<?xml version="1.0" encoding="UTF-8" standalone="yes"?><oembed><version><![CDATA[1.0]]></version><provider_name><![CDATA[Azimuth]]></provider_name><provider_url><![CDATA[https://johncarlosbaez.wordpress.com]]></provider_url><author_name><![CDATA[John Baez]]></author_name><author_url><![CDATA[https://johncarlosbaez.wordpress.com/author/johncarlosbaez/]]></author_url><title><![CDATA[Network Theory Seminar (Part&nbsp;3)]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>&nbsp;</p>
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<p>This time we use the principle of minimum power to determine what a circuit made of resistors actually <i>does</i>. Its &#8216;behavior&#8217; is described by a functor sending circuits to linear relations between the potentials and currents at the input and output terminals.  We call this the &#8216;black box&#8217; functor, since it takes a circuit:</p>
<div align="center"><img src="https://i2.wp.com/math.ucr.edu/home/baez/networks/circuit_made_of_resistors.png" /></div>
<p>and puts a metaphorical &#8216;black box&#8217; around it:</p>
<div align="center"><img src="https://i0.wp.com/math.ucr.edu/home/baez/networks/circuit_made_of_resistors_black_boxed.png" /></div>
<p>hiding the circuit&#8217;s internal details and letting us see only how it acts as viewed &#8216;from outside&#8217;.</p>
<p>For more, see the lecture notes here:</p>
<p>&bull; <a href="https://johncarlosbaez.wordpress.com/2014/10/20/network-theory-part-32/">Network theory (part 32)</a>.</p>
<p><a href="http://johncarlosbaez.wor" rel="nofollow">http://johncarlosbaez.wor</a></p>
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