1. 7.5 Moments, Centers of Mass And Centroids

2. If the forces are all gravitational, then If the net torque is zero, then the system will balance. Since gravity is the same throughout the system, we could factor g out of the equation. This is called the moment about the origin. If we divide M o by the total mass, we can find the center of mass (balance point.)

3. For a thin rod or strip:  = density per unit length moment about origin: (  is the Greek letter delta.) mass: center of mass: For a rod of uniform density and thickness, the center of mass is in the middle.

4. x y strip of mass dm For a two dimensional shape, we need two distances to locate the center of mass. distance from the y axis to the center of the strip distance from the x axis to the center of the strip x tilde (pronounced ecks tilda) Moment about x-axis:Moment about y-axis:Mass:Center of mass:

5. x y For a two dimensional shape, we need two distances to locate the center of mass. Vocabulary: center of mass= center of gravity= centroid constant density  = homogeneous= uniform For a plate of uniform thickness and density, the density drops out of the equation when finding the center of mass.

6. coordinate of centroid = (2.25, 2.7)

7. Note: The centroid does not have to be on the object. If the center of mass is obvious, use a shortcut: square rectangle circle right triangle

8. We can find the centroid of a semi-circular surface by using the Theorems of Pappus and working back to get the centroid.

9. Examples Find the mass of a rod that has a length of 5 meters and whose density is given by at a distance of x meters away from the left end

10. Continuous Mass Density Instead of discrete masses arranged along the x-axis, suppose there is an object lying on the x-axis between x = a and x = b –Divide it into n pieces of length Δx –On each piece the density is nearly constant so the mass of each piece is given by density times the length –Mass of i th piece is