<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>RLC Circuit on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/rlc-circuit/</link><description>Recent content in RLC Circuit on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Fri, 29 Mar 2024 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/rlc-circuit/index.xml" rel="self" type="application/rss+xml"/><item><title>Ordinary Differential Equations (17): Physics and Engineering Applications</title><link>https://www.chenk.top/en/ode/17-physics-engineering-applications/</link><pubDate>Fri, 29 Mar 2024 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/ode/17-physics-engineering-applications/</guid><description>&lt;p>&lt;strong>Differential equations are not a pure mathematical game — they are the language for understanding the physical world.&lt;/strong> From celestial motion to circuit response, from a swinging pendulum to vortex shedding behind a bridge cable, every dynamical system &amp;ldquo;speaks&amp;rdquo; ODE.&lt;/p>
&lt;p>This chapter is a deliberate tour through five canonical applications. Each one will pay back the entire ODE toolkit we built in chapters 1-16: phase planes, eigenvalues, Laplace transforms, modal analysis, conservation laws, numerical integration, control. None of the examples is a &amp;ldquo;toy&amp;rdquo; — they are all genuine working physics, written tightly so that the structure remains visible.&lt;/p></description></item><item><title>Ordinary Differential Equations (3): Higher-Order Linear Theory</title><link>https://www.chenk.top/en/ode/03-linear-theory/</link><pubDate>Fri, 04 Aug 2023 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/ode/03-linear-theory/</guid><description>&lt;p>&lt;strong>A first-order ODE has memory of one number; a second-order ODE has memory of two.&lt;/strong> That tiny extra degree of freedom is what lets the same equation describe a plucked guitar string, the suspension of your car, the L-C tank circuit inside an FM radio, and the swaying of a tall building in the wind. In every case the same three regimes appear — oscillate, return-with-a-touch-of-overshoot, or crawl back — and the same algebraic gadget, the &lt;em>characteristic equation&lt;/em>, predicts which one happens.&lt;/p></description></item></channel></rss>