<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Connections on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/connections/</link><description>Recent content in Connections on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Fri, 19 Nov 2021 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/connections/index.xml" rel="self" type="application/rss+xml"/><item><title>Differential Geometry (10): Riemannian Geometry — Metrics, Connections, and Parallel Transport</title><link>https://www.chenk.top/en/differential-geometry/10-riemannian-geometry/</link><pubDate>Fri, 19 Nov 2021 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/differential-geometry/10-riemannian-geometry/</guid><description>&lt;p>Up to this point in the series we have studied smooth manifolds with their differentiable structure: charts, tangent vectors, differential forms, exterior calculus, integration. None of this required a notion of &lt;em>distance&lt;/em>. We could differentiate functions, integrate top-degree forms, decide whether a distribution is integrable — all without ever measuring how long a curve is or what angle two tangent vectors make. The smooth structure is purely topological-with-derivatives. To do &lt;em>geometry&lt;/em> in the classical sense — to measure, to compare, to speak of curvature, to recover the everyday meanings of &amp;ldquo;length&amp;rdquo; and &amp;ldquo;angle&amp;rdquo; — we need additional structure.&lt;/p></description></item></channel></rss>