<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom" xmlns:content="http://purl.org/rss/1.0/modules/content/"><channel><title>Rocket Equation on Martin‘s Physics Club</title><link>https://martinphysics.club/tags/rocket-equation/</link><description>Recent content in Rocket Equation on Martin‘s Physics Club</description><generator>Hugo</generator><language>en-US</language><copyright>2020-2026 martinphysics.club</copyright><lastBuildDate>Sat, 03 Apr 2021 17:19:03 +0000</lastBuildDate><atom:link href="https://martinphysics.club/tags/rocket-equation/index.xml" rel="self" type="application/rss+xml"/><item><title>从牛顿第二定律到火箭运动方程</title><link>https://martinphysics.club/posts/wp-100010/</link><pubDate>Sat, 03 Apr 2021 17:19:03 +0000</pubDate><guid>https://martinphysics.club/posts/wp-100010/</guid><description>&lt;p&gt;从牛顿第二定律出发，由加速度、动量的定义可以得出动量定理：&lt;/p&gt;
&lt;span class="math-expression" data-display="true"&gt; F=m\frac{dv}{dt}\Rightarrow\Delta p=F\Delta t&lt;/span&gt;
&lt;p&gt;假设变质量时仍然满足动量定理，讨论合外力为0的简单条件下得出动量守恒定律：&lt;/p&gt;
&lt;span class="math-expression" data-display="true"&gt;\Delta p=0&lt;/span&gt;
&lt;p&gt;对火箭，设箭体的对地速度为v，喷射气体对地速度为u，建立变质量动量守恒有：&lt;/p&gt;</description></item></channel></rss>