Math 2.0

Mechanics of particles and systems Definition

Classical mechanics

Builds on Euclidean spaceOrdinary differential equationPicard–Lindelöf theorem

Definition

A Newtonian system of NN point particles consists of the following data.

  1. Masses m1,…,mN>0m_1, \dots, m_N > 0.
  2. For each ii, a position xi(t)∈ℝ3x_i(t) \in \R^3 at time tt, where ℝ3\R^3 is three-dimensional Euclidean space.
  3. For each ii, a force law Fi(t,x,x˙)∈ℝ3F_i(t, x, \dot x) \in \R^3, a function of the time tt, of all positions x=(x1,…,xN)x = (x_1, \dots, x_N) and of all velocities x˙=(x˙1,…,x˙N)\dot x = (\dot x_1, \dots, \dot x_N).

A motion of the system is a twice differentiable map t↦(x1(t),…,xN(t))t \mapsto (x_1(t), \dots, x_N(t)) on an interval that solves the ordinary differential equations mix¨i(t)=Fi(t,x(t),x˙(t)),i=1,…,N.m_i \ddot x_i(t) = F_i\big(t, x(t), \dot x(t)\big), \qquad i = 1, \dots, N. Classical mechanics, in its Newtonian form, is the study of such systems and their motions.

Remarks

Example: one particle of mass mm under the constant force F=(0,0,−mg)F = (0, 0, -mg) with g>0g > 0. The map x(t)=(t,0,−gt2/2)x(t) = (t, 0, -g t^2/2) is a motion, since mx¨=(0,0,−mg)=Fm \ddot x = (0, 0, -mg) = F. Non-example: the map x(t)=(t,0,0)x(t) = (t, 0, 0) is not a motion of this system, since mx¨=0≠Fm \ddot x = 0 \ne F. If the force laws are locally Lipschitz, the Picard–Lindelöf theorem shows that the initial positions and velocities determine the motion on some interval. A dot over a symbol denotes the derivative with respect to time.

Reading path

To understand this page from the ground up, read these 15 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
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  1. Differential equation concept
  2. Euclidean space object
  3. Function concept
  4. Interval concept
  5. Ordinary differential equation concept
  6. Ordinary differential equation definition
  7. Lipschitz condition definition
  8. Solution of an ordinary differential equation definition
  9. Initial value problem definition
  10. Picard–Lindelöf hypotheses definition
  11. Picard operator definition
  12. Integral equation form of an initial value problem statement
  13. An iterate of the Picard operator is a contraction statement
  14. Picard–Lindelöf theorem statement
  15. Classical mechanics definition

Where this leads

96 pages build on this one.

Further reading

  1. Web https://en.wikipedia.org/wiki/Classical_mechanics
About this page
TagSH7J0X3NCC
URIm2://SH7J0X3NCC
Kinddefinition
WritingW0 stub
MSC70A05, 70F10
DefinesClassical mechanics
UsesEuclidean space, Ordinary differential equation, Picard–Lindelöf theorem
Changed3 November 2026

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