<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Bound Charge on gdpark.blog</title><link>https://gdpark.blog/tags/bound-charge/</link><description>Recent content in Bound Charge on gdpark.blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Wed, 19 Nov 2014 00:00:00 +0000</lastBuildDate><atom:link href="https://gdpark.blog/tags/bound-charge/index.xml" rel="self" type="application/rss+xml"/><item><title>Bound Charge Density [Electromagnetism I Studied #11]</title><link>https://gdpark.blog/posts/electromagnetism-11-bound-charge-density/</link><pubDate>Tue, 18 Nov 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-11-bound-charge-density/</guid><description>Working through why σ_b = P·n̂ and ρ_b = −∇·P actually make sense, using a hands-on geometric argument about sliced-up polarized volumes.</description></item><item><title>Electric Displacement [Electromagnetism I Studied #12]</title><link>https://gdpark.blog/posts/electromagnetism-12-electric-displacement/</link><pubDate>Wed, 19 Nov 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-12-electric-displacement/</guid><description>We define the electric displacement vector D to neatly separate the total electric field from polarization effects inside a dielectric — turns out it plays really nicely with Gauss&amp;rsquo;s law!</description></item></channel></rss>