Analytical Mechanics: Regularity Conditions on Constraint Surface

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Discussion Overview

The discussion revolves around the regularity conditions on constraint surfaces in analytical mechanics, specifically focusing on the implications of the gradient of the constraint function G being non-zero. Participants explore the necessity of this condition for determining the motion of particles under constraints.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • One participant questions the necessity of the regularity condition on the constraint surface defined by G = 0, seeking clarification on its implications.
  • Another participant explains that the condition ensures the equations of motion are well-defined, using an example where the gradient is zero at a point, leading to multiple possible paths for the particle.
  • A participant expresses confusion about the relationship between the gradient being zero and the existence of multiple movement paths for the particle, questioning why this is problematic.
  • Another participant emphasizes that a particle's motion must be uniquely determined by its initial conditions, raising a specific scenario with initial position and velocity to illustrate the issue.
  • Further clarification is sought regarding the relationship between the gradient and the particle's motion, with a participant suggesting that the gradient could influence the particle's trajectory.
  • A mathematical problem is introduced involving a particle sliding on a surface defined by a function f(x, y, z) = 0, prompting further exploration of the normal force acting on the particle.
  • Participants discuss Newton's second law in the context of the problem, with one noting the relationship between the normal force and the acceleration of the particle.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the implications of the regularity condition, with some agreeing on its importance while others remain uncertain about its necessity and the relationship to particle motion. The discussion does not reach a consensus on these points.

Contextual Notes

Participants exhibit uncertainty regarding the mathematical implications of the gradient condition and its connection to the uniqueness of motion. The discussion includes unresolved questions about the nature of constraints and their effects on particle dynamics.

apec45
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Hi,
In my course in analytical mechanics, it is said that for a system of n particles subjected to r constraint equations, it is necessary to impose regularity conditions on the constraint surface defined by G = 0 where G is a function of the position of the position of the particles and time, the condition is that the gradient of G is non-zero on the surface G = 0.

I don't understand why we're asking this?

Thanks for your help (and sorry if i made mistakes)
 
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apec45 said:
don't understand why we're asking this?
because this condition guarantees that the equations of motion will be correct

For example if you have a particle and the constraint ##G=x^2-y^6=0## on the plane, then the particle will not know where to move from ##(0,0)##: it can move along the curve ##x=y^3## or along the curve ##x=-y^3##. In this example ##\nabla G\mid_{(0,0)}=0##
 
Last edited:
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Thanks you for the answer! but i don't understand it very well :(

First, I don't see the link between "the gradiant is zero somewhere" and "there is several ways to move the particule somewhere" (I am ok with your example but i don't see the link).

Then, i don't know what's the problem to have several ways to move the particle, for example if there was no constraints (G = 0 = 0 if i can say that), there would be infinitely many ways to move the particule (anywhere on the plane here) but i don't see the problem in this case, in fact i don't see the link with "the equation of movement has exactly one solution"

Thank you for your help!
 
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A motion of the particle must be determined uniquely by its initial position and velocity. In my example for the initial position take (0,0) and for the initial velocity take ##\boldsymbol {e}_y##. So where will the particle move then?
 
Oh okey, i got it! Thank you so much! We don't know where the particule will go (x = y³ or x = -y³).

And could you give me a little bit explanation about the link with the gradiant? :) I really don't see the link with that, or maybe it is that : if G(x, y) = 0 is the equation of the surface then the particule will have, on a point (x, y) of the surface, a velocity proportional to the gradiant of G on (x, y) ? (i mean if we consider a gradiant like a vector field then if we let a particule follow the vector field, we can see its trajectory)

ps: according to me if the gradiant on a point is zero then the particule will stay there and keep that position, it doesn't seem a problem, or am i wrong?
 
apec45 said:
And could you give me a little bit explanation about the link with the gradiant?
Solve the following problem. A particle of mass m slides without friction on a surface ##\{f(x,y,z)=0\}##. The function ##f## is given. For simplicity assume that there is no other forces except the force of normal reaction ##\boldsymbol{N}.## Find $$\boldsymbol {N}=\boldsymbol {N}(\boldsymbol {r},\boldsymbol {\dot r}).$$
Here ##\boldsymbol r=x\boldsymbol {e}_x+ y\boldsymbol {e}_y+z\boldsymbol {e}_z## is the radius-vector of the particle in the standard inertial frame ##Oxyz##
 
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Uhm, i only see that ##N = m . a## (by Newton's second law) and ##f(x, y, z) = 0## (constraint)
 
I also see that if i do that: ##N.t = ma.t## with## t ## tangent to the surface, i get ##a*t = 0##
 

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