<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Magnetic Field on gdpark.blog</title><link>https://gdpark.blog/tags/magnetic-field/</link><description>Recent content in Magnetic Field on gdpark.blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Mon, 21 Dec 2015 00:00:00 +0000</lastBuildDate><atom:link href="https://gdpark.blog/tags/magnetic-field/index.xml" rel="self" type="application/rss+xml"/><item><title>The Biot-Savart Law [Electromagnetism I Studied #16]</title><link>https://gdpark.blog/posts/electromagnetism-16-the-biot-savart-law/</link><pubDate>Thu, 25 Dec 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-16-the-biot-savart-law/</guid><description>We &amp;lsquo;discovered&amp;rsquo; the Biot-Savart law — the equation that tells us exactly how big a magnetic field gets around a current-carrying wire, then worked through some examples hehe~</description></item><item><title>Ampère's Law [Electromagnetism I Studied #17]</title><link>https://gdpark.blog/posts/electromagnetism-17-amp-re-s-law/</link><pubDate>Fri, 26 Dec 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-17-amp-re-s-law/</guid><description>If electrostatics has Gauss&amp;rsquo;s law then magnetostatics has Ampère&amp;rsquo;s law — the line integral of B around any closed loop just equals μ₀i_in, hehe!</description></item><item><title>Ampère's Law (Part 2) [Electromagnetism I Studied #18]</title><link>https://gdpark.blog/posts/electromagnetism-18-amp-re-s-law-part-2/</link><pubDate>Sat, 27 Dec 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-18-amp-re-s-law-part-2/</guid><description>Let&amp;rsquo;s actually work through Ampère&amp;rsquo;s law problems — infinite wires, surface currents, and why symmetry is the magic keyword that makes everything ridiculously easy!</description></item><item><title>The Auxiliary Field H [Electromagnetism I Studied #21]</title><link>https://gdpark.blog/posts/electromagnetism-21-the-auxiliary-field-h/</link><pubDate>Mon, 29 Dec 2014 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/electromagnetism-21-the-auxiliary-field-h/</guid><description>Just like D handles free charges in electrostatics, H is the magnetic field due to free currents — saving us from infinite microscopic madness!</description></item><item><title>Larmor Precession and the Stern-Gerlach Experiment [Quantum Mechanics I Studied #23]</title><link>https://gdpark.blog/posts/quantum-mechanics-23-larmor-precession-and-the-stern-gerlach-experiment/</link><pubDate>Mon, 21 Dec 2015 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/quantum-mechanics-23-larmor-precession-and-the-stern-gerlach-experiment/</guid><description>A casual dive into how electrons behave in magnetic fields — covering the gyromagnetic ratio, Larmor precession, and the Stern-Gerlach experiment with tons of enthusiasm!!!!!</description></item></channel></rss>