<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Poisson's Equation on gdpark.blog</title><link>https://gdpark.blog/tags/poissons-equation/</link><description>Recent content in Poisson's Equation on gdpark.blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Sat, 15 Nov 2014 00:00:00 +0000</lastBuildDate><atom:link href="https://gdpark.blog/tags/poissons-equation/index.xml" rel="self" type="application/rss+xml"/><item><title>Electric Potential [Electromagnetism I Studied #3]</title><link>https://gdpark.blog/posts/electromagnetism-03-electric-potential/</link><pubDate>Fri, 14 Nov 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-03-electric-potential/</guid><description>We dig into electric potential — why curl = 0 lets you define a scalar potential, how E = -∇V falls out of that, and a sneak peek at Poisson&amp;rsquo;s equation~</description></item><item><title>Laplace's Equation [Electromagnetism I Studied #6]</title><link>https://gdpark.blog/posts/electromagnetism-06-laplace-s-equation/</link><pubDate>Sat, 15 Nov 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-06-laplace-s-equation/</guid><description>Chapter 3 kicks off with Poisson&amp;rsquo;s and Laplace&amp;rsquo;s equations — what you get when you plug ∇V into Gauss&amp;rsquo;s law and let the charge density go to zero.</description></item></channel></rss>