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9.6 Center of Mass

The mass-weighted average position of a particle system or extended body, and why it accelerates as if every external force acted there.

University Physics Volume 1, 9.6 Center of Mass

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9 exercises

9.6 Exercise 1

Suppose we included the sun in the system. Approximately where would the center of mass of the Earth-moon-sun system be located? (Feel free to actually calculate it.)

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9.6 Exercise 2

Suppose you have a macroscopic salt crystal (that is, a crystal that is large enough to be visible with your unaided eye). It is made up of a huge number of unit cells. Is the center of mass of this crystal necessarily at the geometric center of the crystal?

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9.6 Exercise 3

How would the firework display change in deep space, far away from any source of gravity?

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9.6 Exercise 7

Two particles of masses m1m_{1} and m2m_{2} separated by a horizontal distance D are let go from the same height h at different times. Particle 1 starts at t=0t = 0, and particle 2 is let go at t=Tt = T. Find the vertical position of the center of mass at a time before the first particle strikes the ground. Assume no air resistance.

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9.6 Exercise 9

Two particles of masses m1m_{1} and m2m_{2} move uniformly in different circles of radii R1R_{1} andR2R_{2} about the origin in the x, y-plane. The coordinates of the two particles in meters are given as follows (z=0z = 0 for both). Here t is in seconds:
x1(t)=4cos(2t)y1(t)=4sin(2t)x2(t)=2cos(3t−π2)y2(t)=2sin(3t−π2)\begin{aligned}x_{1} \left(t\right) & = & 4 \text{cos} \left(2 t\right) \\ y_{1} \left(t\right) & = & 4 \text{sin} \left(2 t\right) \\ x_{2} \left(t\right) & = & 2 \text{cos} \left(3 t - \frac{\pi}{2}\right) \\ y_{2} \left(t\right) & = & 2 \text{sin} \left(3 t - \frac{\pi}{2}\right)\end{aligned}

  1. Find the radii of the circles of motion of both particles.
  2. Find the x- and y-coordinates of the center of mass.
  3. Decide if the center of mass moves in a circle by plotting it…
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9.6 Exercise 11

Find the center of mass of a rod of length L whose mass density changes from one end to the other quadratically. That is, if the rod is laid out along the x-axis with one end at the origin and the other end at x=Lx = L, the density is given by ρ(x)=ρ0+(ρ1−ρ0)(xL)2\rho \left(x\right) = \rho_{0} + \left(\rho_{1} - \rho_{0}\right) \left(\frac{x}{L}\right)^{2}, where ρ0\rho_{0} and ρ1\rho_{1} are constant values.

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9.6 Exercise 13

Find the center of mass of a rectangular material of length a and width b made up of a material of nonuniform density. The density is such that when the rectangle is placed in the xy-plane, the density is given by ρ(x,y)=ρ0xy\rho \left(x , y\right) = \rho_{0} x y.

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9.6 Exercise 15

Find the center of mass of a cone of uniform density that has a radius R at the base, height h, and mass M. Let the origin be at the center of the base of the cone and have +z going through the cone vertex.

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9.6 Exercise 17

Find the center of mass of a uniform thin semicircular plate of radius R. Let the origin be at the center of the semicircle, the plate arc from the +x axis to the −x axis, and the z axis be perpendicular to the plate.

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Adapted from University Physics Volume 1 © 2016 Rice University. Licensed under CC BY 4.0. Source: University Physics Volume 1. Imported at revision db44eb9.