Math 2.0

Mechanics of particles and systems Definition

Scleronomous constraint

Builds on Holonomic constraint

Definition

Consider a system of NN point particles with position vector x∈ℝ3Nx \in \R^{3N} and time tt. Let f(x,t)=0f(x, t) = 0 be a holonomic constraint, with ff defined on U×JU \times J for an open set U⊆ℝ3NU \subseteq \R^{3N} and an interval JJ. The constraint is scleronomous if ff does not depend on tt, that is, ∂f/∂t=0\partial f / \partial t = 0 on U×JU \times J. More generally, a constraint g(x,x˙,t)=0g(x, \dot x, t) = 0 on positions and velocities is scleronomous if gg does not depend on tt.

Remarks

Example: the pendulum constraint ∣x∣2−ℓ2=0\abs{x}^2 - \ell^2 = 0, with fixed length ℓ>0\ell > 0, does not contain tt, so it is scleronomous. Non-example: a bead moves on a wire ring of radius 11, centred at the origin in a vertical plane through the zz-axis. The ring turns about the zz-axis with angular speed ω≠0\omega \ne 0. The bead obeys xsin⁡(ωt)−ycos⁡(ωt)=0x \sin(\omega t) - y \cos(\omega t) = 0 and x2+y2+z2=1x^2 + y^2 + z^2 = 1; the first equation contains tt explicitly, so it is not scleronomous. When all constraints are scleronomous, the positions of the particles can be written as functions x=x(q)x = x(q) of generalized coordinates qq alone, without tt.

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  1. Holonomic constraint concept
  2. Scleronomous constraint definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Scleronomous
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MSC70F20, 70G10
DefinesScleronomous constraint
UsesHolonomic constraint
Changed3 November 2026

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