# 6. Moments of Inertia by Integration

by M. Bourne

The **moment of inertia** is a measure of the resistance of a rotating body to a change in motion.

The moment of inertia of a particle of mass *m *rotating about a particular point is given by:

`"Moment of inertia" = md^2`

where *d* is the radius of rotation.

## Inertia for a Collection of Particles

If a group of particles with masses *m*_{1}, *m*_{2},* m*_{3}, ... , *m*_{n} is rotating around a point with distances *d*_{1}, *d*_{2}, *d*_{3}, ... *d*_{n}, (respectively) from the point, then the moment of inertia *I* is given by:

I=m_{1}d_{1}^{2 }+m_{2}d_{2}^{2 }+m_{3}d_{3}^{2}+... +m_{n}d_{n}^{2}

If we wish to place all the masses at the one point (*R *units from the point of rotation) then

d_{1}=d_{2}=d_{3}= ... =d_{n }=Rand we can write:

I= (m_{1}+m_{2}+m_{3}... +m_{n})R^{2}

*R* is called the **radius of gyration.**

### Example 1

Find the moment of inertia and the radius of gyration w.r.t. the origin (0,0) of a system which has masses at the points given:

Mass |
`6` | `5` | `9` | `2` |

Point |
`(-3, 0)` | `(-2, 0)` | `(1, 0)` | `(8, 0)` |

Answer

The moment of inertia is:

I= 6(-3)^{2}+ 5(-2)^{2}+ 9(1)^{2}+ 2(8)^{2}= 54 + 20 + 9 + 128

= 211

To find *R*, we use:

I= (m_{1}+m_{2}^{ }+m_{3}... +m_{n})R^{2}

211 = (6 + 5 + 9 + 2)

R^{2}

So `R ≈ 3.097`

This means a mass of `22` units placed at `(3.1, 0)` would have the same rotational inertia about O as the 4 objects.

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**Moment of Inertia for Areas**

We want to find the moment of inertia, *I*_{y} of the given area, which is rotating around the *y*-axis.

Each "typical" rectangle indicated has width *dx* and height *y*_{2} − *y*_{1}, so its area is (*y*_{2} − *y*_{1})*dx*.

If *k* is the mass per unit area, then each typical rectangle has mass *k*(*y*_{2} −* y*

_{1})

*.*

*dx*The moment of inertia for each typical rectangle is [*k*(*y*_{2} −* y*

_{1})

*]*

*dx**x*

^{2}, since each rectangle is

*x*units from the

*y*-axis.

We can add the moments of inertia for all the typical rectangles making up the area using integration:

`I_y=kint_a^bx^2(y_2-y_1)dx`

Using a similar process that we used for the collection of particles above, the radius of gyration *R*_{y} is given by:

`R_y=sqrt((I_y)/m`

where *m* is the mass of the area.

### Example 2

For the first quadrant area bounded by the curve

`y = 1 − x^2`,

find:

a) The moment of inertia w.r.t the *y* axis. (*I*_{y})

b) The mass of the area

c) Hence, find the radius of gyration

Answer

As usual, first we sketch the part of the curve in the first quadrant. It's a parabola, passing through (1, 1) and (0, 1). A "typical" rectangle is shown.

In this example,

`y_2= 1 − x^2`, and `y_1= 0`, `a = 0` and `b = 1`.

a) Finding *I*_{y}:

`I_y=k int_a^b x^2(y_2-y_1) dx`

`=k int_0^1x^2 [(1-x^2)-(0)] dx`

`=k int_0^1 [x^2-x^4] dx`

`=k[(x^3)/(3) - (x^5)/(5)]_0^1`

`=k(1/3-1/5)`

`= (2k)/15`

b) The **mass **of the area, *m*.

Now *m* = *kA*, where *A* is the area.

Now

`A=int_0^1 (1-x^2) dx`

`=[x-(x^3)/(3)]_0^1`

`=1-1/3`

` = 2/3`

So `m = kA = (2k)/3`

c) The **radius of gyration:**

`R_y=sqrt{(I_y)/(m)}`

`=sqrt{(2k//15)/(2k//3)}`

`=sqrt[1/5]`

` approx 0.447`

This means that if a mass of `(2k)/3` was placed `0.447` units from the `y`-axis, this would have the same **moment of inertia** as the original shape.

## Rotation about the *x*-axis

For rotation about the *x*-axis, the moment of inertia formulae become:

`I_x=kint_c^(d)y^2(x_2-x_1)dy`

and

`R_x=sqrt((I_x)/m`

### Example 3

Find the moment of inertia and the radius of gyration for the area `y=x^2+1` from `x=1` to `x=2`, and `y>1`, when rotated around the *x*-axis. The mass per unit area is `3` kg m^{−2}.

Answer

We sketch the parabola. The shaded area is the part that's rotating around the `x`-axis, and we have indicated a "typical" rectangle.

In this example, we are rotating the area around the `x`-axis. We need to express our function in terms of `y`.

Since we started with `y=x^2+1`, we solve for `x` and obtain:

`x=sqrt(y-1)`

We take the positive case only, as we are dealing with the first quadrant.

So the required values which we can use in the formula are:

`x_2= 2` (the "curve" furthest from the `y`-axis),

`x_1= sqrt(y-1)` (the curve closest to the `y`-axis), and

`c = 1` and `d = 5`; and `k=3`.

a) Finding *I*_{x}:

`I_x=k int_c^d y^2(x_2-x_1) dy`

`=3 int_1^5 y^2 [(2) - sqrt(y-1)] dy`

`=3 int_2^5 (2 y^2 - y^2 sqrt(y-1)) dy`

We use a computer algebra system to obtain:

`=45.5` kg m

^{2}

b) Now to find the **mass **of the area, *m*.

*m* = *kA*, where *A* is the area.

Now

`A=int_1^2 (x^2+1) dx - 1` (We need to subtract the area of the `1xx1=1` square below the shaded area.)

`=[(x^3)/(3)+x]_1^2 - 1`

`=(8/3+2)-(1/3+1) - 1`

` = 7/3`

So `m = kA = 3xx7/3 = 7` kg

c) The **radius of gyration:**

`R_x=sqrt{(I_x)/(m)}`

`=sqrt{(45.5)/(7)}`

` ~~ 2.6` m

This means that if a single mass of `7` kg was placed `2.6` m from the `x`-axis, this would have the same **moment of inertia** as the original shape when rotating around the `x`-axis.

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