Learning outcomes

To master the different formalisms of classical mechanics (Newton, Lagrange, Hamilton) and use them to tackle selected fundamental mechanical problems.

Content

The course studies first the movement of point masses or solids subjected to forces. The motion and conservation laws of Newtonian mechanics are deduced, as well as the relations between speeds and accelerations observed in different moving reference frames (including that of the centre of mass). One chapter deals with the general study of the one-dimensional motion of a conservative system. Then, the concepts of generalized coordinate, constraint, virtual work and variational problem are introduced to tackle Lagrange's formalism et Hamilton's least action principle. The main characteristics of the formalism are studied (including the conservation laws and the case of electromagnetism). A few fundamental problems of mechanics are dealt with: small oscillations, the two-body problem in a central potential (Kepler's laws and Rutherford scattering), solid rotations. Finally, Hamilton's formalism is introduced and the properties of Hamilton's equations, phase space, canonical transformations, and action are analysed. Hamilton-Jacobi's equation is deduced and the method illustrated through Kepler's problem.

Table of contents

1. Newtonian mechanics
- Point particle mechanics
- One-dimensional conservative systems
- Systems of point particles
- Non inertial reference frames
- The solid (1st part)
2. Lagrangian mechanics
- Bases of Lagrange's formalism
- Hamilton's variational principle
- Properties of the Lagrangian
- Lagrangian systems
- Two-body problem in a central potential
- The solid (2nd part)
3. Hamiltonian mechanics
- Hamilton's formalism
- Canonical transformations
- Hamilton-Jacobi's equation

Exercices

The goal of the supervised exercises is to apply the theoretical concepts taught during the course to concrete applications. A first part deals with the rotation of solid bodies. In particular, we shall study the rotation of typical geometrical bodies (such as cylinders and cones), the gyroscope, and the motion of trailers and helices. After reviewing mathematical tools (such as ordinary differential equations and curvilinear coordinate systems) required to solve mechanical problems, we shall use the Lagrangian and Hamiltonian formalisms in a second part. In particular, we shall use these formalisms will to describe the motion of simple systems (coupled pendulum, two-dimensional systems of coupled oscillators...) and of more complex systems (Foucault pendulum, Penning trap...). The last part of the supervised exercises will include the equation of Hamilton-Jacobi in a synthesis of the major formalisms of analytical mechanics.

Assessment method

The course content taught in Q1 is evaluated with an exam E1 of theory and exercises (exam oragnized in January and August).

The course content taught in Q2 is evaluated with an  exam E2 of exercises and with an  exam E3 of theory (exams oragnized in June and August).

If the grade of the exams E1, E2 et E3 are each better than or equal to 8/20, the global grade is given by the following weighted average: 1/2 E1 + 1/2 (2/3 E2 + 1/3 E3). Otherwise (that is, if one of the three grades at least is lower than 8), the exam is automatically considered failed (independently of the grade average).

Sources, references and any support material

The course does not follow a specific textbook. Nevertheless, here are useful references.
- Mécanique : de la formulation lagrangienne au chaos hamiltonien, Claude Gignoux et Bernard Silvestre-Brac, EDP Sciences
- Problèmes corrigés de mécanique et résumés de cours : de Lagrange à Hamilton, Claude Gignoux et Bernard Silvestre-Brac, EDP Sciences
- Mécanique (volumes 1 et 2), Philippe Spindel, Editions Scientifiques GB
- The variational principles of mechanics, Cornelius Lanczos, Dover
- Classical dynamics of particles and systems, Jerry Marion and Stephen Thornton, Harcourt

Language of instruction

Français
Training Study programme Block Credits Mandatory
Bachelier en sciences physiques Standard 0 7
Bachelier en sciences physiques Standard 2 7