What is the moment of inertia for a square rod using the parallel axis theorem?

In summary, the conversation discusses how to find the moment of inertia for a thin, uniform rod bent into a square shape. The parallel axis theorem is used to find the moment of inertia for each individual rod, and then the total moment of inertia is found by subtracting the moment of inertia calculated from the parallel axis theorem from the moment of inertia of the square. The formula for the moment of inertia of a rectangular plate is also mentioned.
  • #1
Iron Eagle
5
0
Hi all, I have run into a problem requiring the use of the parallel axis theorem. I'm kind of lost as to where to start. Can anyone help?

A thin, uniform rod is bent into a square of side length a. If the total mass is M, find the moment of inertia about an axis through the center and perpendicular to the plane of the square. Use the parallel-axis theorem.

TIA.
 
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  • #2
Treat the object as a set of four thin rods. I assume you know how to find the moment of inertia of each rod about its own center. Now use the parallel axis theorem to find the moment of inertia of each rod about the center of the square.
 
  • #3
Alright. So, first of all, you should know that the moment of inertia of a rectangular plate, axis through the center of the plate is:

I = (1/12)*M*(a^2+b^2)


1. Simply, for a square it would just be (a^2+a^2) or (2a^2)
2. Then, we find moment of inertia from the parallel-axis theorem.
3. Finally, take the moment of inertia from the parallel-axis theorem and subtract.
(so, parallel-axis - moment of inertia)
4. That's it, that should be the answer.
 

FAQ: What is the moment of inertia for a square rod using the parallel axis theorem?

What is the Parallel Axis Theorem?

The Parallel Axis Theorem is a physical law that states the moment of inertia of a rigid body about any axis parallel to its center of mass is equal to the moment of inertia about the body's center of mass plus the product of the body's mass and the square of the distance between the two axes.

How is the Parallel Axis Theorem derived?

The Parallel Axis Theorem is derived from the more general law of the moment of inertia, which states that the moment of inertia of a body is equal to the sum of the products of each particle's mass and the square of its distance from the axis of rotation. By applying this law to the specific case of a parallel axis, the Parallel Axis Theorem can be derived.

What is the significance of the Parallel Axis Theorem?

The Parallel Axis Theorem is significant because it allows for the calculation of the moment of inertia of a body about any parallel axis, rather than just the axis passing through its center of mass. This makes it a useful tool in many areas of physics, such as in the design of rotating machinery and the analysis of rotational motion.

Can the Parallel Axis Theorem be applied to all rigid bodies?

Yes, the Parallel Axis Theorem applies to all rigid bodies, regardless of their shape or size. It is a fundamental law of physics that holds true for all objects, as long as they are rigid and have a defined center of mass.

How is the Parallel Axis Theorem used in practical applications?

The Parallel Axis Theorem is used in various practical applications, including the design and analysis of rotating objects such as flywheels, gyroscopes, and propellers. It is also used in engineering and physics experiments to calculate the moment of inertia of different objects. Additionally, the Parallel Axis Theorem is used in celestial mechanics to calculate the moment of inertia of planets and other celestial bodies.

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