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The frequency that is characteristic of a given freely oscillating system, with no applied driving force. |
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\begin{large} \[\omega_{0} = 2 \pi \nu_{0} \]\end{large} |
For a mass on a spring, the natural frequency is given by
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\begin{large} \[ \omega_{0} = \sqrt{\frac{k}{m}} \]\end{large} |
while for a simple pendulum of mass m on an arm of length L the natural frequency is
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\begin{large} \[ \omega_{0} = \sqrt{\frac{g}{L}} \]\end{large} |
See Simple Harmonic Motion for fuller details.
The natural frequencies are related to the period T by:
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\begin{large} \[ T = \frac{1}{\nu_{0}} = \frac{2 \pi}{\omega_{0}} \]\end{large} |