“Holonomic constraints”的意思、由来-开放百科全书

In classical mechanics, holonomic constraints are relations between the position variables (and possibly time^[1]) which can be expressed in the following form:

where

are the n coordinates which describe the system. For example, the motion of a particle constrained to lie on the surface of a sphere is subject to a holonomic constraint, but if the particle is able to fall off the sphere under the influence of gravity, the constraint becomes non-holonomic. For the first case the holonomic constraint may be given by the equation:

Where

is the distance from the centre of a sphere of radius

. whereas the second non-holonomic case may be given by:

Holonomic system (physics)

In classical mechanics a system may be defined as holonomic if all constraints of the system are holonomic. For a constraint to be holonomic it must be expressible as a function:

i.e. a holonomic constraint depends only on the coordinates

and time

.^[1] It does not depend on the velocities or any higher order derivative with respect to t. A constraint that cannot be expressed in the form shown above is a nonholonomic constraint.

Transformation to independent generalized coordinates

The holonomic constraint equations can help us easily remove some of the dependent variables in our system. For example, if we want to remove

which is a parameter in the constraint equation

, we can rearrange the equation into the following form, assuming it can be done,

and replace the

in every equation of the system using the above function. This can always be done for general physical system, provided that

, then by implicit function theorem, the solution

is guaranteed in some open set. Thus, it is possible to remove all occurrences of the dependent variable

Suppose that a physical system has

degrees of freedom. Now,

holonomic constraints are imposed on the system. Then, the number of degrees of freedom is reduced to

. We can use

independent generalized coordinates (

) to completely describe the motion of the system. The transformation equation can be expressed as follows:

Differential form

where c_ij, c_i are the coefficients of the differentials dq_j and dt for the ith constraint.

If the differential form is integrable, i.e., if there is a function

satisfying the equality

then this constraint is a holonomic constraint; otherwise, nonholonomic. Therefore, all holonomic and some nonholonomic constraints can be expressed using the differential form. Not all nonholonomic constraints can be expressed this way. Examples of nonholonomic constraints which can not be expressed this way are those that are dependent on generalized velocities. With a constraint equation in differential form, whether the constraint is holonomic or nonholonomic depends on the integrability of the differential form.

Classification of physical systems

In order to study classical physics rigorously and methodically, we need to classify systems. Based on previous discussion, we can classify physical systems into holonomic systems and non-holonomic systems. One of the conditions for the applicability of many theorems and equations is that the system must be a holonomic system. For example, if a physical system is a holonomic system and a monogenic system, then Hamilton's principle is the necessary and sufficient condition for the correctness of Lagrange's equation.^[2]

Examples

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 holonomic; it obeys the holonomic constraint

where

are respectively the positions of particles

and

, and

is the distance between them.

References

1. ^¹{{Cite book|url=https://www.worldcat.org/oclc/960166650|title=Classical mechanics|last=Goldstein|first=Herbert|publisher=Addison-Wesley|others=|year=2002|isbn=9788131758915|edition= Third|location=Pearson India|pages=12–13|chapter=1.3 Constraints|oclc=960166650}}
2. ^{{cite book |last=Goldstein |first=Herbert |authorlink=Herbert Goldstein |title=Classical Mechanics |year=1980 |location=United States of America |publisher=Addison Wesley |edition= 3rd |isbn=0-201-65702-3 |page=45}}