A mechanical system is rheonomous if its equations of constraints contain the time as an explicit variable.[1] [2] Such constraints are called rheonomic constraints. The opposite of rheonomous is scleronomous.[1] [2]
As shown at right, a simple pendulum is a system composed of a weight and a string. The string is attached at the top end to a pivot and at the bottom end to a weight. Being inextensible, the string has a constant length. Therefore, this system is scleronomous; it obeys the scleronomic constraint
\sqrt{x2+y2}-L=0
(x, y)
L
The situation changes if the pivot point is moving, e.g. undergoing a simple harmonic motion
xt=x0\cos\omegat
x0
\omega
t
Although the top end of the string is not fixed, the length of this inextensible string is still a constant. The distance between the top end and the weight must stay the same. Therefore, this system is rheonomous; it obeys the rheonomic constraint
\sqrt{(x-x0\cos\omegat)2+y2}-L=0
. Herbert Goldstein . Classical Mechanics . limited . 1980 . United States of America . Addison Wesley . 2nd . 0-201-02918-9 . 12 . Constraints are further classified according as the equations of constraint contain the time as an explicit variable (rheonomous) or are not explicitly dependent on time (scleronomous)..