Linearisation of the pendulum about its two equilibria (Q1618): Difference between revisions

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\\theta\\approx 0:\\ \\ \\frac{d^{2}\\theta}{dt^{2}}+\\frac{g}{L}\\theta=0;\\qquad \\phi=\\theta-\\pi\\approx 0:\\ \\ \\frac{d^{2}\\phi}{dt^{2}}-\\frac{g}{L}\\phi=0
 
Property / LaTeX source: \\theta\\approx 0:\\ \\ \\frac{d^{2}\\theta}{dt^{2}}+\\frac{g}{L}\\theta=0;\\qquad \\phi=\\theta-\\pi\\approx 0:\\ \\ \\frac{d^{2}\\phi}{dt^{2}}-\\frac{g}{L}\\phi=0 / rank
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Property / instance of
 
Property / instance of: mathematical expression / rank
 
Normal rank
Property / LaTeX source
 
\\theta\\approx 0:\\ \\ \\frac{d^{2}\\theta}{dt^{2}}+\\frac{g}{L}\\theta=0;\\qquad \\phi=\\theta-\\pi\\approx 0:\\ \\ \\frac{d^{2}\\phi}{dt^{2}}-\\frac{g}{L}\\phi=0
Property / LaTeX source: \\theta\\approx 0:\\ \\ \\frac{d^{2}\\theta}{dt^{2}}+\\frac{g}{L}\\theta=0;\\qquad \\phi=\\theta-\\pi\\approx 0:\\ \\ \\frac{d^{2}\\phi}{dt^{2}}-\\frac{g}{L}\\phi=0 / rank
 
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Latest revision as of 13:26, 3 September 2026

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Linearisation of the pendulum about its two equilibria
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    \\theta\\approx 0:\\ \\ \\frac{d^{2}\\theta}{dt^{2}}+\\frac{g}{L}\\theta=0;\\qquad \\phi=\\theta-\\pi\\approx 0:\\ \\ \\frac{d^{2}\\phi}{dt^{2}}-\\frac{g}{L}\\phi=0
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