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Electric Field as Gradient of Electric Potential: Relation between E and V

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Estimated time: 8 minutes
CISCE: Class 12

Introduction

Electric field and electric potential are two ways of describing the same electrostatic situation — one in terms of force per unit charge, the other in terms of energy per unit charge. This topic connects the two using a single elegant mathematical relation.

Analogy: Think of electric potential like the height of a hill and electric field like its slope. The steeper the slope (faster the height drops), the stronger the field. Just as water flows from high to low ground, the electric field points from high to low potential.

CISCE: Class 12

Derivation: Relation Between E and V

Step 1: Consider a small positive test charge q0​ moved a small distance dr against the electric field E.

Step 2: Work done by an external agent against the field: dW = −q0E dr

Step 3: By definition, potential difference is work done per unit charge: dV = \[\frac {dW}{q_0}\]

Step 4: Combining Steps 2 and 3: dV = −E dr

Step 5: Rearranging gives the final relation: E = −\[\frac {dV}{dr}\]

CISCE: Class 12

Unit Consistency Check

1 NC−1 = 1 Vm−1

This confirms that electric field can be expressed either in newtons per coulomb (force-based) or volts per metre (potential-based).

CISCE: Class 12

Special Cases

Case A: Uniform Field Between Parallel Plates

For two plates separated by a distance d with a potential difference V1 − V2​:

E = \[\frac{V_1-V_2}{d}\]

Case B: Field Due to a Point Charge

Starting from the potential due to a point charge:

V = \[\frac {1}{4πε_0}\frac {q}{r}\]

Differentiating with respect to r gives the field:

E = \[\frac {1}{4πε_0}\frac {q}{r^2}\]

Case C: Displacement Parallel vs Perpendicular to Field

Displacement Type Formula Result
Parallel to field (angle θ = 0°) VB − VA = −Ed Maximum potential change
At angle θ to field VB − VA = −Ed cos ⁡θ Partial potential change
Perpendicular to field (θ = 90°) VB − VA = 0 No potential change (VA = VB) — points lie on the same equipotential surface
CISCE: Class 12

Example

A parallel plate capacitor has a potential difference of 50 V across plates 2 mm apart. Find the electric field.

Solution:

E = \[\frac {V}{d}\] = \[\frac {50}{2×10^{−3}}\] = 2.5 × 104 V m−1
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