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Striking the Rod in the Middle
First, consider
. That is, we apply an
upward unit-force impulse at time 0 in the middle of the rod. The
total momentum delivered in the neighborhood of
and
is
obtained by integrating the applied force density with respect to time
and position:
This unit momentum is transferred to the two
masses 
. By symmetry,
we have

. We can also refer to

as the
velocity of the center of mass, again obvious by symmetry.
Continuing to refer to Fig.
B.5, we have
Thus, after time zero, each mass is traveling upward at speed

, and there is no rotation about the center of mass at

.
The kinetic energy of the system after time zero is
Note that we can also compute

in terms of the total mass

and the velocity of the center of mass

:
Previous: Two Masses Connected by a RodNext: Striking One of the Masses
About the Author: Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at
Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See
http://ccrma.stanford.edu/~jos/ for details.