Appropriate Language when Discussing Faraday's Law

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The discussion centers on the appropriate phrasing when describing induced electromotive force (emf) in coils, debating whether to say "an emf is induced in the coil" or "an emf is induced across the coil." It is highlighted that emf is not a force but a potential difference, which typically occurs between two points. However, in the context of Faraday's Law, the induced emf does not conform to traditional definitions of potential difference due to the lack of a conservative force. The complexities of measuring voltage across coils are also discussed, emphasizing that voltmeter readings can be misleading in dynamic electromagnetic scenarios. Ultimately, the consensus leans towards using "an emf is induced in the coil" as the more accurate expression.
tzonehunter
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Quick question, when discussing induce emf, would you state:

"An emf is induced in the coil..."
or

"An emf is induced across the coil..."

The reason I ask is that grammatically, it sounds proper to state "An electromotive force is induced in..." (something). However, an emf is a potential difference, which would occur across two points.
 
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tzonehunter said:
"An emf is induced in the coil..."

Definitely. Some people use the term electromotance since emf is not a force and is measured in volts. The result of the Faraday Law is to create a current. This does imply the existence of an electric force which implies the existence of a potential difference. However in a closed good conducting loop having no definite beginning or end you cannot put a voltmeter across any part of it and get the same reading unless the length of the arc subtended is the same. One can think of the situation as being a distributed potential difference i.e., potential difference per unit length that exists around the entire loop.
 
tzonehunter said:
"An emf is induced in the coil..."

That's the way I see it used.

However, an emf is a potential difference, which would occur across two points.

No, that is true only in the electrostatic case. If you review an introductory calculus-based physics textbook, you will see the explanation for why the induced EMF is not a potential difference. In short, to have a potential difference you need two potentials so you can subtract them, and since you do not have a conservative force you cannot define an electrostatic potential.
 
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tzonehunter said:
"An emf is induced in the coil..."
or

"An emf is induced across the coil..."

I thought perhaps this would be a useful illustration here... a photo I took of the innards of an electric skateboard hub motor (84mm tire diameter) with exposed stator core consisting of 12 wound coils/solenoids...

IMG-2257.jpg
 
Mister T said:
That's the way I see it used.

No, that is true only in the electrostatic case. If you review an introductory calculus-based physics textbook, you will see the explanation for why the induced EMF is not a potential difference. In short, to have a potential difference you need two potentials so you can subtract them, and since you do not have a conservative force you cannot define an electrostatic potential.
Good one @Mister T.

It should further be pointed out that a voltmeter does not always indicate the voltage across its two probe tips. In the aforementioned case of a coil of resistance r surrounding a time-changing B field, if the probes are placed across some arc section θ of the coil, and if there is no B-dot field within the meter circuit (coil section θ, the meter and its probe wiring), the voltmeter will read rθI/2π, I = current. This is often mistaken as the voltage across the coil section θ but in reality that voltage is zero. The reason is that the meter wiring itself forms an alternate arc for coil section θ of the closed path. Furthermore, the voltmeter itself always reads actual voltage across itself assuming it forms a negligible length of the meter circuit. Cf. my Insight article on Dr Lewin's conundrum.
 
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