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      <title>The Nyquist Stabilty Criterion revisited</title>
      <link>https://rootloc.us/posts/nyquist/</link>
      <pubDate>Sat, 12 Nov 2022 00:00:00 +0000</pubDate>
      <guid>https://rootloc.us/posts/nyquist/</guid>
      <description>The Nyquist criterion is one of the most powerful tools in classical Control Theory, but if not properly understood it might be &amp;ldquo;hard&amp;rdquo; to remember, at least, it was for me.&#xA;Let&amp;rsquo;s look at the formula:&#xA;$$\boxed{N=Z-P}$$&#xA;Where:&#xA;$N$ is the number encirclement of the critical point $-1$. We count positively the clockwise encirclement and negatively the counterclockwise encirclements. $P$ is the number of poles in the right half plane of the open loop transfer function.</description>
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      <title>Mass-Spring-Damper 101</title>
      <link>https://rootloc.us/posts/mass_spring_damper_101/</link>
      <pubDate>Mon, 01 Jan 0001 00:00:00 +0000</pubDate>
      <guid>https://rootloc.us/posts/mass_spring_damper_101/</guid>
      <description>The model of the Mass-Spring-Damper system is a very simple (and yet useful) one. It can be used to understand a lot of concepts in Dynamical Systems, and to model more complex systems (like car suspensions) in a pretty accurate way.&#xA;According to Newton&amp;rsquo;s second law we can write the equation of forces in this way:&#xA;$$ m\textbf{a}=\Sigma \textbf{F} $$&#xA;The acceleration is the second derivative of our state variable x(t), $\Sigma \textbf{F}$ is the sum of the elastic force imposed by the linear spring (Hooke&amp;rsquo;s law), the viscous damping force imposed by the linear damper and the input force u(t).</description>
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