12.11.2014 Views

Introductory Physics Volume Two

Introductory Physics Volume Two

Introductory Physics Volume Two

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

6.3 Maxwell’s Extension of Ampere’s Law 119<br />

• Third Quarter: E and B ↓ and |B| ↘.<br />

• Fourth Quarter: E and B ↑ and |B| ↗.<br />

Here are the same four quarters in diagrams:<br />

Notice that if the magnitude of the flux is decreasing, the fields have<br />

the same sign. While if the magnitude of the flux is increasing, the<br />

fields have opposite sign. This observation is usually stated in terms of<br />

the current that is caused by the induced electric field if a loop of wire<br />

is placed in line with the electric field loop.<br />

Fact: Lenz’s Law<br />

The induced current creates a magnetic field that opposes the<br />

change in the magnetic flux.<br />

⊲ Problem 6.1<br />

Check to see that Lenz’s law is obeyed in all four quarters in the previous<br />

example.<br />

§ 6.3 Maxwell’s Extension of Ampere’s Law<br />

We have seen that a changing magnetic field causes an electric field.<br />

It ends up that a changing electric field will also cause a magnetic field.<br />

∮<br />

∫<br />

⃗B · ⃗dl d<br />

= µ 0 ɛ 0<br />

⃗E · dA<br />

dt<br />

⃗<br />

This magnetic field is added to the magnetic field produced by currents<br />

so that we arrive at an extension of Ampere’s law that makes it<br />

applicable to time varying fields.<br />

Fact: Ampere’s Law - Time Varying<br />

∮<br />

∫<br />

∫<br />

⃗B · ⃗dl = µ 0<br />

⃗J · dA ⃗ d<br />

+ µ 0 ɛ 0<br />

dt<br />

= µ 0 I through + µ 0 ɛ 0<br />

dφ e<br />

dt<br />

⃗E · ⃗ dA

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!