<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Theorema-Egregium on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/theorema-egregium/</link><description>Recent content in Theorema-Egregium on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Sun, 07 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/theorema-egregium/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (4): Intrinsic Geometry — Theorema Egregium and Geodesics</title><link>https://www.chenk.top/en/differential-geometry/04-intrinsic-geometry/</link><pubDate>Sun, 07 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/04-intrinsic-geometry/</guid><description>&lt;p>The previous two chapters set up a clear dichotomy. Chapter 2 introduced the &lt;em>first fundamental form&lt;/em> &lt;span class="math-inline">$\mathrm{I}$&lt;/span>
 — the intrinsic metric, what an ant on the surface can measure. Chapter 3 introduced the &lt;em>second fundamental form&lt;/em> &lt;span class="math-inline">$\mathrm{II}$&lt;/span>
 and the shape operator — the extrinsic data, how the surface bends in &lt;span class="math-inline">$\mathbb{R}^3$&lt;/span>
. From &lt;span class="math-inline">$\mathrm{II}$&lt;/span>
 we computed Gaussian curvature &lt;span class="math-inline">$K = \det S$&lt;/span>
 and mean curvature &lt;span class="math-inline">$H = \mathrm{tr}\,S/2$&lt;/span>
. By all appearances, both &lt;span class="math-inline">$K$&lt;/span>
 and &lt;span class="math-inline">$H$&lt;/span>
 should depend on the embedding. Bend the surface (without stretching) and you would expect both to change.&lt;/p></description></item></channel></rss>