<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Stokes-Theorem on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/stokes-theorem/</link><description>Recent content in Stokes-Theorem on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Wed, 17 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/stokes-theorem/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (9): Integration on Manifolds and Stokes' Theorem</title><link>https://www.chenk.top/en/differential-geometry/09-integration-stokes/</link><pubDate>Wed, 17 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/09-integration-stokes/</guid><description>&lt;p>In single-variable calculus, the fundamental theorem says that integrating a derivative over an interval equals the boundary difference: &lt;span class="math-inline">$\int_a^b f&amp;#39;(x)\,dx = f(b) - f(a)$&lt;/span>
. The &amp;ldquo;boundary&amp;rdquo; of &lt;span class="math-inline">$[a, b]$&lt;/span>
 is the two-point set &lt;span class="math-inline">$\{a, b\}$&lt;/span>
, with &lt;span class="math-inline">$b$&lt;/span>
 counted positively and &lt;span class="math-inline">$a$&lt;/span>
 negatively. The right-hand side is the integral of &lt;span class="math-inline">$f$&lt;/span>
 over this signed boundary. The left-hand side is the integral of the derivative over the interval. This is, in essence, every &amp;ldquo;fundamental theorem&amp;rdquo; you have ever met — Green&amp;rsquo;s theorem in the plane, the divergence theorem in three dimensions, the classical Stokes&amp;rsquo; theorem on surfaces. They are all instances of one statement on manifolds: &lt;strong>the integral of &lt;span class="math-inline">$d\omega$&lt;/span>
 over &lt;span class="math-inline">$M$&lt;/span>
 equals the integral of &lt;span class="math-inline">$\omega$&lt;/span>
 over &lt;span class="math-inline">$\partial M$&lt;/span>
&lt;/strong>.&lt;/p></description></item></channel></rss>