Magnetic Field at the Centre of a Circular Current Loop

Physics · Moving Charges And Magnetism · NEET

The magnetic field at the centre of a circular current loop is B = μ₀I/2R for one turn, and B = μ₀NI/2R for N turns, where R is the loop radius and I the current. It points along the axis, and its direction is given by the right-hand rule. Memory hook: "centre of a loop = half of μ₀I over R" (the ½ is the signature of the loop; a straight wire has no ½).
Field at the centre of a circular current loopIcentreRB(along axis)B = μ₀ N I / 2Rno π in denominatorN = turns, R in metresRight-hand rule: fingers curl with I,thumb points along B at the centre
Every element of the loop is a distance R from the centre with dl perpendicular to R, so the Biot-Savart terms add cleanly to give B = μ₀NI/2R directed along the axis (right-hand rule).

Your doubts, answered

Is the denominator 2R or 2πR for the field at the centre of a loop?

It is 2R. The formula is B = μ₀I/2R. Students confuse it with the straight-wire formula B = μ₀I/2πR, which does have π. Trick: the circular loop already 'used up' the geometry, so its centre field is cleaner with just 2R. If you ever see 2πR for a loop's centre, it is wrong.

Why is there no sin θ term in the field at the centre of a loop?

In Biot-Savart, dB = (μ₀/4π)(I dl sinθ)/r². For every small element of the loop, the element dl is always perpendicular to the line joining it to the centre, so θ = 90° and sinθ = 1. Also every element is the same distance r = R from the centre. Both simplifications remove the angle term, giving a clean B = μ₀I/2R.

How is the centre-of-loop field different from a straight-wire field?

A long straight wire gives B = μ₀I/2πR (has π, field circles the wire). A circular loop's centre gives B = μ₀I/2R (no π, field points along the axis through the centre). Same μ₀I but the loop is stronger at equal R because its whole length wraps around one point.

If a coil has N turns, does N multiply the field?

Yes. N identical turns of radius R stacked at the same place carry current I each, and their fields add: B = μ₀NI/2R. A 100-turn coil gives 100 times the field of a single turn. This is why coils, not single loops, are used to make strong fields.

Which way does the field point at the centre?

Along the axis, perpendicular to the plane of the loop. Curl the right hand's fingers along the current direction; the extended thumb points the way B goes at the centre. One face of the loop acts like a North pole (field coming out), the other like South.

⚠️ The NEET trap
Using B = μ₀I/2πR (the straight-wire formula) for the centre of a loop, or forgetting to multiply by N for a multi-turn coil.
For the centre of a circular loop use B = μ₀I/2R (no π). For N turns use B = μ₀NI/2R. Convert radius to metres before substituting.
🧠 Loop centre = NO π. Straight wire = HAS π. And never drop the N for a coil.

Real NEET questions

2024

A tightly wound 100 turns coil of radius 10 cm carries a current of 7 A. The magnitude of the magnetic field at the centre of the coil is (Take μ₀ = 4π × 10⁻⁷ SI units):

A · 4.4 T
B · 4.4 mT
C · 44 T
D · 44 mT
Solution: Use B = μ₀NI/2R. Here N = 100, I = 7 A, R = 10 cm = 0.1 m. Numerator = μ₀NI = 4π×10⁻⁷ × 100 × 7 = 2800π×10⁻⁷ = 8.796×10⁻⁴. Then B = 8.796×10⁻⁴ / (2×0.1) = 8.796×10⁻⁴ / 0.2 = 4.4×10⁻³ T = 4.4 mT. Note the radius must be in metres, and N is not forgotten. Answer: B.
2026

A 100-turn closely wound circular coil of radius 5 cm has a magnetic field of 3.14 × 10⁻³ T at its centre. The current flowing through the coil, and the magnitude of the magnetic moment of this coil are, respectively: (Take μ₀ = 4π × 10⁻⁷ T m/A)

A · 2 A, 10 A m²
B · 2.5 A, 20 A m²
C · 2 A, 4 A m²
D · 2.5 A, 2 A m²
Solution: Step 1 (find I): from B = μ₀NI/2R, I = 2BR/(μ₀N) = (2 × 3.14×10⁻³ × 0.05)/(4π×10⁻⁷ × 100). Numerator = 3.14×10⁻⁴. Denominator = 4π×10⁻⁵ ≈ 1.2566×10⁻⁴. So I = 3.14×10⁻⁴ / 1.2566×10⁻⁴ = 2.5 A. Step 2 (magnetic moment): m = NIA = NI(πR²) = 100 × 2.5 × π × (0.05)² = 250 × π × 2.5×10⁻³ = 250 × 7.85×10⁻³ ≈ 1.96 ≈ 2 A m². Answer: D.

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Frequently asked

What is the formula for the magnetic field at the centre of a circular loop?

For a single turn, B = μ₀I/2R. For a coil of N turns of the same radius, B = μ₀NI/2R, where μ₀ = 4π×10⁻⁷ T m/A, I is current in amperes and R is radius in metres.

How do you derive B = μ₀I/2R using Biot-Savart law?

Take dB = (μ₀/4π)(I dl sinθ)/r². At the centre every element has θ = 90° (sinθ = 1) and r = R. So dB = (μ₀/4π)(I dl)/R². Integrating dl around the loop gives 2πR, so B = (μ₀I/4πR²)(2πR) = μ₀I/2R.

What is the direction of the magnetic field at the centre of a loop?

It is along the axis of the loop, perpendicular to its plane. Use the right-hand rule: curl fingers along the current, the thumb shows the field direction at the centre.

Does the field at the centre depend on the loop's radius?

Yes, inversely. B = μ₀I/2R, so a smaller radius gives a stronger field at the centre for the same current. Doubling R halves the central field.

Why is the loop field larger than a straight wire field at the same distance?

The loop formula μ₀I/2R has no π in the denominator, while the straight wire has μ₀I/2πR. Because every part of the loop wraps around the centre, all contributions add up in the same direction, giving a bigger field.