<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Boltzmann on gdpark.blog</title><link>https://gdpark.blog/tags/boltzmann/</link><description>Recent content in Boltzmann on gdpark.blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Sat, 23 Apr 2016 00:00:00 +0000</lastBuildDate><atom:link href="https://gdpark.blog/tags/boltzmann/index.xml" rel="self" type="application/rss+xml"/><item><title>Gibbs' Expression for the Entropy [Thermal &amp; Statistical Mechanics I Studied #26]</title><link>https://gdpark.blog/posts/thermal-statistical-26-gibbs-expression-for-the-entropy/</link><pubDate>Thu, 07 Jan 2016 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/thermal-statistical-26-gibbs-expression-for-the-entropy/</guid><description>A casual (and slightly reluctant) walkthrough of Gibbs&amp;rsquo; entropy formula, showing how entropy gets re-expressed through probability over macrostates and microstates.</description></item><item><title>Relationship Between the Partition Function and State Functions [Thermal &amp; Statistical Mechanics I Studied #34]</title><link>https://gdpark.blog/posts/thermal-statistical-34-relationship-between-the-partition-function-and-state-functi/</link><pubDate>Sat, 23 Apr 2016 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/thermal-statistical-34-relationship-between-the-partition-function-and-state-functi/</guid><description>We derive thermodynamic state functions like U, F, and S straight from the partition function Z — turns out one sneaky differential trick does all the heavy lifting!</description></item></channel></rss>