<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Signal Processing on Chen Kai Blog</title><link>https://www.chenk.top/en/tags/signal-processing/</link><description>Recent content in Signal Processing on Chen Kai Blog</description><generator>Hugo</generator><language>en</language><lastBuildDate>Wed, 19 Mar 2025 09:00:00 +0000</lastBuildDate><atom:link href="https://www.chenk.top/en/tags/signal-processing/index.xml" rel="self" type="application/rss+xml"/><item><title>Essence of Linear Algebra (12): Sparse Matrices and Compressed Sensing — Less Is More</title><link>https://www.chenk.top/en/linear-algebra/12-sparse-matrices-and-compressed-sensing/</link><pubDate>Wed, 19 Mar 2025 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/linear-algebra/12-sparse-matrices-and-compressed-sensing/</guid><description>&lt;p>&lt;figure class="article-figure">
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&lt;h2 id="the-less-is-more-miracle" class="heading-anchor">The &amp;ldquo;Less Is More&amp;rdquo; Miracle&lt;a href="#the-less-is-more-miracle" class="heading-link" aria-label="Permalink to this section" title="Copy link to this section">#&lt;/a>
&lt;/h2>&lt;p>A raw 24-megapixel photograph weighs in at roughly 70 MB. JPEG compresses it to a few hundred kilobytes — a 100&lt;span class="math-inline">$\times$&lt;/span>
reduction — and you cannot tell the difference. A traditional MRI scan takes thirty minutes; a modern compressed sensing MRI gets the same image in five.&lt;/p></description></item><item><title>Ordinary Differential Equations (4): The Laplace Transform</title><link>https://www.chenk.top/en/ode/04-constant-coefficients/</link><pubDate>Mon, 21 Aug 2023 09:00:00 +0000</pubDate><guid>https://www.chenk.top/en/ode/04-constant-coefficients/</guid><description>&lt;p>&lt;strong>The Laplace transform turns calculus into algebra.&lt;/strong> Instead of grinding through integration, guessing trial solutions, and bolting on initial conditions at the end, you transform the entire ODE — equation, forcing, and initial data — into a single polynomial equation in a complex variable &lt;span class="math-inline">$s$&lt;/span>
. You solve it like a high-school problem, then transform back. Along the way, the &lt;em>shape&lt;/em> of the solution becomes geometry: poles in the left half of the complex plane decay, poles on the right blow up, poles on the imaginary axis ring forever. This chapter develops that picture from first principles and connects it to the engineering tools — transfer functions, Bode plots, PID control — that made the Laplace transform the lingua franca of dynamics.&lt;/p></description></item></channel></rss>