Q.A short bar magnet placed with its axis at 30∘ with a uniform external magnetic field of 0.25 T experiences a torque of magnitude equal to 4.5×10−2 J. What is the magnitude of magnetic moment of the magnet?
Concept understanding — Magnetic Poles
Magnetic Poles: The Intuition First
Imagine you have a bar magnet — the kind you might have stuck on your refrigerator. If you bring two of them close, something interesting happens. Sometimes they snap together with a satisfying click. Other times, they push each other away, refusing to touch no matter how hard you try.
That's not random. Every magnet has two special regions, one at each end, where the magnetic force is strongest. These are its magnetic poles.
The word "pole" comes from the Greek polos, meaning "pivot" or "axis" — the Earth itself has a North Pole and a South Pole, and it behaves like a giant magnet.
The Two Types of Poles
Every magnet has exactly two poles: a north pole and a south pole. You cannot have a magnet with only one pole — cut a bar magnet in half, and each half immediately becomes a complete magnet with its own north and south poles.
The rule of interaction is simple and memorable:
- Unlike poles attract: north pulls south, south pulls north.
- Like poles repel: north pushes north away; south pushes south away.
This is the fundamental behaviour. No exceptions.
The Precise Statement
Magnetic poles are the regions of a magnet where the external magnetic field is strongest. Every magnet has exactly two poles — a north pole and a south pole — that cannot be isolated. Like poles repel; unlike poles attract.
The key points to remember for exams:
- Poles always come in pairs — there is no magnetic monopole (a single isolated pole) in nature, despite decades of searching.
- The north pole is defined as the pole that points toward Earth's geographic north when the magnet is freely suspended.
- The south pole points toward Earth's geographic south.
A Common Confusion (Watch Out)
Earth's geographic North Pole is actually a magnetic south pole. Why? Because the north pole of a compass needle (which is a magnetic north pole) is attracted to it. And unlike poles attract. So the Earth's north pole behaves like a magnetic south pole. This often trips students up in exams.
Why This Matters
Magnetic poles are the starting point for understanding everything from simple compasses to electric motors, generators, and MRI machines. The idea that "opposites attract" in magnetism is the same principle that makes electric charges behave the way they do — but with one crucial difference: you can have a single positive or negative electric charge, but you can never have a single magnetic pole.
That asymmetry is one of the deepest facts about magnetism.
The behaviour of magnetic poles — always in pairs, with like poles repelling and unlike poles attracting — is covered in the NCERT Class 12 Physics chapter on magnetism and matter, a frequent source of short-answer CBSE board questions. Searches for "magnetic poles and Earth's magnetism class 12 physics" will find this north-south pole explanation, including the Earth's-north-pole-is-a-magnetic-south-pole detail, matches the NCERT textbook's own framing.
Why this formula?
Magnetic Poles: Why the Key Formulas Hold
Let's build this from first principles — understanding why a magnetic pole behaves the way it does, not just memorizing the result.
1. What Is a Magnetic Pole?
A magnetic pole is a conceptual point where the magnetic field appears to originate or terminate. In reality, magnetic poles always come in north-south pairs (no isolated monopoles exist in nature), but we treat them as idealized sources for calculations.
- North pole: source of magnetic field lines (outward)
- South pole: sink of magnetic field lines (inward)
2. The Key Formula: Force Between Two Magnetic Poles
The force between two magnetic poles of strengths m1 and m2, separated by distance r, is:
F=4πμ0⋅r2m1m2
Why this form?
This is a Coulomb's law analog — and that's not a coincidence. Here's the reasoning:
-
Experimental observation: Magnetic poles attract/repel with a force that:
- Varies as 1/r2 (inverse square law)
- Is proportional to the product of pole strengths
- Depends on the medium (via μ0, the permeability of free space)
-
Mathematical analogy: The magnetic field B at distance r from a single pole m is:
B=4πμ0⋅r2m
This comes from Gauss's law for magnetism applied to a point source.
- Force derivation: The force on pole m2 in the field of pole m1 is:
F=m2⋅B1=m2⋅(4πμ0⋅r2m1)
Hence:
F=4πμ0⋅r2m1m2
Key insight: The 1/r2 dependence is not arbitrary — it follows from the geometry of 3D space (flux spreads over a sphere of area 4πr2).
3. The Magnetic Field of a Bar Magnet (Two Poles)
For a bar magnet of length 2l with poles +m and −m, the field at a point on the axis at distance x from the center is:
B=4πμ0⋅(x2−l2)22ml
Why this form?
-
Superposition principle: The total field is the vector sum of fields from the north pole (+m) and south pole (−m).
-
Field from north pole at distance (x−l):
BN=4πμ0⋅(x−l)2m(away from north)
- Field from south pole at distance (x+l):
BS=4πμ0⋅(x+l)2m(toward south)
- Net field (both along same direction on axis):
B=BN−BS=4πμ0m[(x−l)21−(x+l)21]
- Simplify using algebra:
(x−l)21−(x+l)21=(x2−l2)24xl
Therefore:
B=4πμ0⋅(x2−l2)24mxl
But for a bar magnet, the magnetic moment is M=m⋅(2l) (pole strength × separation). So 2ml=M, giving:
B=4πμ0⋅(x2−l2)22Mx
Key insight: The field is not simply 1/r2 because we have two poles — the net effect is a dipole field, which falls off as 1/r3 at large distances.
4. The Far-Field Approximation (Dipole Formula)
For x≫l (far from the magnet), x2−l2≈x2, so:
B≈4πμ0⋅x32M
Why 1/x3?
- A single pole gives 1/r2
- Two opposite poles separated by distance d give a dipole — the fields nearly cancel at large distances, leaving a weaker 1/r3 dependence
- This is a universal property of dipoles (electric or magnetic)
5. Torque on a Magnetic Dipole in a Uniform Field
τ=MBsinθ
Why this form?
-
Force on each pole: In uniform field B, north pole feels F=mB along field, south pole feels F=mB opposite field.
-
Torque calculation: These equal and opposite forces form a couple:
- Lever arm = 2lsinθ (perpendicular distance between forces)
- Torque = force × lever arm = (mB)×(2lsinθ)
-
Using magnetic moment M=m⋅2l:
τ=MBsinθ
Key insight: The torque tries to align the magnet with the field — this is why a compass needle points north.
Summary Table: Why Each Formula Has Its Form
| Formula | Key Reason |
|---|---|
| F∝1/r2 | Flux spreads over sphere area 4πr2 |
| F∝m1m2 | Force is proportional to source strength (linear response) |
| B∝1/x3 (dipole) | Two opposite poles nearly cancel; residual is dipole field |
| τ=MBsinθ | Lever arm depends on sinθ in a couple |
Remember: Every formula in magnetism is either a Coulomb analog (for poles) or a superposition of such analogs. The 1/r2 law is the foundation — everything else builds on it.
Concept: Magnetic Poles — torque on a magnetic dipole in a uniform field depends on the magnetic moment, field strength, and the sine of the angle between them.
Step 1: The torque on a magnetic dipole is
τ=MBsinθ
where M is the magnetic moment, B=0.25 T, and θ=30∘.
Step 2: Substitute the given values:
4.5×10−2=M×0.25×sin30∘
Since sin30∘=0.5, this becomes
4.5×10−2=M×0.25×0.5=M×0.125
Step 3: Solve for M:
M=0.1254.5×10−2=0.36 A⋅m2
The magnetic moment of the magnet is 0.36 A⋅m2.
The torque on a magnetic dipole in a uniform field is τ=MBsinθ. Using the given values, the magnetic moment works out to M=0.36 A⋅m2.
The key idea here is that a bar magnet behaves like a magnetic dipole — it has a north and south pole separated by a small distance, giving it a magnetic moment M. When placed in an external magnetic field B, the field exerts a torque that tries to align the moment with the field. The magnitude of this torque depends on three things: the strength of the moment, the strength of the field, and the angle between them.
The formula τ=MBsinθ is the magnetic analogue of τ=pEsinθ for an electric dipole in an electric field. The sinθ factor tells you that the torque is maximum when the dipole is perpendicular to the field (θ=90∘) and zero when it's aligned (θ=0∘ or 180∘). Here, the axis is at 30∘ to the field, so the angle between M (which points along the axis from south to north) and B is exactly 30∘.
Let's work through the numbers.
- Write down the torque equation. For a magnetic dipole in a uniform field,
τ=MBsinθ
where τ is the torque magnitude, M is the magnetic moment magnitude, B is the field magnitude, and θ is the angle between M and B.
-
Identify the given quantities.
- τ=4.5×10−2 J (torque has units of N·m, which is the same as J)
- B=0.25 T
- θ=30∘
-
Solve for M.
Rearranging the formula:
M=Bsinθτ
- Plug in the values. sin30∘=21=0.5, so
M=0.25×0.54.5×10−2=0.1254.5×10−2
- Do the division.
M=1.25×10−14.5×10−2=1.254.5×10−1=3.6×10−1=0.36 A⋅m2
A common mistake is to use the angle between the axis and the field as 60∘ (the complement), thinking torque depends on the perpendicular component. But the formula uses the angle between M and B directly — here it's given as 30∘, so sin30∘ is correct. Don't overcomplicate it.
Notice that torque has units of energy (J), and B has units of T (which is N/(A·m)). So M=τ/(Bsinθ) gives units of J·m/N = (N·m)·m/N = m², but multiplied by A from the definition of T gives A·m² — exactly the unit of magnetic moment. A quick unit check can catch errors.
The magnitude of the magnetic moment is 0.36 A⋅m2.
Method: Torque on a Magnetic Dipole in a Uniform Field
This problem uses the torque formula for a magnetic dipole (bar magnet) placed in a uniform external magnetic field.
Steps
Step 1: Recall the torque formula
The torque τ experienced by a magnetic dipole of magnetic moment M placed in a uniform magnetic field B at an angle θ between the dipole axis and the field is:
τ=MBsinθ
Step 2: Identify the given values
- θ=30∘
- B=0.25 T
- τ=4.5×10−2 J (Note: torque has units of N·m, which is same as J)
Step 3: Rearrange the formula for M
M=Bsinθτ
Step 4: Substitute and calculate
sin30∘=21
M=0.25×214.5×10−2=0.1254.5×10−2
M=0.36 A⋅m2
Step 5: Write the final answer
M=0.36 A⋅m2
Key Concept Check
- Torque is maximum when θ=90∘ (perpendicular)
- Torque is zero when θ=0∘ or 180∘ (parallel or antiparallel)
- The unit A⋅m2 is equivalent to J/T for magnetic moment
Here are the common mistakes students make on this exact problem, along with how to avoid each one.
1. Using the Wrong Formula for Torque
Mistake:
Students often confuse torque on a current loop (τ=NIABsinθ) with torque on a magnetic dipole (τ=MBsinθ). They may also mistakenly use cosθ instead of sinθ.
How to avoid:
- For a bar magnet (a magnetic dipole), the torque is always:
τ=MBsinθ
where θ is the angle between the magnetic moment vector M and the external field B.
- Memorise: Torque is maximum when θ=90∘ (perpendicular), and zero when aligned (θ=0∘). This helps you remember it’s sinθ, not cosθ.
2. Misidentifying the Angle θ
Mistake:
The problem says the axis is at 30∘ to the field. Many students take θ=30∘ directly, but sometimes the angle given is between the axis and the field — which is exactly θ for a bar magnet.
How to avoid:
- For a bar magnet, the magnetic moment M points along the axis from south to north.
- So the angle between M and B is the angle given between the axis and the field.
- Here, θ=30∘ is correct. Do not use 90∘−30∘=60∘ unless the problem says “angle with the perpendicular.”
3. Forgetting to Convert Units
Mistake:
Torque is given as 4.5×10−2 J. Since torque has units of N·m, some students mistakenly treat it as energy and try to use work formulas.
How to avoid:
- Torque and energy both have the same SI unit (Joule = N·m), but they are different physical quantities.
- In this formula, τ is torque, not work. Just plug it in directly — no conversion needed.
- Always check: if the problem says “torque,” use τ=MBsinθ.
4. Solving for M Incorrectly
Mistake:
After substituting, students sometimes invert the sine or forget to divide by sinθ.
How to avoid:
- Write the formula clearly:
M=Bsinθτ
- Substitute step-by-step:
M=0.25×sin30∘4.5×10−2
Since sin30∘=0.5:
M=0.25×0.54.5×10−2=0.1254.5×10−2
- Then compute:
M=0.36 A⋅m2
- Double-check: The answer should be in A·m² (or J/T). If you get a very small or huge number, re-check the division.
5. Not Stating the Final Answer with Correct Units
Mistake:
Giving M=0.36 without units, or writing wrong units like N·m.
How to avoid:
- Magnetic moment has SI unit A·m² (ampere metre squared) or equivalently J/T (joule per tesla).
- Always write:
M=0.36 A⋅m2
- In exams, missing units can cost you marks even if the number is correct.
Quick Summary Checklist
| Mistake | Fix |
|---|---|
| Wrong formula | Use τ=MBsinθ for a bar magnet |
| Wrong angle | θ = angle between axis and field = 30∘ |
| Unit confusion | Torque is in N·m, just plug in as given |
| Calculation error | Solve stepwise: M=τ/(Bsinθ) |
| Missing units | Answer in A·m² or J/T |
By avoiding these, you’ll solve this problem correctly every time.
- CBSE 2026Set ANNUAL1 markQ.If magnetic monopoles existed then write the equation of Gauss's law for magnetism.
›Reveal solutionSolution
Currently Gauss's law for magnetism states the net magnetic flux through any closed surface is zero (no monopoles); if monopoles existed, the right side would instead equal mu0 times the enclosed pole strength, just like the electric case.
Gauss's law for magnetism in its present form is: the closed surface integral (over any closed surface S) of B . dA = 0, reflecting the experimental fact that isolated magnetic poles (monopoles) have never been observed - magnetic field lines always form closed loops with no starting/ending point (no magnetic 'charge'). If magnetic monopoles did exist, with an isolated pole strength qm enclosed by the surface, this law would take a form exactly analogous to Gauss's law for electric charge:
closed-surface integral of B . dA = mu0 * qm_enclosed
i.e. the net magnetic flux through a closed surface would be proportional to the net magnetic 'charge' enclosed, just as electric flux is proportional to enclosed electric charge (qenclosed/epsilon0).
✓Final answerClosed-surface integral of B.dA = mu0 * (net enclosed pole strength qm), instead of zero.
- CBSE 2025Set ANNUAL1 markMCQQ.The value of magnetic induction at a distance r from a single pole is inversely proportional to(a) r(b) r^2(c) 1/r(d) 1/r^2
›Reveal solutionSolution
An isolated magnetic pole of strength m produces B = (mu0/4pi)(m/r^2), an inverse-square law, so the magnetic induction is inversely proportional to r^2.
The magnetic field (magnetic induction) at a distance r from a single magnetic pole of pole strength m is given by Coulomb's law of magnetism:
B = (mu0 / 4*pi) * (m / r^2)
The distance r appears in the denominator as r^2, so B decreases as the square of the distance - if r is doubled, B falls to one quarter. In the wording of the question, "inversely proportional to" is therefore completed by r^2. This mirrors the inverse-square fall-off of a point charge's electric field.
[!ANSWER]
(b) r^2.
- CBSE 2025Set ANNUAL1 markMCQQ.The ultimate individual unit of magnetism in any magnet is :(a) north pole(b) south pole(c) magnetic dipole(d) quadrupole
›Reveal solutionSolution
Isolated magnetic monopoles (single north or south poles) do not exist in nature; magnetic poles always occur in pairs, so the magnetic dipole is the basic unit of magnetism.
Unlike electric charge, where an isolated positive or negative charge can exist, no isolated magnetic 'monopole' has ever been observed. If a bar magnet is cut into pieces, each piece becomes a smaller magnet with its own north and south pole — the poles can never be separated. This means the fundamental, indivisible unit of magnetism is always a pair of poles, i.e., a magnetic dipole (analogous to an electric dipole), not a single north or south pole.
✓Final answerThe magnetic dipole is the ultimate individual unit of magnetism — option (c).
- CBSE 2025Set ANNUAL1 markQ.The strength of bar magnet is maximum at its center. (T/F)
›Reveal solutionSolution
This statement is False — the strength (pole strength) of a bar magnet is maximum at its two ends (poles), not at its centre.
A bar magnet's magnetism is concentrated near its two ends, called the north and south poles, where the pole strength m is maximum. At the exact centre of the magnet, the effects of the two equal and opposite poles (north and south) tend to cancel, so the net magnetic effect (and hence the 'strength' measurable there) is minimum, not maximum. So the correct statement should be that the strength is maximum at the poles/ends.
✓Final answerFalse — the strength of a bar magnet is maximum at its poles (ends), not its centre.
- CBSE 2024Set A1 markMCQQ.The value of magnetic potential at a distance r from a pole strength m is (A) (μ₀/4π)(m/r) (B) (μ₀/4π)(m/r^2) (C) (μ₀/4π)(m/r^3) (D) zero
›Reveal solutionSolution
Magnetic scalar potential of a pole falls as 1/r: V = (μ₀/4π)(m/r).
By analogy with electrostatics, a magnetic pole of strength m produces a field that falls off as 1/r2:
B=4πμ0r2m,
and a magnetic scalar potential that falls off as 1/r:
V=4πμ0rm.
Just as the electric potential (∝1/r) is the integral of the field (∝1/r2), the magnetic potential varies as 1/r while the field varies as 1/r2. So the correct expression is (μ0/4π)(m/r).
✓Final answer(A) (μ₀/4π)(m/r).
- CBSE 2022Set I1 markMCQQ.S.I. unit of pole strength is (A) Am^-1 (B) Am^-2 (C) Am (D) Fm
›Reveal solutionSolution
SI unit of magnetic pole strength = ampere-metre (A·m).
The magnetic dipole moment of a bar magnet is m = (pole strength) × (magnetic length), i.e. M = q_m × 2l. The SI unit of magnetic moment is A·m² (same as current × area). Since the magnetic length has unit metre:
qm=2lM=mAm2=Am
So pole strength has the unit ampere-metre.
✓Final answer(C) Am.
- CBSE 2021Set A1 markMCQQ.S.I. unit of magnetic pole strength is (A) N (B) N/A.m (C) A.m (D) A.m/N
›Reveal solutionSolution
Magnetic pole strength has SI unit ampere·metre (A·m).
Magnetic pole strength m is related to magnetic moment by M = m × 2l, where 2l is the magnetic length. Since magnetic moment has unit ampere·metre² (A·m²) and length has unit metre, pole strength has unit:
[m]=mA⋅m2=A⋅m
So the SI unit of pole strength is ampere-metre (A·m).
✓Final answer(C) A.m.
- CBSE 2019Set ANNUAL1 markQ.________ Law for magnetism establishes that monopoles do not exist.
›Reveal solutionSolution
Gauss's Law for magnetism states the net magnetic flux through any closed surface is always zero — the direct proof that isolated magnetic monopoles do not exist.
Gauss's law for magnetism is written as:
∮B⋅dA=0
for any closed surface. This is in contrast to Gauss's law for electric fields, ∮E⋅dA=qenc/ε0, which is non-zero whenever a net electric charge (monopole) is enclosed.
Because magnetic field lines always form closed loops (they emerge from a north pole and re-enter at a south pole, continuing through the magnet back to the north pole), every field line that enters a closed surface must also leave it. So the net outward flux is always exactly zero — meaning there is no magnetic 'charge' (monopole) that field lines can originate from or terminate on, unlike electric charge.
✓Final answerGauss's Law for magnetism (∮B⋅dA=0) establishes that isolated magnetic monopoles do not exist.
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