Why a Loop Outside the Field Region Still Gets an EMF

Physics · Electromagnetic Induction · NEET

A loop can sit fully outside the magnetic field region and still have an induced EMF, but ONLY if it encloses the changing field. EMF depends on the flux through the loop's area, not on whether the wire itself is in the field. Memory hook: "It is not where the wire is, it is what the loop wraps around." If the loop encloses a changing field it gets EMF; if the changing field is entirely outside the loop, EMF is zero.
B(t), radius rdB/dtxxxxLoop 1 (radius R)EMF = -(dB/dt) pi r squaredB(t)radius rxxLoop 2 (outside)no fluxEMF = 0
Left: Loop 1 (red) encloses the changing-field region of radius r, so its EMF uses the field area πr², not πR². Right: Loop 2 (green, dashed) sits fully outside the field region — no changing flux passes through it, so its EMF is zero.

Your doubts, answered

The wire is outside the field, so how can there be any EMF at all?

EMF is not created at the wire because the wire feels the field. Faraday's law says EMF = rate of change of flux THROUGH the loop's enclosed area (ε = -dΦ/dt). If a changing magnetic field passes through the flat area bounded by the loop, the flux changes and an EMF appears, even though the wire itself is in a field-free region. So the correct question is never 'is the wire in the field?' but 'does the loop enclose changing flux?'

Loop 1 (radius R) surrounds a small field region (radius r < R). Which area do I use for the EMF?

Use only the area that actually has field. The flux through loop 1 is Φ = B × (πr²), because the field exists only inside radius r; the extra ring between r and R has zero field and adds nothing. So EMF = -(dB/dt)πr², NOT -(dB/dt)πR². A very common NEET mistake is plugging in πR².

Loop 2 is entirely outside the field region. Why is its EMF exactly zero?

Loop 2's enclosed area has no magnetic field anywhere inside it (the field lives inside radius r, which is completely outside loop 2). So its flux Φ = 0 at all times, and dΦ/dt = 0, giving EMF = 0. It does not matter that the field is changing somewhere far away; that change is not passing through loop 2's area.

But my teacher said a changing B creates an induced electric field even in the field-free region outside — doesn't that drive a current in loop 2?

Both statements are true and they do not contradict. A changing B does create a swirling induced electric field E even outside radius r. That E can push charges. But the NET EMF around loop 2 is the closed line integral of E, which by Faraday's law equals -dΦ/dt through loop 2. Since loop 2 encloses zero flux, the induced E-field pushes on one side and pulls back equally on the other, and the total EMF around the closed loop cancels to zero. Local E is non-zero; the loop's net EMF is zero.

Is EMF about the wire moving or about the flux changing here?

Here nothing moves. This is 'static' EMF caused purely by a time-changing B (dB/dt), not motional EMF. There is no rod, no velocity, no Bvl. The only rule you need is ε = -dΦ/dt, with Φ = B × (area that has field, enclosed by the loop).

⚠️ The NEET trap
Use πR² for loop 1 because the loop has radius R, giving EMF = -(dB/dt)πR².
Use πr², the area that actually contains field: EMF = -(dB/dt)πr² in loop 1. The empty ring between r and R carries no flux. Loop 2 (fully outside) encloses zero field, so its EMF is zero. Correct choice: loop 1 = -(dB/dt)πr², loop 2 = zero.
🧠 Loop 1 has radius R but the field only fills radius r. Which radius goes in the area?

Real NEET questions

2016

A uniform magnetic field is restricted within a region of radius r. The magnetic field changes with time at a rate dB/dt. Loop 1 of radius R > r encloses the region r and loop 2 of radius R is outside the region of magnetic field. Then the e.m.f. generated is:

A · Zero in loop 1 and zero in loop 2
B · -(dB/dt)πr² in loop 1 and -(dB/dt)πr² in loop 2
C · -(dB/dt)πR² in loop 1 and zero in loop 2
D · -(dB/dt)πr² in loop 1 and zero in loop 2
Solution: Step 1 - Rule: EMF = -dΦ/dt, where Φ = B times the area of the loop that actually contains magnetic field. Step 2 - Loop 1 (radius R) encloses the whole field region of radius r. Field exists only inside radius r, so flux Φ₁ = B(πr²). The ring between r and R has no field, so it adds nothing. EMF₁ = -d/dt[B·πr²] = -(dB/dt)πr². Do NOT use πR². Step 3 - Loop 2 lies completely outside the field region, so no field passes through its area: Φ₂ = 0 at all times, hence dΦ₂/dt = 0 and EMF₂ = 0. Step 4 - Match: loop 1 = -(dB/dt)πr², loop 2 = zero. Answer: D.

Solved Electromagnetic Induction NEET PYQs

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Frequently asked

Can a coil have EMF if it is nowhere near the magnetic field wire?

Yes, if the changing field passes through the area the coil encloses. EMF depends on enclosed flux (ε = -dΦ/dt), not on the wire touching the field. If the field is entirely outside the enclosed area, EMF is zero.

Why do we use πr² and not πR² for the enclosing loop?

Flux counts only the region that actually has field. The field exists inside radius r, so Φ = B(πr²). The area between r and R is field-free and contributes zero flux, no matter how big R is.

Is there an electric field outside the changing-field region?

Yes. A changing magnetic field produces a circulating induced electric field even outside radius r (E is non-zero there). But for a loop enclosing no flux, the net EMF (closed integral of E) is zero because the contributions cancel around the loop.

Is this motional EMF or static EMF?

Static EMF. Nothing moves; the EMF comes purely from dB/dt (time-changing field). There is no velocity, so ε = Bvl does not apply here — only ε = -dΦ/dt.

Why does this concept matter for NEET?

NTA repeats this exact loop-1 vs loop-2 idea (2016 PYQ) to test whether you use enclosed flux or the loop's geometric size. Getting πr² vs πR² right, and loop 2 = 0, is a guaranteed one-mark decision.