Figure
2
The center of mass of an object is the position at which the entire mass of the object could be concentrated, and still have the same "average motion" as the entire body does.
If a rigid body is composed of n particles connected in a straight
line, then the location of the center of mass for the system is x_cm
where
(m1 + m2 + . . . + m_n)x_cm = m1 x1 + . . . + m_n x_n
If the particles are extended into two or three dimensions
the coordinates of the center of mass are defined by (x_cm, y_cm, z_cm)
where
(m1 + . . . + m_n) x_cm = m1 x1 + . . . + m_n x_n
(m1 + . . . + m_n) y_cm = m1 y1 + . . . + m_n y_n
(m1 + . . . + m_n) z_cm = m1 z1 + . . . + m_n z_n
For a continuous distribution of matter, the summations turn into
integrals. We want to think of the object as being cut into thin
strips of small mass. For example, in Figure 3
the object is horizontally symmetric, so x_cm = 0.
Figure 3
To find y_cm, we
can chop the object into strips of small mass: dm = p w(y) dy.
Then y_cm satisfies the equation
Index
More: Centroids
Next: Moments of Inertia
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Jennifer Powell<jpowell@geom.umn.edu> Fati Liamidi<liamidi@geom.umn.edu>