Answer:
[tex] I = \frac{mgd}{4\pi^{2}f^{2}} [/tex]
Explanation:
The moment of inertia (I) of the pendulum can be found using the following equation:
[tex] T = 2\pi\sqrt{\frac{I}{mgd}} [/tex]
Where:
T: is the period of the pendulum
m: is the pendulum's mass
g: is the gravity
d: is the distance of the pivot from the center of mass
Solving the above equation for I:
[tex] I = \frac{T^{2}*mgd}{(2\pi)^{2}} [/tex] (1)
We have that the pendulum moves in simple harmonic motion with a frequency f, and this f is equal to:
[tex] f = \frac{1}{T} \rightarrow T = \frac{1}{f} [/tex]
By entering T into equation (1) we have:
[tex] I = \frac{T^{2}*mgd}{(2\pi)^{2}} [/tex]
[tex] I = \frac{(1/f)^{2}*mgd}{(2\pi)^{2}} [/tex]
[tex] I = \frac{mgd}{4\pi^{2}f^{2}} [/tex]
Therefore, the moment of inertia of the pendulum about the pivot point is [tex] I = \frac{mgd}{4\pi^{2}f^{2}} [/tex].
I hope it helps you!