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Kinetic Energy of a Mass
Kinetic energy is energy associated with motion. For
example, when a spring uncompresses and accelerates a mass, as in the
configuration of Fig.B.2, work is performed on the mass
by the spring, and we say that the potential energy of the spring is
converted to kinetic energy of the mass.
Suppose in Fig.B.2 we have an initial spring compression
by
meters at time
, and the mass velocity is zero at
. Then from the equation of motion Eq.
(B.5), we can calculate
when the spring returns to rest (
). This first happens at the
first zero of
, which is time
. At this time, the velocity,
given by the time-derivative of Eq.
(B.5),
can be evaluated at

to yield the mass velocity
![$ v[(\pi/2)/\omega_0] = -A\omega_0 = -A\sqrt{k/m}$](http://www.dsprelated.com/josimages_new/pasp/img2652.png)
, which is when all
potential energy from the spring has been converted to kinetic energy
in the mass. The square of this value is
and we see that if we multiply

by

, we get
which is the initial potential energy stored in the spring. We
require this result. Therefore, the kinetic energy of a mass must be
given by
in order that the kinetic energy of the mass when spring compression
is zero equals the original potential energy in the spring when the
kinetic energy of the mass was zero. In the next section we derive
this result in a more general way.
Previous: Potential Energy
in a SpringNext: Mass Kinetic Energy from Virtual Work
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.