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In a pendulum, why is the small angle approximation used, even though large angles are involved?
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The approximation \(\cos \theta \approx 1- \Large \frac {\theta ^2}{2}\) leading to a linear differential equation is valid to 1% up to \(\theta = 0.7\, rad = 40°\) Usually, 'small' amplitude is kept within 20°, so there is no problem.
Are there similar bounds for\[\sin \theta= \theta\]?
Oh, you can derive one from the other. Thank you
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