<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Canonical Ensemble on gdpark.blog</title><link>https://gdpark.blog/tags/canonical-ensemble/</link><description>Recent content in Canonical Ensemble on gdpark.blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Mon, 20 Jun 2016 00:00:00 +0000</lastBuildDate><atom:link href="https://gdpark.blog/tags/canonical-ensemble/index.xml" rel="self" type="application/rss+xml"/><item><title>Grand Potential [Thermal &amp; Statistical Mechanics I Studied #42]</title><link>https://gdpark.blog/posts/thermal-statistical-42-grand-potential/</link><pubDate>Sun, 19 Jun 2016 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/thermal-statistical-42-grand-potential/</guid><description>We define the grand potential Φ_G = -k_BT·ln(Z_G) by building on how F works in the canonical ensemble — because the partition function holds all the power, hehehe!</description></item><item><title>Chemical Potential of an Ideal Gas [Thermal &amp; Statistical Mechanics I Studied #43]</title><link>https://gdpark.blog/posts/thermal-statistical-43-chemical-potential-of-an-ideal-gas/</link><pubDate>Mon, 20 Jun 2016 00:00:00 +0000</pubDate><guid>https://gdpark.blog/posts/thermal-statistical-43-chemical-potential-of-an-ideal-gas/</guid><description>We derive μ = k_BT ln(nλ_th³) for an ideal gas via the canonical ensemble and Helmholtz free energy — a relation we&amp;rsquo;ll keep pulling out freely from here on.</description></item></channel></rss>