Q.A circular coil of wire consisting of 100 turns, each of radius 8.0 cm carries a current of 0.40 A. What is the magnitude of the magnetic field B at the centre of the coil?
Concept understanding — Magnetic Force Balance
Magnetic Force Balance
When a current-carrying wire or coil sits in a magnetic field, it feels a force F=BILsinθ (or, for a point charge, F=qvBsinθ). On its own that force just pushes the conductor - but in many real situations the push is deliberately set up to CANCEL another force, so the whole system sits in equilibrium. That equilibrium condition - magnetic force balanced against weight, against another wire's magnetic force, or against a mechanical counterweight - is what "magnetic force balance" means, and it is also historically how the ampere itself was defined.
The balance condition
Whenever a conductor is in equilibrium under a magnetic force and one other force, the two must be equal and opposite:
BILsinθ=Fother
Solving this equation for whichever quantity is unknown (B, I, L, or the other force) is the entire skill in this class of problem - the only new step, beyond the force law itself, is correctly identifying what the magnetic force is opposing.
Case 1: a wire suspended against gravity
A straight horizontal wire of mass m and length l, carrying current I, can be held up ("floated") in mid-air by a horizontal magnetic field perpendicular to it. The upward magnetic force must equal the downward weight:
BIl=mg⟹B=Ilmg
For example, a 200g, 1.5m wire carrying 2A needs B=(2)(1.5)(0.2)(9.8)≈0.65T to stay suspended.
Case 2: two wires balancing each other
Two long parallel wires carrying currents I1,I2 exert a force per unit length on each other of 2πdμ0I1I2 (attractive if the currents run the same way, repulsive if opposite). If one wire is free to move, this magnetic force can itself balance that wire's weight:
2πhμ0I2L=mg⟹h=2πmgμ0I2L
This is exactly how a "current balance" apparatus works, and historically it is how the ampere was defined: the current that, flowing in two infinite parallel wires one metre apart, produces a force of exactly 2×10−7N per metre of length.
Case 3: balancing on a beam
A current-carrying coil arm hanging from one pan of a beam balance feels an extra force F=NBIl when only that arm sits in an external field. Re-balancing the beam means adding a mass m so that mg=NBIl.
Always check which length enters the formula - for a coil of N turns the force multiplies by N; for a single suspended straight wire it doesn't.
The direction of the magnetic force (via the right-hand rule on IL×B) has to already point the right way to oppose the other force - check direction FIRST, before solving the magnitude equation, or you may set up a balance condition that is physically backwards.
Why this differs from the general force law
The formula F=BILsinθ is common to every problem here - but "magnetic force balance" problems are specifically the ones where the magnetic force is set exactly equal to something else (gravity, another wire's force, a beam's counterweight) so the system sits still. It is this equilibrium framing, not the force law by itself, that defines the concept, and what distinguishes it from the general force-on-a-current topic.
Balancing the magnetic force on a current-carrying conductor against gravity or another wire's force is a classic numerical application from the NCERT Class 12 Physics chapter on moving charges and magnetism, tested in CBSE boards and JEE Main. Students searching "force on a current carrying conductor in magnetic field numericals class 12" will find this equilibrium-condition approach, including the historical current-balance definition of the ampere, matches the NCERT treatment.
Why this formula?
Magnetic Force Balance: Why the Key Formulas Hold
The Magnetic Force Balance describes when the magnetic force on a charged particle or current-carrying conductor is exactly balanced by another force (gravity, electric force, or tension). Let's build the reasoning step-by-step.
1. The Core Idea: What Does "Balance" Mean?
A force balance means the net force on an object is zero:
Fnet=0
For magnetic forces we use the Lorentz force law:
- On a moving charge: Fm=q(v×B)
- On a current-carrying wire: Fm=I(L×B)
When this is balanced by another force (say gravity Fg=mg):
Fm+Fother=0
2. Case 1: Charged Particle in Crossed Fields (Velocity Selector)
A charged particle moves perpendicular to both electric field E and magnetic field B.
- Electric force: Fe=qE (along E)
- Magnetic force: Fm=q(v×B) (perpendicular to both v and B)
For straight-line motion (no deflection), the two forces must cancel:
qE=qvB⇒v=BE
Key insight: Only particles with this exact speed pass undeflected — this is how velocity selectors work in mass spectrometers.
3. Case 2: Current-Carrying Wire Balanced by Gravity
A horizontal wire carrying current I sits in a perpendicular magnetic field B, suspended by strings.
The magnetic force on a straight wire is Fm=ILBsinθ; for a wire perpendicular to the field (θ=90∘), Fm=ILB. Setting this equal to the weight Fg=mg for equilibrium:
ILB=mg
Key insight: This balance lets you measure B if I, L, and m are known — the principle behind a current balance experiment.
4. Case 3: Circular Motion of a Charged Particle
A charged particle moving perpendicular to a uniform magnetic field has the magnetic force supply the centripetal force:
qvB=rmv2⇒r=qBmv
Key insight: The radius depends on momentum (mv) and charge-to-mass ratio — this is why cyclotrons and mass spectrometers work.
5. Quick Summary
| Situation | Balanced Forces | Key Formula |
|---|---|---|
| Velocity selector | qE vs qvB | v=E/B |
| Current balance | ILB vs mg | ILB=mg |
| Circular motion | qvB vs mv2/r | r=mv/(qB) |
Every formula follows the same recipe: identify all forces, set the vector sum to zero (or to ma), and solve along the direction of interest. Because the magnetic force is always perpendicular to both velocity/current and field, getting the direction right matters as much as the magnitude.
The key idea is the magnetic field at the centre of a circular coil, given by the formula for a current-carrying loop.
Step 1 – Write the formula
For a single circular loop of radius r carrying current I, the field at the centre is
Bsingle=2rμ0I
Step 2 – Adjust for N turns
For N closely wound turns, the fields add, so
B=N⋅2rμ0I
Step 3 – Substitute values
N=100, I=0.40 A, r=8.0 cm=0.080 m, μ0=4π×10−7 T m/A
B=2×0.080100×(4π×10−7)×0.40
Simplify:
B=0.16100×4π×10−7×0.40=1100×4π×10−7×2.5
B=1000π×10−7=π×10−4 T
The magnitude of the magnetic field at the centre is 3.14×10−4 T.
The magnetic field at the centre of a circular coil is given by B=2Rμ0NI. Substituting N=100, I=0.40 A, R=0.080 m gives B=3.14×10−4 T.
Why the centre is special
When current flows through a circular loop, each tiny segment of wire produces a magnetic field that points along the axis at the centre. By symmetry, all these contributions add up in the same direction — straight out of the plane of the coil (or into it, depending on current direction). The centre is the simplest point to calculate because every current element is at the same distance R from the point, and the angle between the element and the line joining it to the centre is always 90∘.
For a single turn, the field at the centre is:
Bsingle=2Rμ0I
where μ0=4π×10−7 T⋅m/A is the permeability of free space.
If you have N turns closely wound together, each turn contributes the same field at the centre, so the total field is simply N times that of one turn:
B=N⋅2Rμ0I
This is the formula we’ll use.
Step-by-step calculation
-
Write down the known quantities
- Number of turns: N=100
- Current: I=0.40 A
- Radius: R=8.0 cm=0.080 m (always convert to metres)
- μ0=4π×10−7 T⋅m/A
-
Plug into the formula
B=2Rμ0NI=2×0.080(4π×10−7)×100×0.40
-
Simplify step by step
First, the numerator:
4π×10−7×100=4π×10−5
Then multiply by 0.40:
4π×10−5×0.40=1.6π×10−5
Denominator:
2×0.080=0.16
So:
B=0.161.6π×10−5
-
Cancel the factor of 0.16
Notice 1.6/0.16=10, so:
B=10×π×10−5=π×10−4
-
Evaluate numerically
π≈3.1416, so:
B≈3.14×10−4 T
A common mistake is to forget that R must be in metres, not centimetres. Using R=8.0 (in cm) would give an answer 100 times too large. Always convert cm to m by dividing by 100.
Notice that B came out as π×10−4 exactly — a neat result because NI/(2R)=100×0.40/0.16=250, and 250×4π×10−7=π×10−4. This kind of simplification often happens in textbook problems, so keep an eye out for cancellations.
The magnitude of the magnetic field at the centre is 3.14×10−4 T.
Method: Biot–Savart Law for a Circular Current Loop
This is the standard method for finding the magnetic field at the centre of a current-carrying circular coil.
Steps
- Recall the formula For a single circular loop of radius r carrying current I, the magnetic field at the centre is:
Bsingle=2rμ0I
- Account for multiple turns For a coil with N turns, each turn contributes equally, so:
B=N⋅2rμ0I
- Insert the given values
- N=100
- r=8.0 cm=0.080 m
- I=0.40 A
- μ0=4π×10−7 T m A−1
B=100×2×0.0804π×10−7×0.40
-
Simplify step by step
- Numerator: 4π×10−7×0.40=1.6π×10−7
- Denominator: 2×0.080=0.16
- So: B=100×0.161.6π×10−7
Since 0.161.6=10, we get:
B=100×10×π×10−7=1000π×10−7
- Final magnitude
B=π×10−4 T
Numerically:
B≈3.14×10−4 T
Key Concept Check
- The field is directly proportional to N and I, and inversely proportional to r.
- At the centre, all turns produce the field in the same direction (perpendicular to the plane of the coil), so the net field is simply N times that of a single turn.
Here are the most common mistakes students make when solving this standard magnetic field problem, along with how to avoid each.
1. Forgetting the Number of Turns (N)
The Mistake:
Students often use the formula for a single loop:
B=2Rμ0I
This gives the field for one turn only. For a coil of N turns, the field is N times larger.
How to Avoid:
Always check if the problem mentions “N turns” or “N loops.” The correct formula for a circular coil is:
B=2Rμ0NI
Here, N=100, so the field is 100 times the field of a single loop.
2. Unit Conversion Errors (cm → m)
The Mistake:
Plugging R=8.0 directly into the formula without converting to metres.
Since μ0 is in SI units (4π×10−7 T m/A), the radius must be in metres.
How to Avoid:
Convert all lengths to metres before substituting:
R=8.0 cm=0.080 m
A quick check: if you forget, your answer will be off by a factor of 100.
3. Using the Wrong Value of μ0
The Mistake:
Using μ0=4π×10−7 but forgetting the 4π in calculations, or using an approximate value like 1.26×10−6 incorrectly.
How to Avoid:
Write μ0 explicitly as 4π×10−7 and keep it symbolic until the final step. Cancel π where possible to simplify arithmetic.
4. Arithmetic Errors with π Cancellation
The Mistake:
After substituting, students often multiply and divide without simplifying π first, leading to messy decimals and errors.
How to Avoid:
Write the expression step-by-step:
B=2×0.080(4π×10−7)×100×0.40
Cancel π and simplify numbers first:
B=0.164π×10−7×40=0.16160π×10−7
Then 160/0.16=1000, so:
B=1000π×10−7=π×10−4 T
Final answer: B=3.14×10−4 T.
5. Confusing Centre vs. Axis Formula
The Mistake:
Using the formula for field on the axis of a coil (which includes distance x from centre) instead of the simpler centre formula.
How to Avoid:
The problem explicitly says “at the centre.” For the centre of a circular coil:
Bcentre=2Rμ0NI
Only use the axis formula if the point is not at the centre.
6. Forgetting the Direction (When Asked)
The Mistake:
If the problem asks for magnitude and direction, students often give only the magnitude.
How to Avoid:
Use the right-hand thumb rule: curl fingers along current direction, thumb points in direction of B at centre. For a coil, the field is perpendicular to the plane of the coil. If direction is required, state it clearly (e.g., “out of the page” or “along the axis”).
Quick Checklist to Avoid All Mistakes
- ✓ Use B=2Rμ0NI (not single-loop formula)
- ✓ Convert R to metres
- ✓ Keep μ0=4π×10−7 and cancel π
- ✓ Simplify numbers step-by-step
- ✓ Use centre formula, not axis formula
- ✓ State direction if asked
Final Answer for Reference:
B=3.14×10−4 T
- AP EAPCET 2026Set eng-2026-05-14-AN1 markMCQQ.The radius of a coil of wire with N turns is 0.1 m and 2A current flows in the coil as shown. A long straight wire carrying a current of 20π A as shown is located at 0.5 m from the centre of the coil. The number of turns in the coil if the resultant magnetic field at the centre of the coil is zero [FIGURE: a circular coil of radius r carrying a current of 2A, with a current-direction arrow shown on the loop; a long straight wire is drawn above the coil (dashed line) carrying a current of 20π A shown flowing to the left, positioned at a perpendicular distance of 0.5 m from the coil's centre] (A) 2 (B) 4 (C) 6 (D) 10
›Reveal solutionSolution
This tests superposition of the magnetic field of a circular coil (at its centre) and of a long straight wire, set to cancel — solve for N by equating magnitudes.
Concept and Intuition
A circular coil of N turns carrying current I produces a field at its own centre of B=2rμ0NI, directed along the coil's axis (direction fixed by the right-hand rule for the shown current sense). A long straight wire carrying current I produces, at perpendicular distance d, a field B=2πdμ0I, circling the wire (again right-hand rule). The problem is engineered so that, given the current directions in the figure, these two fields point in opposite directions at the coil's centre. "Resultant field is zero" therefore just means the two magnitudes are equal — the geometry/direction part is already built into the problem statement, so we only need magnitude balance.
Step-by-Step Solution
- Field due to the coil at its centre: Bcoil=2rμ0NIcoil=2(0.1m)μ0N(2)=10μ0N.
- Field due to the straight wire at the coil's centre (distance d=0.5 m): Bwire=2πdμ0Iwire=2π(0.5)μ0(20π)=πμ0⋅20π=20μ0.
- Setting Bcoil=Bwire (opposite directions, net zero): 10μ0N=20μ0⇒N=2.
Common Mistakes
- Forgetting the factor of N (number of turns) in the coil's field formula.
- Mixing up 2r (coil formula) with 2πd (straight-wire formula) — they look similar but are structurally different.
- Not cancelling the π correctly when Iwire=20π A is combined with the 2πd in the denominator.
✓Final answerThe correct option is (A) — 2.
ANSWER: A
- AP EAPCET 2025Set eng-2025-05-21-AN1 markMCQQ.If a straight current carrying wire of linear density 0.12 kgm−1 is suspended in mid air by a uniform horizontal magnetic field of 0.5 T normal to the length of the wire, then the current through the wire is (Acceleration due to gravity =10 ms−2; Neglect earth's magnetic field) (A) 2.4 A (B) 1.2 A (C) 0.6 A (D) 4.8 A
›Reveal solutionSolution
A current-carrying wire floats in a horizontal magnetic field when the magnetic force exactly cancels gravity; solving gives I=2.4 A.
Concept and Intuition
A straight wire carrying current I in a magnetic field B (perpendicular to the wire) experiences a force per unit length F/L=BI. For the wire to be suspended in mid-air (in equilibrium), this magnetic force must balance the weight per unit length of the wire, which is λg where λ is the linear mass density.
Step-by-Step Solution
- Force balance per unit length: BI=λg.
- Solve for current: I=Bλg.
- Substitute values: λ=0.12 kg m−1, g=10 m s−2, B=0.5 T.
- I=0.50.12×10=0.51.2=2.4 A.
Common Mistakes
- Forgetting that the balance is per unit length, so total wire length L cancels out.
- Mixing up direction: the force must be upward to cancel gravity, which fixes the direction of current relative to B, but doesn't change the magnitude calculation.
✓Final answerThe correct option is (A) — 2.4 A.
ANSWER: A
- AP EAPCET 2022Set eng-2022-07-06-AN1 markMCQQ.Two infinitely long wires are placed at (1cm, 1cm) and (+1cm, -1cm) with 1A current in each and in the same directions perpendicular to x-y plane. Let the magnetic field due to these current carrying wires at the origin be B. If B0 is the magnitude of the field if only one of them was present, then B0∣B∣ is (A) 2 (B) 1 (C) 21 (D) 221
›Reveal solutionSolution
Two parallel wires symmetric about the x-axis add their fields at the origin constructively along one direction; the resultant is 2 times the field of either wire alone.
Concept and Intuition
An infinite straight wire carrying current I produces a field of magnitude μ0I/(2πd) at perpendicular distance d, circling the wire (direction given by z^×r^, where r^ points from the wire towards the field point, for current along +z^). With two wires we must add the two field vectors, not just their magnitudes.
Step-by-Step Solution
- Wire 1 is at (1,1) cm, wire 2 at (1,−1) cm; both distances from the origin are d=12+12=2 cm, so each alone gives a field of magnitude B0=2π2μ0I.
- Vector from wire 1 to origin: r1=(−1,−1). Field direction ∝z^×r1=(1,−1,0) (up to normalization).
- Vector from wire 2 to origin: r2=(−1,1). Field direction ∝z^×r2=(−1,−1,0).
- Adding the (equal-magnitude) contributions: the x-components (+1 and −1, in matched units) cancel, and the y-components (−1 and −1) add, doubling that component relative to each single wire's y-component contribution.
- Careful vector addition (each wire contributes magnitude B0 total, only half of which — by symmetry of the 45∘ geometry — survives after cancellation/addition) gives net magnitude ∣B∣=2B0.
Common Mistakes
- Simply adding magnitudes (2B0) instead of vectors — the directions are not parallel.
- Getting the direction of z^×r^ backwards and concluding the fields cancel to zero.
✓Final answerThe correct option is (A) — 2.
ANSWER: A
- AP EAPCET 2022Set eng-2022-07-06-FN1 markMCQQ.Two long parallel straight metal wires A and B carrying currents 12 A and 36 A respectively, in the same direction are separated by 50 cm. The point relative to A, where the resultant magnetic induction between the two wires due to the currents is zero, will be (A) 90 cm (B) 7.5 cm (C) 28 cm (D) 12.5 cm
›Reveal solutionSolution
With both currents in the same direction, the magnetic fields cancel only in the region between the two wires. Equating BA=BB and solving gives the null point at 12.5 cm from wire A (closer to the weaker current, as expected).
Concept and Intuition
Each long straight wire produces a field B=2πdμ0I circling around it. Between two wires carrying current in the same direction, the two fields point in opposite directions (one wire's field goes into the page there, the other's comes out), so they can cancel at some point between them. The cancellation point sits closer to the wire with the smaller current (since a weaker source needs to be closer to match the stronger one's field at the same magnitude).
Step-by-Step Solution
- Let the null point be at distance x from wire A, so it is at (50−x) cm from wire B.
- Equate the magnitudes: 2πxμ0(12)=2π(50−x)μ0(36).
- Cancel common factors: x12=50−x36.
- Cross-multiply: 12(50−x)=36x⇒600−12x=36x⇒600=48x.
- x=12.5 cm.
Common Mistakes
- Looking for the null point outside the wires (impossible here since currents are in the same direction — outside, the fields always add).
- Forgetting that the null point should be closer to the smaller-current wire (A, 12 A) — getting x>25 cm would be a red flag.
✓Final answerThe correct option is (D) — 12.5 cm.
ANSWER: D
- AP EAPCET 2021Set eng-2021-10-05-FN1 markMCQQ.A tangent galvanometer has a coil of 50 turns and a radius of 20 cm. The horizontal component of earth's magnetic field is 3×10−5 T. What will be the current which gives a deflection of 45°? (A) 5π3 A (B) 3π5 A (C) 53π A (D) 35π A
›Reveal solutionSolution
At a 45° deflection the tangent law gives tan45°=1, so the coil's magnetic field exactly equals Earth's horizontal field, letting us solve directly for the current: I=5π3A.
Concept and Intuition
A tangent galvanometer balances the magnetic field of its coil against Earth's horizontal field H; the needle's deflection θ obeys tanθ=HBcoil, where Bcoil=2rμ0nI.
Step-by-Step Solution
- Tangent law: Bcoil=Htanθ. At θ=45°, tan45°=1, so Bcoil=H.
- Bcoil=2rμ0nI, so 2rμ0nI=H⇒I=μ0n2rH.
- Substitute r=0.2m, H=3×10−5T, n=50, μ0=4π×10−7: I=(4π×10−7)(50)2(0.2)(3×10−5)=2π×10−51.2×10−5=2π1.2=π0.6.
- Simplify: π0.6=5π3A.
Common Mistakes
- Forgetting that tan45°=1 simplifies the tangent law nicely — some students needlessly keep tanθ symbolic and make arithmetic slips.
✓Final answerThe correct option is (A) — 5π3 A.
ANSWER: A
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