Monogenic system

Source: Wikipedia, the free encyclopedia.

In classical mechanics, a physical system is termed a monogenic system if the force acting on the system can be modelled in a particular, especially convenient mathematical form. The systems that are typically studied in physics are monogenic. The term was introduced by Cornelius Lanczos in his book The Variational Principles of Mechanics (1970).[1][2]

In

holonomic system and a monogenic system, then it is possible to derive Lagrange's equations from d'Alembert's principle; it is also possible to derive Lagrange's equations from Hamilton's principle.[3]

Mathematical definition

In a physical system, if all forces, with the exception of the constraint forces, are derivable from the

generalized velocities
, or time, then, this system is a monogenic system.

Expressed using equations, the exact relationship between

generalized force
and generalized potential is as follows:

where is generalized coordinate, is generalized velocity, and is time.

If the generalized potential in a monogenic system depends only on generalized coordinates, and not on generalized velocities and time, then, this system is a conservative system. The relationship between generalized force and generalized potential is as follows:

.

See also

References

  1. ^ J., Butterfield (3 September 2004). "Between Laws and Models: Some Philosophical Morals of Lagrangian Mechanics" (PDF). PhilSci-Archive. p. 43. Archived from the original (PDF) on 3 November 2018. Retrieved 23 January 2015.
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