Q.A short bar magnet placed with its axis at 30∘ with a uniform external magnetic field of 0.25T experiences a torque of magnitude equal to 4.5×10−2J. What is the magnitude of magnetic moment of the magnet?
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.
Note
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)
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 momentM=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=0.25T, 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=0.36A⋅m2
✓Final answer
The magnetic moment of the magnet is 0.36A⋅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=0.36A⋅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=4.5×10−2J (torque has units of N·m, which is the same as J)
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 betweenM and B directly — here it's given as 30∘, so sin30∘ is correct. Don't overcomplicate it.
Tip
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.
✓Final answer
The magnitude of the magnetic moment is 0.36A⋅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=0.25T
τ=4.5×10−2J (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=0.36A⋅m2
Step 5: Write the final answer
M=0.36A⋅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 Bis 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 4.5×10−2J. 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=0.36A⋅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=0.36A⋅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.