potential Energy of Dipole in E-field: —

U = -\vec{p} \cdot \vec{E} = -pE \cos\theta

Relation between E and V: —

\vec{E} = -\nabla V

(or

E_x = -\frac{dV}{dx}

in 1D).

Equipotential Surfaces: — Surfaces of constant potential. Electric field lines are perpendicular to them. No work done along them.

To remember the relationship between Electric Field and Potential: Electric field Decreases Voltage. Think of 'EDV' as 'Electric Drives Voltage'. The negative sign implies the field points in the direction of decreasing potential.