11 - Classical Mechanics - TTM
Our exploration of the theoretical underpinnings of modern physics begins with classical mechanics, the mathematical physics worked out by Isaac Newton (1642--1727) and later by Joseph Lagrange (1736--1813) and William Rowan Hamilton (1805--1865). We will start with a discussion of the allowable laws of physics and then delve into Newtonian mechanics. We then study three formulations of classical mechanics respectively by Lagrange, Hamiltonian and Poisson. Throughout the lectures we will focus on the relation between symmetries and conservation laws. The last two lectures are devoted to electromagnetism and the application of the equations of classical mechanics to a particle in electromagnetic fields.
This first lecture is a general discussion of the nature of the laws of physics and in particular classical mechanics. The notions of configuration, reversibility, determinism, and conservation law are introduced for simple systems with a finite number of states.
Topics
Allowable laws of physics
Configurations of a coin
Equations of motion of a coin and a die
The concept of conserved quantities and conservation laws
Systems with infinite number of configurations
Laws of physics that are not allowable
Non reversibility
Predictability in the real world
Determinism in the past and future
System of point particles in space
Mathematics: coordinate systems, vector algebra, vector dot product, triangle law of cosines
Motion of a particle: position, velocity and acceleration
Circular motion and centripetal acceleration
References
This lecture focuses on classical mechanics expressed using Newton’s 2nd law. The notions of phase space, momentum and energy are introduced.
Topics
Aristotle incorrect laws of motion
Newton’s law (the 2nd law)
Inertial reference frames
Newton’s determinism and the need of position and velocity
Momentum and Newton’s law
Phase space
Newton and reversibility
Newton’s law and conserved quantities
Newton’s 3 laws
Proof of conservation of momentum for an isolated system of particles
Potential energy
Energy conservation for a system of particles
Harmonic oscillator and energy
References
This lecture introduces Lagrange’s formulation of classical mechanics. That formulation is formal and elegant; it is based on the Least Action Principle. The concepts introduced here are central to all modern physics. The lecture ends with angular momentum and coordinate transforms.
Topics
Principle of Least Action (“stationary action”)
Equilibrium points of a function
Trajectories
Calculus of variations
Light in a refractive media and hanging chain catenary
Lagrangian and Action
Euler Lagrange equations of motion
Newton equations from the Lagrangian of a system of particles
Importance of the Lagrange formulation of physics
Lagrangian and coordinate changes
Rotating frame, centrifugal and Coriolis forces
Polar coordinates and angular momentum conservation
Lagrangian, conservation and cyclic coordinates
References
This lecture focuses on the relation between continuous symmetries of the Lagrangian and conserved quantities. Generalized coordinates and canonical conjugate momentum are introduced.
Topics
Symmetry and conservation laws: they are always related
Review of the principle of least action (stationary action)
Generalized coordinates and their canonical conjugate momentum
Conserved quantities and translation and rotation symmetry
Noether theorem concept and outline
Momentum conservation as a consequence of translation symmetry
Angular momentum conservation as a consequence of rotational symmetry
The harmonic oscillator
Discrete symmetries have no associated conserved quantities in classical mechanics
References
This lecture starts with a thorough review of symmetries and conservation laws. Energy conservation is shown to be a consequence of time translation symmetry and the Hamiltonian is introduced.
Topics
Recommended books
Superluminal neutrinos in the news
Review of symmetries and conservation laws
Active vs passive transformations
Review of momentum and angular momentum conservation and associated symmetries
Energy conservation as a consequence of time translation symmetry
Hamiltonian and energy conservation
References
In this lecture many mechanical practical examples are worked out. Hamilton’s equations are introduced: they represent one more way to do classical mechanics. The harmonic oscillator is revisited using Hamilton’s equations.
Topics:
Motion of a ball on a wedge as an example of Euler-Lagrange equations
The ball on a wedge: Associated symmetries and conservation laws, conjugate momentum
Double pendulum example treated in detail. Associated symmetries and conservation
Hamiltonian, forbidden laws, reversibility, convergent and divergent paths in state space
Hamilton’s equations of motion
Harmonic oscillator using Hamilton’s equations and energy conservation
Phase space
References:
This lecture analyses the flow in phase space of multiple systems, and that flow is shown to be incompressible. Poisson brackets are introduced as yet another way to express classical mechanics formally.
Topics
Liouville’s famous theorem
Review of Hamiltonian and energy conservation
Energy conservation and surfaces in phase space
Concept of flow in phase space
Compressible and incompressible flows, the divergence
Demonstration of Liouville’s theorem
Liouville using a toy Hamiltonian. Topology of evolving phase space elements
The damped harmonic oscillator as a counterexample of Liouville
Definition of Poisson bracket
Poisson bracket and time derivative of any quantity
References
Poisson brackets are another formal formulation of classical mechanics. They help make the connection between symmetries and conservation laws more explicit. The Poisson bracket of the x,y,z components of angular momentum are derived.
Topics
Poisson brackets and angular momentum
Review of Poisson brackets
The algebra of Poisson brackets
Angular momentum conservation, rotation symmetry and Poisson brackets as tools to compute the generators of rotation
Momentum conservation, translation symmetry and Poisson brackets as tools to compute the generators of translation
Energy conservation, time shift symmetry and Poisson bracket as a tool to compute the time shift generator
General relation between symmetry and conservation law expressed with Poisson bracket.
Poisson brackets of the x, y, z components of angular momentum.
The gyroscope equations of motion as an example of the power of Poisson brackets
References
This lecture introduces the static electric and magnetic fields, the associated Lagrangian and the Lorentz force. The vector potential, it’s gauge field and gauge invariance are also introduced.
Topics
Magnetic and electric fields
The concept of field
The “del” or “nabla” symbol
Vector calculus: Gradient, Divergence and Curl
The Levi-Civita symbol
Algebra: div curl and curl grad vanish
The vector potential and why it’s needed
Gauge field: “Gauge” is a misnomer
Lorentz force. Lorentz force compared with the Coriolis force
Lagrangian for charged particles in a electro-static and magneto-static fields
Gauge invariance of the equations of motions associated to the electro-magneto-static Lagrangian
References
This final lecture is a general review of all the concepts learned so far applied to a particle in electric and magnetic static fields
Topics
Review of the vector potential, concept of gauge and gauge invariance
Lorentz force law
Example of different vector potentials for a constant magnetic field and the gauge transformation that relate them
Importance of gauge invariance and choice of gauge
Lagrangian of a particle in a static magnetic field. Review of the related action gauge invariance
Distinction between mechanical and canonical momentum: only the canonical momentum is related to symmetries and invariance
Derivation of the Euler-Lagrange equation of motion from the magneto-static Lagrangian and rediscovery of the Lorentz force
Justification of the vector potential as an essential tool for the least action principle
Derivation of the magneto-static Hamiltonian
Smart choice of gauge and derivation of the Lorentz force from symmetry arguments only, “cyclic coordinates”
Circular motion of a charged particle in a static magnetic field
Monopoles discussion as part of the questions session
Brief Quaternions discussion as part of the questions session
References