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Introductory Physics Volume Two

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116 Time Varying Fields 6.2<br />

The induced current is caused by an electric field. This induced<br />

electric field is not like the other electric fields we have seen. This is a<br />

new type of electric field. The electric field is created by the changing<br />

magnetic field.<br />

The electric field wraps around the changing<br />

magnetic field somewhat like a static magnetic field<br />

wraps around a steady current. There are some additional<br />

subtleties due to the fact that the induced<br />

electric field is caushed by the change in the magnetic<br />

field. The relationship between the induced electric<br />

field and the changing magnetic field is stated in the<br />

following law of physics.<br />

Fact: Faraday’s Law<br />

The line integral of the electric field around any closed curve is<br />

equal to negative the rate of change of the magnetic flux through<br />

any surface bounded by the curve.<br />

∮<br />

⃗E · ⃗dl = − d ∫<br />

dt<br />

⃗B · ⃗ dA<br />

Notice that this is very similar to Ampere’s Law:<br />

∮<br />

∫<br />

⃗B · ⃗dl = µ 0<br />

⃗J · dA ⃗<br />

Ampere’s Law and Faraday’s Law both relate the line integral around<br />

closed curve to the flux of a vector field through the area enclosed by<br />

the curve. The difference is that Faraday’s Law has the time derivative<br />

of the flux.<br />

Another important and potentially confusing thing to notice, is<br />

that the line integral of the electric field ( ∫ ⃗ E · ⃗ dl) has so far been<br />

referred to as the electric potential difference between the end points<br />

of the curve. The confusing thing is that since it is a closed curve the<br />

electric potential difference must be zero, ∆V = 0, while Faraday’s Law<br />

tells us that the line integral of the induced electric field is not zero, but<br />

equal to the rate of change of the magnetic flux. So we learn from this<br />

that the force caused by the induced electric field is not a conservative<br />

force field. We also see that there is no electric potential associated with<br />

this electric field, ( ⃗ E ≠ − ⃗ ∇V ). To avoid confusion we will refer to the<br />

line integral of the induced electric field by its historical name, the<br />

electromotive force, or EMF. In equations the EMF is represented by<br />

the symbol E, so that E = ∮ ⃗ E · ⃗ dl. Note that the unit of EMF is the<br />

volt.

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