Pendulum as a first-order system (Q1617)
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| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Pendulum as a first-order system |
No description defined |
Statements
\\begin{cases}\n\\omega=\\frac{d\\theta}{dt} \\\\\n\\frac{d\\omega}{dt}=-\\frac{g}{L}\\sin\\theta\n\\end{cases}
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From equation 2 it can be inferred that equilibria is reached at $\\theta=0$ or $\\theta=\\pi$
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