Rotational Inertia formula help

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To calculate the moment of inertia of a 24 kg solid door rotating about a vertical axis 17 cm from one edge, the correct formula is I = (1/12)mL^2 + m((L/2)-d)^2, where L is the length of the door and d is the distance from the edge. The center of mass for a uniformly thick door is located at its midpoint, which is L/2 from the edge. The parallel axis theorem can be applied to find the total moment of inertia by adding the inertia about the center of mass to the product of mass and the square of the distance from the center of mass to the desired axis. An alternative method involves treating the door as two separate sections and summing their individual moments of inertia. Both approaches yield the same result for the moment of inertia.
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A 24 kg solid door is 220 cm tall, 95 cm wide. What is the door's moment of inertia for rotation about a vertical axis inside the door, 17 cm from one edge?

I've looked at examples of how to do this problem. They connect it to center mass but I get confused when determining what the center mass is. They also talk about parallel axis theorem, but my professor has not introduced this approach.

The formula that I have been using is I= (1/3)mr^2
 
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If you're like me and look at other examples for help:
I was using the wrong eq. use I=(1/12)mL^2 + m (L/2 -d)^2
L is the length of the door and d is the distance from the edge
 
That looks right.

From here..
http://hedberg.ccnysites.cuny.edu/img203207/moments-wide.png

The moment of inertia about the center of mass (Icm) of the door is..
Icm = (1/12)mL2

The centre of mass will be the middle of the door (L/2 from the edge) for a door of uniform thickness.

Then the parallel axis theorem says..
I = Icm + mx2

where x is the distance between the centre of mass and the required axis. In your case x = (L/2)-d so the total moment of inertial is

I = (1/12)mL2 + m((L/2)-d)2.......(1)

Which is your equation.

You should also be able to get the same answer without using parallel axis theorem...

You could also approach this problem by pretending you had TWO doors, a narrow one (width d) and a wide one (width=L-d) connected together at a common hinge and add together the moments of inertia of each.

The moment of inertia of a door about it's edge is..
Ih = (1/3)mL2

In this case you have two doors of different width L..

The narrow one..
In = (1/3)md^2
The wide one..
Iw = (1/3)m(L-d)2

So the total moment of inertial would be..
I = In + Iw

I = (1/3)md^2 + (1/3)m(L-d)2.........(2)

I'll let you prove (1) and (2) are the same.
 
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