davisnotes/mag_intro.html

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<title>Magnetism - Introduction - Physics 299</title>
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<h1>Introduction to Magnetism <br>
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<div class="copy-paste-block"><font color="#ff0000"><i><span
class="bqQuoteLink">"</span></i></font><font
color="#ff0000"><i><span class="bqQuoteLink">Physics Is
Imagination In A Straight Jacket</span></i><span></span>"</font><br>
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<font color="#ff0000"><i> </i><font color="#000000">John Moffat</font></font><br>
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<li>As we will see shortly, Electricity and Magnetism are
different aspects of the same basic physical phenomenon - hence
the description <a
href="http://www.britannica.com/EBchecked/topic/183324/electromagnetism">Electromagnetism.</a>&nbsp;&nbsp;</li>
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<li>However, initially it is convenient to treat magnetism in a
separate, but similar, manner to electricity.&nbsp; In other
words we will define, magnetic forces, magnetic fields and
magnetic dipoles exactly as we did the electric variables.</li>
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<li>After this initial description we will develop the
relationship between magnetism and electricity through Faraday's
Law of Induction and the Displacement Current, leading finally
to a complete description of (classical) electromagnetism in the
form of <a href="http://www.maxwells-equations.com/">Maxwell's
equations</a>.</li>
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<li>So our starting point in describing magnetism will be the
assumption of the existence of a magnetic field, <b>B</b>, the
origin of which will be described later.</li>
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<li><img alt="fig3" src="mag_intro_fig3.jpg" align="right"
height="193" width="257">Exactly as for the electric field <b>E</b>,
we will assume that the <b>B</b> field can be represented by
field lines where,</li>
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<li>the tangent to a field line gives the direction of <b>B</b>
at that point and</li>
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<li>the number of field lines per unit cross sectional area is
proportional to the strength of <b>B</b>.</li>
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<li><img alt="exclamation" src="exclamation-icon.gif" height="30"
width="31"> It is important to realize immediately that unlike
electric field lines, magnetic field lines <u><i><b>DO NOT</b></i></u>
represent the direction of the force acting on a charged
particle.</li>
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<blockquote><img alt="exclamation" src="exclamation-icon.gif"
height="30" width="31">&nbsp; The magnetic phenomenon most
familiar to most people is that of permanent magnetism -
refrigerator magnets etc.&nbsp; As it happens, permanent magnetism
is not a simple topic to explain.&nbsp; In fact a complete
description requires a detailed knowledge of the quantum behavior
of materials.&nbsp; For this reason we will barely mention
permanent magnets in this course. <br>
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Q: What is the name of the first electricity detective?<br>
A: Sherlock Ohms </i></font><br>
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&nbsp;<img src="celticbar.gif" height="22" width="576"> <br>
&nbsp;
<p><i>Dr. C. L. Davis</i> <br>
<i>Physics Department</i> <br>
<i>University of Louisville</i> <br>
<i>email</i>: <a href="mailto:c.l.davis@louisville.edu">c.l.davis@louisville.edu</a>
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