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Atom as a Magnetic Dipole

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Estimated time: 7 minutes
CISCE: Class 12

Introduction

An electron revolving around the nucleus in an atom is not just executing circular motion — it also constitutes a tiny current loop. Since a current loop produces a magnetic field, the orbiting electron behaves like a microscopic magnetic dipole.

Analogy: Think of the electron's orbit as a small circular wire loop carrying current — similar to a coil in an electromagnet. Just as current in a coil creates a magnetic field, the electron's motion creates a magnetic moment.

CISCE: Class 12

Key Terms

Term Symbol Meaning
Magnetic Dipole Moment μ Product of current and loop area; measure of a current loop's magnetic strength
Angular Momentum L Product of mass, velocity, and radius of orbiting particle
Gyromagnetic Ratio e/2me Ratio of magnetic moment to angular momentum of an electron
Bohr Magneton μB Smallest unit of magnetic moment for an electron in the ground state
CISCE: Class 12

Derivation

Step 1: Current due to an orbiting electron

An electron completing one revolution in a time period T constitutes current: I = \[\frac {e}{T}\]

Step 2: Magnetic moment of current loop

For any current loop, magnetic moment = current × area: μ = IA = I(πr2)

Step 3: Express in terms of velocity

Since T = \[\frac {2πr}{v}\], substituting gives: \[{\mu = \frac{evr}{2}}\]   ...(Equation 1)

Step 4: Relate to angular momentum

Angular momentum of electron: L = mevr

Dividing Equation (1) by L:

\[{\mu = \left(\frac{e}{2m_e}\right)L}\]   ...(Equation 2)

Important Point: The term \[\frac {e}{2m_e}\]​ is called the gyromagnetic ratio — a constant for all electrons.

Step 5: Apply Bohr's Quantisation Condition

Bohr postulated: L = \[\frac {nh}{2π}\]​, where n = 1, 2, 3...

Substituting into Equation (2): \[{\mu = n\mu_B}\]   ...(Equation 3)

where: \[\mu_B = \frac{eh}{4\pi m_e} = 9.27 \times 10^{-24}\ \text{A·m}^2\]

CISCE: Class 12

Comparison Table: Types of Magnetic Moment

Type Origin Formula Remarks
Orbital Magnetic Moment Electron's orbital motion μ = n·μB Quantised; depends on orbit number n
Spin Magnetic Moment Electron's intrinsic spin μs = (eh)/(4πme) Present even without orbital motion
Bohr Magneton Fundamental unit μB = eh/4πme Constant = 9.27 × 10-24 A·m2
CISCE: Class 12

Example

Problem: Two electrons revolve in circular orbits of radii 5.3 × 10−11 m and 2.1 × 10−10 m in opposite directions, each with speed 2.2 × 106 m/s. Find the net magnetic moment.

Given:

  • r1 = 5.3 × 10−11 m, r2 = 2.1 × 10−10 m
  • v = 2.2 × 106 m/s (same for both)
  • Directions: opposite

Formula Used: μ = \[\frac {evr}{2}\]

Step 1 - Moment of electron 1: \[\mu_1 = \frac{(1.6\times10^{-19})(2.2\times10^6)(5.3\times10^{-11})}{2} = 9.32 \times 10^{-24}\ \text{A·m}^2\]

Step 2 - Moment of electron 2: \[\mu_2 = \frac{(1.6\times10^{-19})(2.2\times10^6)(2.1\times10^{-10})}{2} = 3.696 \times 10^{-23}\ \text{A·m}^2\]

Step 3 - Net moment (opposite directions → subtract):

\[\mu_{net} = \mu_2 - \mu_1 = 2.764 \times 10^{-23}\ \text{A·m}^2\]

Answer: Net magnetic moment = 2.764 × 10−23 A·m2

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