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Moment Of Inertia Of Rectangle Section

The moment of inertia of a rectangle section or cross-section have different formulas for finding it and values as well. They depend on the location of the axis of rotation.

A moment of inertia is the resisting force experienced by any object which is under any angular torque or acceleration or motion. A rectangular section or cross-section observes any kind of moment of inertia about an axis of rotation it can be passing through the centroid of the rectangle, it can pass through its base, through a centroidal axis which is also perpendicular to the base of the rectangle. There are different MOI values for each of them. We’ll here discuss the formula for all of them and the calculation for one of the methods. And also the method discussed here will explain the moment of inertia of the rectangle by integrating the small strip of the rectangle.

Calculator of MOI of a rectangular section where the axis of rotation is edge CD of the figure

Consider a rectangular cross-section having ABCD as its vertices. Where b is the width of the section and d is the depth of the section. Consider the line or the edge CD as the axis of rotation for this section. Now, let us find the MOI about this line or the axis of rotation CD. 

Also, consider a small strip of width ‘dy’ in the rectangular section which is at a distance of value y from the axis of rotation. Involvement of this ‘dy’ will make the assumptions and calculations easier. And after finding the moment of inertia of the small strip of the rectangle we’ll find the moment of inertia by integrating the MOI of the small rectangle section having boundaries from D to A.

Now,

If we see the area of a small rectangular strip having width ‘dy’ will be

dA=dy × b

Consider a rectangular cross-section having ABCD as its vertices. Where b is the width of the section and d is the depth of the section. Consider the line or the edge CD as the axis of rotation for this section. Now, let us find the MOI about this line or the axis of rotation CD. 

Also, consider a small strip of width ‘dy’ in the rectangular section which is at a distance of value y from the axis of rotation. Involvement of this ‘dy’ will make the assumptions and calculations easier. And after finding the moment of inertia of the small strip of the rectangle we’ll find the moment of inertia by integrating the MOI of the small rectangle section having boundaries from D to A.

Now,

If we see the area of a small rectangular strip having width ‘dy’ will be

dA=dy × b

Or 

dA=bdy

And the moment of inertia of this small area dA about the axis of rotation CD according to a simple moment of inertial formula which is 

I=Mr²

Will be 

IdA=bdy × y²

Or 

IdA=by²dy

Now, 

Similar to mathematical derivations, as we found the MOI for the small rectangular strip ‘dy’ we’ll now integrate it to find the same for the whole rectangular section about the axis of rotation CD.

Therefore, the equation or moment of inertia of a rectangular section having a cross-section at its lower edge as in the figure above will be,

ICD=bd³ ⁄ 3

Let us see when we change the axis of rotation, and then how the calculation for the formula changes for it.

Formula when the axis is passing through the centroid

When the axis of rotation of a rectangle is passing through its centroid. The formula for finding the MOI of the rectangle is

I=bd³ ⁄ 12

Where,

b = width of the rectangle and

d = depth or length of the rectangle

Formula when the axis is passing through the base of the rectangle

When the axis is passing through the base of the rectangle the formula for finding the MOI is,

I=bd³ ⁄ 3

Where,

The variables are the same as above, b is the width of the rectangle and d is the depth of it.

Formula when the axis is passing through the centroid perpendicular to the base of the rectangle

In this case, the formula for the moment of inertia is given as,

I=hb³ ⁄ 12

Where,

h is the depth and b is the base of the rectangle.

Conclusion

To sum up, the formula for finding the moment of inertia of a rectangle is given by I=bd³ ⁄ 3, when the axis of rotation is at the base of the rectangle. However, when we change the location of the axis of rotation the formula as well as the value of the moment of inertia of a rectangle changes with it. There are two different methods for finding the moment of inertia of any object, that is, the parallel axis theorem and the other one is the perpendicular axis theorem.

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