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Acceleration of a Charged Particle Between Two Points in an Electric Field

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Estimated time: 7 minutes
CISCE: Class 12

Introduction

When a charged particle is placed in an electric field, it experiences a force that causes it to accelerate. The work done by the field on the particle changes its kinetic energy, allowing us to calculate its final velocity or time taken to travel between two points.

Key Idea: An electric field can do work on a charge and change its speed. A magnetic field, in contrast, only changes the direction of a moving charge — it never changes its speed.

CISCE: Class 12

Derivation

Step 1 - Force on the charge:

F = qE

Step 2 - Acceleration produced:

a = \[\frac {qE}{m}\]

Step 3 - Work done in moving from A to B:

W = q(VA − VB) = qVAB

Step 4 - Work-Energy Theorem (work equals change in kinetic energy):

qVAB = \[\frac {1}{2}\]m(v2 − u2)

Step 5 - If the particle starts from rest (u = 0):

v = \[\sqrt{\frac{2qV_{AB}}{m}}\]

Step 6 - Time taken to travel distance d (starting from rest):

t = \[\sqrt{\frac{2dm}{qE}}\]
CISCE: Class 12

Direction of Motion — Comparison Table

Charge Type Direction of Acceleration Reason
Positive charge Along the electric field \[\vec E\] Force F = qE is in the same direction as E
Negative charge Opposite to the electric field \[\vec E\] Force direction reverses due to the negative sign of q
CISCE: Class 12

Example 1

Given: 1010 electrons accelerated through a potential difference of 2000 V.

Find: Total energy gained.

Solution:

Energy = n × q × V = 1010 × 1.6 × 10−19 × 2000

Answer: 3.2 × 10−6 J = 3.2 µJ

CISCE: Class 12

Example 2

Given: An electron accelerated through a potential difference of 105 V, starting from rest.
Find: Maximum speed attained.
Solution: Using v = \[\sqrt {2qV/m}\]​ with q = 1.6 × 10−19 C, m = 9.1 × 10−31 kg
Answer: v ≈ 1.87 × 108 m/s

CISCE: Class 12

Real-Life Analogy

Think of potential difference like height on a hill. A ball released at the top (higher potential) rolls down to the bottom (lower potential), gaining speed as it goes.
Similarly, a positive charge "rolls down" the potential slope from high potential (A) to low potential (B), gaining kinetic energy along the way.

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