<?xml version="1.0" encoding='utf-8'?>
<!DOCTYPE wml PUBLIC "-//WAPFORUM//DTD WML 1.1//EN" "http://www.wapforum.org/DTD/wml_1.1.xml">
<wml>
<card id="card1" title="Distributed-element model - Page 14 - Wikipedia">
<p>
<a accesskey="1" href="page.php?w=distributed-element_model&amp;p=13">1.Previous</a><br />
<a accesskey="3" href="page.php?w=distributed-element_model&amp;p=15">3.Next</a>
</p>
<p>windings and more accurate models distributed capacitance to other turns must also be considered.  This model is fairly difficult to deal with in simple calculations and, for the most part, is avoided.  The most common approach is to roll up all the distributed capacitance into one lumped element in parallel with the inductance and resistance of the coil.  This lumped model works successfully at low frequencies but falls apart at high frequencies where the usual practice is to simply measure (or specify) an overall <a href="page.php?w=Q_factor">{{mvar</a></p><p>
<a accesskey="1" href="page.php?w=distributed-element_model&amp;p=13">1.Previous</a><br />
<a accesskey="3" href="page.php?w=distributed-element_model&amp;p=15">3.Next</a>
</p>

<do type="prev" label="Search">
        <go href="search.wml"/>
</do>

</card>
</wml>
