<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Curvature on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/curvature/</link><description>Recent content in Curvature on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Fri, 05 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/curvature/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (3): The Shape Operator — Curvature of Surfaces</title><link>https://www.chenk.top/en/differential-geometry/03-second-form-curvature/</link><pubDate>Fri, 05 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/03-second-form-curvature/</guid><description>&lt;p>The previous article gave us the intrinsic apparatus: the first fundamental form &lt;span class="math-inline">$\mathrm{I}$&lt;/span>
, encoded as the symmetric matrix &lt;span class="math-inline">$\begin{pmatrix}E &amp;amp; F \\ F &amp;amp; G\end{pmatrix}$&lt;/span>
. With it, an ant on the surface can measure lengths, angles, and areas without ever leaving. What an ant on a cylinder cannot do, equipped only with &lt;span class="math-inline">$\mathrm{I}$&lt;/span>
, is detect that the cylinder is bent. The cylinder has the same first fundamental form as the plane, yet sits very differently in &lt;span class="math-inline">$\mathbb{R}^3$&lt;/span>
.&lt;/p></description></item></channel></rss>