<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Topology on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/topology/</link><description>Recent content in Topology on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Thu, 11 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/topology/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (6): Smooth Manifolds — Geometry Beyond Embedded Surfaces</title><link>https://www.chenk.top/en/differential-geometry/06-smooth-manifolds/</link><pubDate>Thu, 11 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/06-smooth-manifolds/</guid><description>&lt;p>The first five chapters of this series lived inside &lt;span class="math-inline">$\mathbb{R}^3$&lt;/span>
. We had curves and surfaces, parametrized explicitly, with all the geometric data — first and second fundamental forms, principal curvatures, Christoffel symbols, the Theorema Egregium, Gauss-Bonnet — built up from coordinates we could write down. The Theorema Egregium revealed that the intrinsic story can be told without reference to the embedding. But &amp;ldquo;without reference to the embedding&amp;rdquo; still meant &amp;ldquo;the embedding exists; we just choose not to use it.&amp;rdquo;&lt;/p></description></item><item><title>Differential Geometry (5): The Gauss-Bonnet Theorem — Where Geometry Meets Topology</title><link>https://www.chenk.top/en/differential-geometry/05-gauss-bonnet/</link><pubDate>Tue, 09 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/05-gauss-bonnet/</guid><description>&lt;p>The Theorema Egregium of the previous chapter showed that Gaussian curvature is intrinsic — bend a surface without stretching and &lt;span class="math-inline">$K$&lt;/span>
 does not change. The Gauss-Bonnet theorem, which we develop here, says something equally remarkable in a different direction: integrate &lt;span class="math-inline">$K$&lt;/span>
 over a closed surface and you get a topological invariant. The total curvature of any sphere is &lt;span class="math-inline">$4\pi$&lt;/span>
. The total curvature of any torus is &lt;span class="math-inline">$0$&lt;/span>
. The total curvature of a double torus is &lt;span class="math-inline">$-4\pi$&lt;/span>
. These facts are blind to the specific geometry — bend, twist, or smoosh the surface as you please, the total curvature does not change.&lt;/p></description></item></channel></rss>