00:01
In this question there is a xy plane this is x plane and this is y plane the equilitary triangle this is equal triangle the length of the equal triangle is l and the mass is m this is made from three rods so one rod mass is capital m and one rod length is l so we can write here masses and length so this is the origin this is the origin and total mass of the frame is three times m so this is symmetric about x -axis so we are calculating the moment of inertia of the triangle about x -axis and moment of inertia of this triangle about y -axis finally we are calculating the angular momentum about y -axis so in first part we are calculating the moment of inertia about x -axis so this is first rod, second rod, and this is third rod.
01:06
So let's find out the moment of inertia.
01:08
This is sum of all the rods.
01:11
So you can see this is symmetric about x -axis.
01:14
So we are considering this length, this is y, and this distance is x.
01:21
This angle is 30 degree and this angle is 30 degree because this is equilateral triangle.
01:26
So equal to triangle is 60 degree and it is symmetric, so that's why it is half.
01:30
The value of y is equal to x this is sign 30 degree so this is small movement of inertia for rod one this is equal to y square times small mass we are considering small mass dm now and the thickness is d x so we can write the mass per unit length dm divided by d x is equal to mass divided by l so you will get the value of dm that is m divided by l times d x so if you integrate this is moment of inertia or rod 1 y square integration this is mass time divided by length times d x so we are integrating from 0 to l length so i1 is equal to this is 0 to l this is x sine 30 degrees so this is x divided by 2 square m divided by l is constant and this is d x so you so after solving integration this is x cube divided by three times four because two square is four and this is zero to l m divided by l is constant so we can write mass this is l square divided by 12 so this is the moment of inertia for rod one so it is symmetric so moment of inertia for rod two is m l square divided by 12.
03:00
Now we know that the moment of inertia for rod third because it is center point so at center this is ml square divided by 12.
03:10
So the moment of inertia about x -axis is equal to i1 plus i2 plus i3 and all values is same so we can write three times i will so this is three times ml squared divided by 12 so this is ml squared divided by 4 so moment of inertia about x -axis is ml squared divided by 4.
03:34
So this is our moment of inertia...