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Consider the case of a one-dimensional harmonic ocillator. Suppose x is the displacement coordinate. It is clear that the only x Cartesian coordinate is the coordinate Only generalized. The grange is L(x,±) = T – V = m²² -kx² 2

Consider the case of a one-dimensional harmonic ocillator. Suppose x is the displacement coordinate. It is clear that the only x Cartesian coordinate is the coordinate Only generalized. The grange is L(x,±) = T – V = m²² -kx² 2

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Consider the case of a one-dimensional harmonic ocillator. Suppose x is the displacement coordinate. It is clear that the only x Cartesian coordinate is the coordinate Only generalized. The grange is L(x,£) = T – V = ¿ mt² -kx?
Transcribed Image Text:Consider the case of a one-dimensional harmonic ocillator. Suppose x is the displacement coordinate. It is clear that the only x Cartesian coordinate is the coordinate Only generalized. The grange is L(x,£) = T – V = ¿ mt² -kx?
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