<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Lie-Bracket on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/lie-bracket/</link><description>Recent content in Lie-Bracket on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Sat, 13 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/lie-bracket/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (7): Vector Fields, Flows, and the Lie Bracket</title><link>https://www.chenk.top/en/differential-geometry/07-vector-fields-flows/</link><pubDate>Sat, 13 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/07-vector-fields-flows/</guid><description>&lt;p>A tangent vector lives at one point. It tells you &amp;ldquo;this direction, this speed, right here, right now.&amp;rdquo; It is fundamentally local — pluck it off the manifold and it remembers nothing about its neighbors. A &lt;strong>vector field&lt;/strong>, by contrast, is what you get when you let one tangent vector at every point conspire smoothly. It is a velocity prescription on the entire manifold: stand anywhere, and the field tells you where to go. Follow the prescription, and you trace out an &lt;strong>integral curve&lt;/strong>. Follow it from every starting point at once, and you get a &lt;strong>flow&lt;/strong> — a one-parameter family of diffeomorphisms that drags the whole manifold along itself like a slow river.&lt;/p></description></item></channel></rss>