Parallel axis theorem and moment of inertia

In summary, using the parallel axis theorem and the equation for a rectangular plate, the moment of inertia of a thin rectangular sheet of steel with dimensions 0.30m by 0.40m and mass 0.470kg about an axis passing through one corner is 0.05021 kg * m^2.
  • #1
Edwardo_Elric
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Homework Statement


A thin rectangular sheet of steel is 0.30m by 0.40m and has mass 0.470kg. Find the moment of inertia about an axis that is perpendicular to the plane of the sheet and that passes through one corner of the sheet.


Homework Equations


Parallel axis theorem:
Ip = Icm + Md^2
Rectangular plate(but not thin):
Icm = 1/12 M(a^2 + b^2) << where a and b are the sides of the rectangle


The Attempt at a Solution



Ip = 1/12((0.30)^2 + (0.40m)^2) + (0.470kg)((0.15m)^2 + (0.20m)^2)
Ip = (0.0208333 + 0.029375)kg * m^2
Ip = 0.05021 kg * m^2
 
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  • #2
Edwardo_Elric said:

Homework Statement


A thin rectangular sheet of steel is 0.30m by 0.40m and has mass 0.470kg. Find the moment of inertia about an axis that is perpendicular to the plane of the sheet and that passes through one corner of the sheet.


Homework Equations


Parallel axis theorem:
Ip = Icm + Md^2
Rectangular plate(but not thin):
Icm = 1/12 M(a^2 + b^2) << where a and b are the sides of the rectangle


The Attempt at a Solution



Ip = 1/12((0.30)^2 + (0.40m)^2) + (0.470kg)((0.15m)^2 + (0.20m)^2)

you didn't multiply by M... 1/12M (a^2 + b^2)
 
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  • #3


The moment of inertia for a thin rectangular sheet can be found using the parallel axis theorem, which states that the moment of inertia of a body about any axis is equal to the moment of inertia about a parallel axis through the center of mass plus the product of the mass and the square of the distance between the two axes. In this case, the axis passing through one corner of the sheet is parallel to the axis passing through the center of mass, so the moment of inertia can be calculated using the formula above.

Using the given dimensions and mass, we can find the moment of inertia about the center of mass using the formula for a rectangular plate. Then, we can use the parallel axis theorem to find the moment of inertia about the axis passing through the corner.

Substituting the values into the equations, we get a moment of inertia of approximately 0.05021 kg * m^2. This value represents the resistance of the thin rectangular sheet to changes in its rotational motion about the given axis.
 

1. What is the parallel axis theorem?

The parallel axis theorem states that the moment of inertia of a body about any axis is equal to the moment of inertia about a parallel axis through the center of mass, plus the product of the mass of the body and the square of the distance between the two axes.

2. How is the moment of inertia calculated using the parallel axis theorem?

The moment of inertia using the parallel axis theorem can be calculated by adding the moment of inertia about the center of mass to the product of the mass of the body and the square of the distance between the center of mass and the axis of rotation.

3. What is the significance of the parallel axis theorem in physics?

The parallel axis theorem is significant in physics because it allows us to calculate the moment of inertia of a body about any axis, not just the center of mass. This is useful in analyzing rotational motion and calculating the torque required to rotate an object about a specific axis.

4. How does the parallel axis theorem relate to the moment of inertia of a rigid body?

The parallel axis theorem is directly related to the moment of inertia of a rigid body. It states that the moment of inertia of a body about any axis is equal to the moment of inertia about a parallel axis through the center of mass, plus an additional term that takes into account the distance between the two axes.

5. Can the parallel axis theorem be applied to all types of objects?

Yes, the parallel axis theorem can be applied to all types of objects, regardless of their shape or size. As long as the mass and distance between the two axes are known, the moment of inertia can be calculated using this theorem.

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