Compound pendulum experiment to find the acceleration due to gravity

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SUMMARY

The discussion focuses on the compound pendulum experiment to determine the acceleration due to gravity, specifically analyzing the relationship between the time period and the distance from the point of oscillation. The time period initially decreases and then increases steeply due to the interplay between torque and rotational inertia. When the pendulum is suspended at its center of gravity, the time period approaches infinity because there is no net torque to induce oscillation. The moment of inertia, described by the formula I = (1/3) * M * L * (L^3/4 + 3Lx^2), is parabolic in relation to the distance from the center, influencing the pendulum's behavior.

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  • Understanding of compound pendulum mechanics
  • Familiarity with torque and rotational inertia concepts
  • Knowledge of angular acceleration and its relationship to period
  • Basic grasp of pendulum dynamics and gravitational potential energy
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In this experiment, I still can't figure out why the graph between time period and distance from point of oscillation is like that. Why does it first decrease and increase so steeply? I got the second part because it goes near the centre of gravity and time period becomes almost infinite there but why does it first decrease and then increase?
 
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As a pendulum gets longer the time period gets longer, so it is clear why T should be going up at the ends. When the bar is attached at its middle at the center of gravity, there is no change in gravitational potential energy as the bar swings, so there is no reason to oscillate, so T goes to infinity. Near there, with very little net torque to make it oscillate T is very large, so it is clear why it should go up in the middle. There must be a minimum in between.

Another way to look at it is comparing the torque to the rotational inertia. The angular acceleration is inversely related to the period, and angular acceleration is torque / inertia. So you can see how the period changes by examining torque / inertia. Picture the bar tilted from vertical by some particular angle. The torque increases linearly as you move the suspension point away from the center of gravity. However, the inertia does not change linearly. If L is the total length of the rod and x is how far the suspension point is from the center, then the moment of inertia is

## \frac 1 3 \frac M L (\frac {L^3} 4 + 3 L x^2)##

Which is parabolic in x.
 
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