courses:phy101l:2
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2. Gravitational acceleration from a pendulum
1. Introduction and theory
For a simple pendulum
$$ T = 2\pi \sqrt{\frac{L}{g}} \Rightarrow g = 4\pi^2 \frac{L}{T^2}. $$
For a compound pendulum
$$ T = 2\pi \sqrt{\frac{K^2/l+l}{g}} $$
and, hence, a compound pendulum is equivalent to a simple pendulum if
$$ L = \frac{K^2}{l} + l \Rightarrow l^2 - lL + K^2 = 0 $$
which is a quadratic equation with two solutions $l_1$ and $l_2$ where $l_1+l_2=L$ and $l_1l_2=K^2$.
2. Method and data
3. Graphical analysis
4. Results
5. Discussion and conclusion
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