Notes on Relativity and Cosmology - Physics Department, UCSB
Notes on Relativity and Cosmology - Physics Department, UCSB
Notes on Relativity and Cosmology - Physics Department, UCSB
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2.1. THE BASICS OF E & M 45<br />
⋆ C<strong>on</strong>versely, Maxwell discovered that an electric field which changes in time<br />
produces a magnetic field. Maxwell codified both this observati<strong>on</strong> <strong>and</strong> Faraday’s<br />
law in a set of equati<strong>on</strong>s known as, well, Maxwell’s equati<strong>on</strong>s. Thus, a field that<br />
is purely electric in <strong>on</strong>e reference frame will have a magnetic part in another<br />
frame of reference.<br />
As a result, it is best not to think of electricity <strong>and</strong> magnetism as separate phenomena.<br />
Instead, we should think of them as forming a single “electromagnetic”<br />
field which is independent of the reference frame. It is the process of breaking<br />
this field into electric <strong>and</strong> magnetic parts which depends <strong>on</strong> the reference frame.<br />
There is a str<strong>on</strong>g analogy 2 with the following example: The spatial relati<strong>on</strong>ship<br />
between the physics building <strong>and</strong> the Hall of Languages is fixed <strong>and</strong> independent<br />
of any coordinate system. However, if I am st<strong>and</strong>ing at the <strong>Physics</strong> building<br />
<strong>and</strong> want to tell some<strong>on</strong>e how to walk to HOL, depending <strong>on</strong> which directi<strong>on</strong> I<br />
am facing I may tell that pers<strong>on</strong> to “walk straight ahead across the quad,” or I<br />
might tell them to “walk mostly in the directi<strong>on</strong> I am facing but bear a little to<br />
the right.” The relati<strong>on</strong>ship is fixed, but the descripti<strong>on</strong> differs. For the moment<br />
this is just a taste of an idea, but we will be talking much more about this in<br />
the weeks to come. In the case of electromagnetism, note that this is c<strong>on</strong>sistent<br />
with the discovery that magnetic charge is really moving electric charge.<br />
Not <strong>on</strong>ly do we find a c<strong>on</strong>ceptual unity between electricity <strong>and</strong> magnetism, but<br />
we also find a dynamical loop. If we make the electric field change with time<br />
in the right way, it produces a magnetic field which changes with time. This<br />
magnetic field then produces an electric field which changes with time, which<br />
produces a magnetic field which changes with time..... <strong>and</strong> so <strong>on</strong>. Moreover, it<br />
turns out that a changing field (electric or magnetic) produces a field (magnetic<br />
or electric) not just where it started, but also in the neighboring regi<strong>on</strong>s of space.<br />
This means that the disturbance spreads out as time passes! This phenomen<strong>on</strong><br />
is called an electromagnetic wave. Electromagnetic waves are described in more<br />
detail below in secti<strong>on</strong> 2.1.1, <strong>and</strong> all of their properties follow from Maxwell’s<br />
equati<strong>on</strong>s. For the moment, we merely state an important property of electromagnetic<br />
waves: they travel with a precise (finite) speed. See secti<strong>on</strong> 2.1.1 for<br />
the derivati<strong>on</strong>.<br />
2.1.1 Maxwell’s Equati<strong>on</strong>s <strong>and</strong> Electromagnetic Waves<br />
The purpose of this secti<strong>on</strong> is to show you how Maxwell’s equati<strong>on</strong>s lead to<br />
electromagnetic waves (<strong>and</strong> just what this means). This secti<strong>on</strong> is more mathematical<br />
than anything else we have d<strong>on</strong>e so far, <strong>and</strong> I will probably not go<br />
through the details in class. If you’re not a math pers<strong>on</strong>, you should not be<br />
scared off by the calculati<strong>on</strong>s below. The important point here is just to get<br />
the general picture of how Maxwell’s equati<strong>on</strong>s determine that electromagnetic<br />
waves travel at a c<strong>on</strong>stant speed.<br />
2 This analogy may be clear as mud at the moment, but will be clearer later in the course<br />
as we think about a number of similar effects.