Scleronomous Explained

A mechanical system is scleronomous if the equations of constraints do not contain the time as an explicit variable and the equation of constraints can be described by generalized coordinates. Such constraints are called scleronomic constraints. The opposite of scleronomous is rheonomous.

Application

See main article: Generalized velocity. In 3-D space, a particle with mass

m , velocity v has kinetic energy T T = (1)/(2) m v ^{2} .

Velocity is the derivative of position

r with respect to time t . Use chain rule for several variables:v = (d r)/(dt) = \sum _{i (\partial r)/(\partial q _{i})} • q ^{i + (\partial r)/(\partial t)} . where q _{i} are generalized coordinates.

Therefore,

T = (1)/(2) m \left(\sum _{i (\partial r)/(\partial q _{i})} • q ^{i + (\partial r)/(\partial t)} \right) ^{2.}

Rearranging the terms carefully,^[1]

T = T _{0+T} _{1+T} _{2:} T _{0= (1)/(2)} m\left( (\partial r)/(\partial t) \right) ^{2,} T _{1=\sum} ^{i m (\partial r)/(\partial t)} ⋅ (\partial r)/(\partial q _{i}) • q _{i,} T _{2=\sum} _{i,j} (1)/(m 2) (\partial r)/(\partial q _{i}) ⋅ (\partial r)/(\partial q _{j}) • q ^{• i q} _{j,}

where

T _{0} , T _{1} , T _{2} are respectively homogeneous functions of degree 0, 1, and 2 in generalized velocities. If this system is scleronomous, then the position does not depend explicitly with time:(\partial r)/(\partial t) =0 . Therefore, only term T _{2} does not vanish:T = T _{2.} Kinetic energy is a homogeneous function of degree 2 in generalized velocities .

Example: pendulum

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’s length is a constant. Therefore, this system is scleronomous; it obeys scleronomic constraint

\sqrt{x ^{2+y} ^{2}} - L =0 ,

where

(x,y) is the position of the weight and L is length of the string.

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 a simple harmonic motion

x _{t=x} _{0\cos\omega} t,

where

x _{0} is amplitude, \omega is angular frequency, and t is 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

\sqrt{(x - x _{0\cos\omega} t) ^{2+y} ^{2}} - L =0 .

See also

• Lagrangian mechanics
• Holonomic system
• Nonholonomic system
• Rheonomous
• Mass matrix

References

1. Book: Goldstein, Herbert. Classical Mechanics. limited. 1980. United States of America . Addison Wesley. 3rd. 0-201-65702-3 . 25.