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2. Gravitational acceleration from a pendulum
1. Introduction and theory
For a simple pendulum
T=2π√Lg⇒g=4π2LT2.T=2π√Lg⇒g=4π2LT2.
For a compound pendulum
T=2π√K2/l+lgT=2π√K2/l+lg
and, hence, a compound pendulum is equivalent to a simple pendulum if
L=K2l+l⇒l2−lL+K2=0L=K2l+l⇒l2−lL+K2=0
which is a quadratic equation with two solutions l1l1 and l2l2 where l1+l2=Ll1+l2=L and l1l2=K2l1l2=K2.
2. Method and data
2.1 Data table
Hole no. | Distance [cm] | Trial | Time for 10 oscillations [s] |
---|---|---|---|
1 | 10 | 1 | |
2 | |||
2 | 20 | 1 | |
2 | |||
3 | 30 | 1 | |
2 | |||
4 | 40 | 1 | |
2 | |||
6 | 60 | 1 | |
2 | |||
7 | 70 | 1 | |
2 | |||
8 | 80 | 1 | |
2 | |||
9 | 90 | 1 | |
2 |
3. Graphical analysis
4. Results
5. Discussion and conclusion
courses/phy101l/2.1687018719.txt.gz · Last modified: 2023/06/17 10:18 by asad