Skip to main content
Library homepage
 

Text Color

Text Size

 

Margin Size

 

Font Type

Enable Dyslexic Font
Mathematics LibreTexts

15.6: Moments and Centers of Mass

( \newcommand{\kernel}{\mathrm{null}\,}\)

This section shows how to calculate the masses and moments of two- and three- dimensional objects in Cartesian (x,y,z) coordinates.

Mass

We saw before that the double integral over a region of the constant function 1 measures the area of the region. If the region has uniform density 1, then the mass is the density times the area which equals the area. What if the density is not constant. Suppose that the density is given by the continuous function

Density=ρ(x,y).

In this case we can cut the region into tiny rectangles where the density is approximately constant. The area of mass rectangle is given by

Mass=(Density)(Area)=(ρ(x,y))(ΔxΔy)

You probably know where this is going. If we add all to masses together and take the limit as the rectangle size goes to zero, we get a double integral.

Definition: Mass of a Two-Dimensional lamina

Let ρ(x,y) be the density of a lamina (flat sheet) R at the point (x,y). Then the total mass of the lamina is the double integral

Masslamina=ρ(x,y)dydx

or written as an integral over an area (A):

Masslamina=baρdA

Example 15.6.1

A rectangular metal sheet with 2<x<5 and 0<y<3 has density function

ρ(x,y)=x+y.

Set up the double integral that gives the mass of the metal sheet.

Solution

We just have to evaluate the integral in Equation ???

5230(x+y)dydx.

Extending this to three-dimensional solids requires redefining ρ(x,y,z) to be the density (mass per unit volume) of an object occupying a region D in space. The integral over D gives us the mass of the object. To see why, imagine partitioning the object into n mass elements. And when summing these mass elements up, it is the total mass.

M=limnnk=1Δmk=limnnk=1ρ(xk,yk,zk)ΔVk=baρ(x,y,z)dV.

The integral of ρ(x,y,z) gives us the mass of the object.

Definition: Mass of a Three-Dimensional Solid

Let ρ(x,y,z) be the density of a solid R at the point (x,y,s). Then the total mass of the solid is the triple integral

Masssolid=ρ(x,y,z)dydx,dz

or written as an integral over an volume (V):

Masssolid=baρdV

Moments and Center of Mass

The moments about an axis are defined by the product of the mass times the distance from the axis.

Mx=(Mass(y))

My=(Mass(x))

If we have a region R with density function ρ(x,y), then we do the usual thing. We cut the region into small rectangles for which the density is constant and add up the moments of each of these rectangles. Then take the limit as the rectangle size approaches zero. This will give us the total moment.

Definition: Moments of Mass and Center of Mass

Suppose that ρ(x,y) is a continuous density function on a lamina R. Then the moments of mass are

Mx=1020k(x2+y2)ydydx

and

My=1020k(x2+y2)xdydx

and if M is the mass of the lamina, then the center of mass is

(ˉx,ˉy)=(MyM,MxM).

Example 15.6.2

Set up the integrals that give the center of mass of the rectangle with vertices (0,0), (1,0), (1,1), and (0,1) and density function proportional to the square of the distance from the origin. Use a calculator or computer to evaluate these integrals.

Solution

The mass is given by

M=1020k(x2+y2)dydx=2k3.

The moments are given by (definition 2a):

Mx=1020k(x2+y2)ydydx

and

My=1020k(x2+y2)xdydx.

These evaluate to

Mx=5k12

and

My=5k12.

It should not be a surprise that the moments are equal since there is complete symmetry with respect to x and y. Finally, we divide to get

(x,y)=(58,58).

This tells us that the metal plate will balance perfectly if we place a pin at (58,58).

Moments of Inertia

We often call Mx and My the first moments. They have first powers of y and x in their definitions and help find the center of mass. We define the moments of inertia (or second moments) by introducing squares of y and x in their definitions. The moments of inertia help us find the kinetic energy in rotational motion. Below is the definition

Definition: Moments of Inertia

Suppose that ρ(x,y) is a continuous density function on a lamina R. Then the moments of inertia are

Ix=Rρ(x,y)y2dydx

Iy=Rρ(x,y)x2dydx.

Exercise 15.6.1

Find the moments of inertia for the square metal plate in Example 15.6.2.

First Moment

The first moment of a 3-D solid region D about a coordinate plane is defined as the triple integral over D of the distance from a point (x,y,z) in D to the plane multiplied by the density of the solid at that point. First moments about the coordinate planes:

M(yz)=baδxdV

M(xz)=baδydV

M(xy)=baδzdV

The first moment about the y-axis is the double integral over the region R forming the 2-D plate of the distance from the axis multiplied by the density.

M(y)=baδxdV

M(x)=baδydV

Center of Mass

We defined center of mass located in ˉx,ˉy,ˉz. Then it is found from the first moments:

ˉx=M(y)M

ˉy=M(x)M.

Contributors and Attributions

  • Shengqiao Luo (UCD)
  • Integrated by Justin Marshall.


15.6: Moments and Centers of Mass is shared under a CC BY-NC-SA license and was authored, remixed, and/or curated by LibreTexts.

Support Center

How can we help?