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Force and Field Due to Bar Magnet

NEET > Physics > Magnetic Effects of Current and Magnetism > Magnetism > Force and Field Due to Bar Magnet

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Overview content

Topic 4 of 6 • Chapter: Magnetism • Physics

Force and Field Due to Bar Magnet – Complete Notes, Revision, Important Questions & Downloads

Force and Field Due to Bar Magnet is the calculation-heavy dipole block of Magnetism, where the student must distinguish axial, equatorial, and general positions and then connect those field expressions to torque, work, and potential energy of a bar magnet placed in a uniform field. NEET usually tests this topic through direct MCQs on the short-magnet results Ba = (mu0/4pi)(2M/r^3) and Be = (mu0/4pi)(M/r^3), the 2:1 axial-to-equatorial field ratio at equal distance, and the stability logic that follows from U = -MB cos theta. The trap is geometric as well as conceptual: the factor 2 belongs only to the axial line, and zero torque does not by itself mean stable equilibrium because anti-parallel orientation has maximum potential energy.

⬇ Download Notes PDFView Important Questions →
Bar Magnet FieldFormula DenseNEET Core
Expected QuestionsQ
1
question from axial versus equatorial field, or torque and energy of a dipole in uniform field
Time Required⏱
3 Hours
to separate the field formulas by geometry and lock the dipole-in-field relations without sign confusion
Difficulty⚡
Medium
the ideas are standard, but the formulas look similar enough to invite axial-equatorial swaps
NRI USA Curriculum GapUS
Moderate
many curricula stop at qualitative dipole language, while NEET expects quick use of position-specific field formulas and energy relations
0Subtopics
30+Practice Questions
4Free Downloads
3 hrsPrep Time
⬇ Get Free Downloads

NEET Weightage & Exam Pattern

Magnetism
NEET YearQuestions from this TopicBarMarks
20241
 
1 Q
4
20231
 
1 Q
4
20221
 
1 Q
4
20211
 
1 Q
4
20201
 
1 Q
4
Topic Weightage5 20
Axial and equatorial field formulas are among the most directly testable relations in the magnetism chapter because only the geometry changes while the notation stays almost the same.
Torque, work, and potential energy of a magnetic dipole in uniform field are often paired with orientation words such as stable, unstable, parallel, or anti-parallel.

Questions on short magnets usually reduce the exact expressions to the r much greater than l limit, so the student must notice when the inverse-cube approximation is intended.
📊
0.8
Avg Questions / Year
🎯
20
Total Marks (6 yrs)
📈
Direct
Pattern
⚠️
Medium
Difficulty

Preparation Strategy

1

Separate Axial from Equatorial Before Writing the Formula Read the position first, then write the field expression. Axial position carries the factor 2, while equatorial position does not. Most losses here happen because students remember M and r^3 correctly but place the wrong geometry factor on top.

2

Recognise the Short-Magnet Approximation If the question implies r is much larger than the magnetic length, use the inverse-cube forms directly. This saves algebra and also signals that the problem is testing dipole behavior rather than exact finite-length correction terms.

3

Keep Torque and Energy Together Revise tau = MB sin theta, W = MB(1 - cos theta), and U = -MB cos theta in one set. Stable equilibrium corresponds to minimum potential energy, so direction language and sign logic must be read along with the formula.

4

Check Whether the Question Wants Magnitude or Direction The same bar magnet can produce different field direction statements on axial and equatorial lines. In torque questions, the vector relation M cross B matters, but many NEET MCQs only require the magnitude after the angle is identified correctly.

Download Topic Notes

PDF · Cheat Sheet · MCQ Set · PYQ
📄
Full Topic Notes
Detailed notes on axial and equatorial fields, short-magnet approximation, and dipole behavior in a uniform magnetic field.
PDF7 Pages
Download Notes
📝
Formula Sheet
One-page sheet for Ba, Be, tau = MB sin theta, U = -MB cos theta, and the short-magnet inverse-cube forms.
PDF1 Page
Download Formulas
🎯
MCQ Practice
Practice set on field geometry, torque, work, potential energy, and magnetic dipole orientation.
PDF30 Questions
Download MCQs
⏳
Previous Year Questions
Selected PYQs on bar-magnet field formulas and magnetic dipole equilibrium in external field.
PDF12 Questions
Download PYQs

Topic Coverage

2-Column Table
Column AColumn B

Quick Revision

Concept → Trap → Example

1) Force and Field Due to Bar Magnet

Axial Line

For a short bar magnet, the magnetic field on the axial line is Ba = (mu0/4pi)(2M/r^3). The exact finite-length expression contains l, but the inverse-cube form is the exam favorite when r is much larger than the magnetic length.

  • Axial position means the observation point lies on the magnetic axis of the bar magnet.
  • The factor 2 is the quickest identifier of axial field in the short-magnet limit.
  • Trap: students often copy the equatorial expression and miss the extra factor 2.
Example (NEET-style)If a short magnet has magnetic moment M and the point lies at distance r = 2a on its axis, the field becomes Ba = (mu0/4pi)(2M/(2a)^3) = (mu0/4pi)(M/4a^3).

2) Force and Field Due to Bar Magnet

Equatorial Line

On the equatorial line of a short bar magnet, the field magnitude is Be = (mu0/4pi)(M/r^3). It has the same inverse-cube dependence as the axial field but only half its magnitude at the same distance.

  • Equatorial position is perpendicular to the magnetic axis through the centre of the magnet.
  • At the same r, Ba : Be = 2 : 1 for the short-magnet formulas.
  • Trap: writing the right inverse-cube dependence but carrying the axial factor 2 into the equatorial case.
Example (NEET-style)For the same magnet and same centre-to-point distance r, if the axial field is 6 x 10^-5 T, the equatorial field is 3 x 10^-5 T because the equatorial magnitude is half the axial magnitude.

3) Force and Field Due to Bar Magnet

Dipole in Field

A bar magnet in uniform magnetic field experiences torque tau = MB sin theta, potential energy U = -MB cos theta, and work W = MB(1 - cos theta) when turned from stable alignment. These relations encode both orientation and stability.

  • Torque becomes zero when the dipole is parallel or anti-parallel to the field.
  • Potential energy is minimum in stable equilibrium and maximum in unstable equilibrium.
  • Trap: confusing zero torque with minimum energy. Anti-parallel orientation has zero torque too, but it is unstable.
Example (NEET-style)If a dipole of moment 0.5 A m^2 is held at 60 degree in a uniform field of 0.2 T, the torque magnitude is tau = MB sin 60 degree = 0.5 x 0.2 x root3/2 N m.

US Curriculum Gaps

Note for NRI/OCI students studying abroad.

Position-Specific Dipole Fields Are Less Emphasised In Some Tracks

Many school treatments stop at qualitative field-line pictures of a bar magnet, while NEET expects immediate use of separate axial and equatorial formulas with the correct distance dependence.

  • axial carries factor 2
  • both short-magnet fields scale as 1/r^3

Energy Language Is Tested As Physics, Not Memorised Terminology

The chapter expects you to connect stable and unstable equilibrium to the sign of U = -MB cos theta and not just to a descriptive sentence about alignment.

  • zero torque is not enough
  • minimum U marks stable equilibrium

Concept IQ Check

Exam-style checks
1For the same short bar magnet and same distance r from its centre, the ratio of axial field to equatorial field is:Field ratio
1 : 1
2 : 1
1 : 2
4 : 1
For a short magnet, Ba = (mu0/4pi)(2M/r^3) and Be = (mu0/4pi)(M/r^3). The common factor cancels immediately, leaving Ba/Be = 2. NEET likes this question because it checks whether the student remembers that the same inverse-cube dependence appears in both positions while the numerical factor changes only because of geometry.
2A magnetic dipole is anti-parallel to a uniform magnetic field. Which statement is correct?Energy logic
torque is maximum and potential energy is minimum
torque is zero and potential energy is maximum
torque is zero and potential energy is zero always
torque is maximum and potential energy is zero
At theta = 180 degree, tau = MB sin theta becomes zero, but U = -MB cos theta becomes +MB, which is the maximum value. That makes the anti-parallel orientation an unstable equilibrium. The trap is to think zero torque automatically means stable configuration, but stability depends on whether the potential energy is minimum, not merely on the torque vanishing at that instant.

NEET Practice Questions

Click "Reveal Answer" after attempting
1The field at a point on the equatorial line of a short bar magnet varies with distance r as:
1/r
1/r^2
1/r^3
1/r^4
👁 Reveal Answer
1/r^3. In the short-magnet limit the equatorial field is Be = (mu0/4pi)(M/r^3), so the inverse-cube dependence is exact for the simplified result.
2If the axial field of a short magnet at a point is 8 x 10^-6 T, then the equatorial field at the same distance is:
16 x 10^-6 T
8 x 10^-6 T
4 x 10^-6 T
2 x 10^-6 T
👁 Reveal Answer
4 x 10^-6 T. At equal distance, the equatorial field is half the axial field for a short bar magnet.
3The torque on a magnetic dipole in a uniform field is maximum when the angle between M and B is:
0 degree
30 degree
60 degree
90 degree
👁 Reveal Answer
90 degree. Since tau = MB sin theta, the torque magnitude is largest when sin theta = 1.
4Potential energy of a magnetic dipole in a uniform magnetic field is minimum when the dipole is:
parallel to the field
perpendicular to the field
anti-parallel to the field
at 45 degree to the field
👁 Reveal Answer
Parallel to the field. For theta = 0 degree, U = -MB cos theta becomes -MB, the least possible value.
5Gauss's law in magnetism states that net magnetic flux through a closed surface is:
positive
negative
zero
infinite
👁 Reveal Answer
Zero. The law expresses the non-existence of isolated magnetic monopoles in standard classical treatment, so the total magnetic flux through any closed surface is always zero.

Physics Revision Checklist

Check off chapters as you revise

Use this section for quick chapter tracking before mocks, part tests, and final NEET revision.

Tip: Mark a chapter complete only after revising formulas, solving PYQs, and reviewing your error log for that chapter.

Frequently Asked Questions

Notes · Downloads · Revision · Important Questions
Why is the axial field of a short magnet larger than the equatorial field at the same distance?
Because the axial expression carries an extra factor 2, so the short-magnet result on the axis is twice the equatorial magnitude at equal distance.
What is the most common formula mistake in this topic?
Students often swap the axial and equatorial expressions, especially by carrying the axial factor 2 into the equatorial case or by forgetting which position lies on the magnetic axis.
When does a magnetic dipole experience zero torque in a uniform field?
When it is parallel or anti-parallel to the field, because sin theta becomes zero in tau = MB sin theta.
Does zero torque always mean stable equilibrium?
No. A dipole anti-parallel to the field also has zero torque, but its potential energy is maximum there, so that orientation is unstable.
Why does potential energy become negative in stable alignment?
Because U = -MB cos theta, and in parallel orientation cos theta = 1, giving U = -MB, the minimum energy configuration.
What does the short-magnet approximation mean physically?
It means the observation point is far compared with the magnetic length of the magnet, so the magnet behaves like an ideal dipole and the field reduces to the inverse-cube forms.
Why is Gauss's law in magnetism mentioned with bar magnets?
Because it captures the basic dipole fact that magnetic poles do not exist as isolated monopoles in this classical chapter treatment, so net flux through any closed surface remains zero.
How does NEET usually test this topic?
Most questions are direct formula or concept checks on axial versus equatorial field, or on torque, work, and potential energy of a magnetic dipole in uniform field.
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