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The physical pendulum is any rigid body of irregular shape that oscillates attached to a string from a fixed point called the pivot. The center of gravity of the pendulum’s mass will be directly below the pivot. Our Physical Pendulum Calculator will help you calculate the frequency and time period of the Physical Pendulum.
In a simple pendulum, we consider the mass to be a point mass hanging at the end of a massless string, whereas this idealized system doesn’t work so well for any real pendulum.
So, if we assume the angular displacement of the physical pendulum is assumed to be small, we can consider the pendulum’s motion to be simple harmonic motion and then calculate the frequency and time period.
Using the physical pendulum calculator, you can calculate the angular frequency, frequency, and periods of the physical pendulum.
The variables in the calculator include
Mass (m) The mass of the object at the end of the string.
Distance (d) The distance from the center of gravity to the pivot point.
Moment of inertia (I) The body’s rotational inertia describes how easy or difficult it is to rotate a body about a given axis.
Angular Frequency (ω) Angular frequency of the simple pendulum
Frequency (f) Frequency of the simple pendulum
Period (T) Period of the simple pendulum
A physical pendulum is an irregularly shaped rigid body that oscillates back and forth, hanging from the end of a string connected to a fixed point called the pivot.
The gravitational force acts at the center of mass of the physical pendulum, which will be directly below the pivot at equilibrium.
When the rigid body is pushed or pulled to one side and released, it oscillates back and forth about its equilibrium position. The torque due to the weight of the object is given by
The negative sign indicates that the torque will be in the opposite direction to the displacement of the object. If the object is pushed clockwise, then the torque will be counterclockwise. If the object is pushed counterclockwise, then the torque will be clockwise.
The motion resulting from the torque is not simple harmonic motion because the torque is proportional to sinθ. But, if θ is a very small value, we can approximate sinθ as θ. The measure of the angle will be in radians in this case.
The Angular frequency of the physical pendulum is calculated using the following formula
m → Mass of the rigid body
d → Distance from pivot to center of gravity
g → Acceleration due to gravity
I → Moment of Inertia, about the axis of rotation from the pivot point
The frequency (f) of the physical pendulum is calculated using the following formula
ω → Angular Frequency
m → Mass of the rigid body
d → Distance from pivot to center of gravity
g → Acceleration due to gravity
I → Moment of Inertia, about the axis of rotation from the pivot point
The Period (T) of a physical pendulum is calculated using the following formula
ω → Angular Frequency
m → Mass of the rigid body
d → Distance from pivot to center of gravity
g → Acceleration due to gravity
I → Moment of Inertia, about the axis of rotation from the pivot point
A physical pendulum’s length and moment of inertia—a measurement of a body’s resistance to rotational motion—determine its oscillation period. The oscillation period is longer for pendulums with a greater moment of inertia and longer lengths.
A physical pendulum’s oscillation period is independent of the angular displacement from its equilibrium position.
A physical pendulum’s period of oscillation differs from a basic pendulum’s because the length and moment of inertia of a physical pendulum determine its oscillation period. In contrast, a simple pendulum’s length and gravitational acceleration determine its oscillation period.
We can measure the acceleration due to gravity by using a physical pendulum using the following formula
m → Mass of the rigid body
d → Distance from pivot to center of gravity
g → Acceleration due to gravity
I → Moment of Inertia, about the axis of rotation from the pivot point
T → period of oscillation of the physical pendulum
Some examples of physical pendulums are rod, disk, spherical, and conical pendulums. These are often used in physics experiments and demonstrations to study the properties of oscillations and motion.

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