Is This a Case of Motional emf?

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A straight wire moving through a magnetic field generates a motional emf, but if the magnet moves toward the wire, no emf is produced unless the reference frame changes. In a frame where the wire moves, motional emf arises from the forces on charge carriers due to their motion through the magnetic field. Conversely, if the magnet is considered stationary and the wire is part of a circuit, an emf can be induced based on the Faraday/Maxwell equation due to the changing magnetic flux. The discussion clarifies that while a moving magnet creates an electric field, the absence of a circuit means no emf can be induced in the wire alone. Ultimately, understanding the reference frame is crucial for determining the presence and type of emf.
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If a straight length of wire moves in a suitable direction through the magnetic field of a magnet, there will be a motional emf in the wire. If the magnet moves toward the wire, is there an emf in the wire, motional or otherwise?
 
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Strictly, no. Whether the emf is classed as motional or not depends on your reference frame.

If your frame is one in which the magnet is stationary and the wire moves, you have a motional emf. It can be thought of as arising from the qvxB forces on the charge carriers in the conductor, as the conductor moves through space.

If you are in a frame in which the magnet moves and the wire is stationary, but part of a circuit, there will be an emf in that circuit according to the Faraday/Maxwell equation
\oint Edl = -\int\int \frac{\partial B}{\partial t}dA. The line integral is evaluated around the closed loop of the circuit, and the surface integral over any surface bounded by the circuit. So the force on the charge carriers is qE, arising from the electric field produced by the changing magnetic field.

Faraday's description of the phenomenon – the emf arises when the magnetic flux linking a circuit changes – fits in either reference frame.
 
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Thanks. It is as I suspected. To be more precise I should have asked if there would be a potential difference between the ends of the wire, arising from a non-electrostatic emf induced in the wire. The TOTAL emf would be zero in that case, also.
 
It has been pointed out to me elsewhere that a moving magnet is accompanied by an electric field. Therefore, the wire, being in that field, will have an emf.
 
That's what I meant when I said (above) "So the force on the charge carriers is qE, arising from the electric field produced by the changing magnetic field."
 
Yes, but you specified that there had to be a circuit, and there is none.
 
I did indeed specify a circuit, as I was trying to deal with the case of an emf in a wire, as posed in your original question. But I agree that the Faraday/Maxwell equation that I quoted does not require the line integral to be taken around a conducting circuit. I'm sorry if I inadvertently misled.
 
No problem; I believe that it is all clear, now. Thanks.
 
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