russ_watters said:
Yes, but the OP has not provided a valid reference, which means a direct quote and a link to where it may be read/heard in context. That's the only way for other users to judge the quote for themselves. 'Take my word for it' isn't a reference.
Unless the reference is posted so the others here can know what the heck the OP is talking about, this thread will have to be locked.
No need to get up in arms about it. Don't you have a copy? So here's a reference and quote.
The Feynman Lectures on Physics, Feynman, Leighton, and Sands, 1964
Volume II, section 17-2. Exceptions to the "flux rule"
"We now give some examples, due in part to Faraday, which show the importance of keeping clearly in mind the distinction between the two effects responsible for emf's. Our examples involve situations to which the "flux rule" cannot be applied--either because there is no wire at all or because the
path taken by induced currents moves about within an extended volume of a conductor."
These exceptions consist of a 1) homoplanar motor and 2) two conducting plates with arced surfaces that have a contact point, that when rocked together change the amount of enclosed flux but produce no change in emf around the loop. Each plate is connected to a wire to a galvenometer to form a complete circuit. These are given in figures 17-2 and 17-3.
In closing to 17-2,
"When the material of the curcuit is changing, we must return to the basic laws. The
correct physics is always given by the two basic laws
F = q(E + v \cross B)[/itex]<br />
<br />
\nabla \cross E = -\frac{\partial B}{\partial t}\ .[/itex]&quot;<br />
<br />
The flux rule is given in section 17-1 by<br />
<br />
&quot;emf = wB \frac{dL}{dt} = wBv \ .[/itex]&amp;quot;