Mechanical system whose constraints are independent of time
Amechanical systemisscleronomousif the equations ofconstraintsdo not contain the time as an explicitvariableand the equation of constraints can be described by generalized coordinates. Such constraints are calledscleronomicconstraints. The opposite of scleronomous isrheonomous.
where,,are respectivelyhomogeneous functionsof degree 0, 1, and 2 in generalized velocities. If this system is scleronomous, then the position does not depend explicitly with time:
Therefore, only termdoes not vanish:
Kinetic energy is a homogeneous function of degree 2 in generalized velocities.
As shown at right, a simplependulumis 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’s length is a constant. Therefore, this system is scleronomous; it obeys scleronomic constraint
whereis the position of the weight andis length of the string.
A simple pendulum with oscillating pivot point
Take a more complicated example. Refer to the next figure at right, Assume the top end of the string is attached to a pivot point undergoing asimple harmonic motion
whereis amplitude,is angular frequency, andis time.
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 as it obeys constraint explicitly dependent on time