Goldstein Derivation 1.6: Nonholonomic Constraints in Particle Motion

In summary, the problem statement discusses a particle moving in the xy plane with a constraint on its velocity vector. The attempt at a solution involves a differential equation and the integrability of an expression involving the given function f(t). The question arises as to why this integral cannot be performed in general due to the arbitrariness of f(t), which is explained by considering t as an implicit function of x and y.
  • #1
DrHouse
1
0
1. The problem statement

A particle moves in the ##xy## plane under the constraint that its velocity vector is always directed towards a point on the ##x## axis whose abscissa is some given function of time ##f(t)##. Show that for ##f(t)## differentiable but otherwise arbitrary, the constraint is NONHOLONOMIC.

2. The attempt at a solution
I have got the differential equation relating the generalised coordinates (in this case they are ##x## and ##y## since the system has two degrees of freedom):

## ydx + [f(t)-x]dy = 0 ##

If the constraint equation is nonholonomic, then the previous integral can not be performed but it's true that it can be written as

## \displaystyle \int \frac{dx}{x-f(t)} = \int \frac{dy}{y}##


which, I think is an integrable expression in terms of logarithmic functions for any ##f(t)##. Some people say that the previous integral can not be performed in general due to the arbitrariness of ##f(t)##. Can anyone explain me why?
 
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  • #2
Are you forgetting that t must be considered as an implicit function of x and y in your differential expression? That is, f(t) cannot be considered as independent of x and y.
 

Related to Goldstein Derivation 1.6: Nonholonomic Constraints in Particle Motion

1. What is Goldstein Derivation 1.6?

Goldstein Derivation 1.6 is a mathematical equation used in classical mechanics to calculate the motion of a rigid body in a rotating frame of reference.

2. Who developed Goldstein Derivation 1.6?

Goldstein Derivation 1.6 was developed by Herbert Goldstein, a renowned physicist and mathematician, in his book "Classical Mechanics."

3. What is the purpose of Goldstein Derivation 1.6?

The purpose of Goldstein Derivation 1.6 is to simplify the equations of motion for a rigid body in a rotating frame, making it easier to analyze and understand the behavior of the system.

4. How is Goldstein Derivation 1.6 different from other equations in classical mechanics?

Goldstein Derivation 1.6 takes into account the rotational motion of a rigid body, while other equations may only consider translational motion. This makes it more accurate for systems involving rotation.

5. In what fields is Goldstein Derivation 1.6 commonly used?

Goldstein Derivation 1.6 is commonly used in fields such as physics, engineering, and astronomy, where the behavior of rotating bodies is of interest.

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