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1. Thursday Week 2 Lecture. Jeff Eldred Review. 2. Overview. Lagrange, Hamilton, Poisson, Mechanics Accelerator Physics Electromagnetism Relativity Synchrotron Radiation. 3. Lagrange, Hamilton, Poisson Mechanics (see Lectures 1-5). Lagrangian Mechanics.
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1 Thursday Week 2 Lecture Jeff Eldred Review
2 Overview Lagrange, Hamilton, Poisson, Mechanics Accelerator Physics Electromagnetism Relativity Synchrotron Radiation
3 Lagrange, Hamilton, Poisson Mechanics (see Lectures 1-5)
Lagrangian Mechanics The Lagrangian is defined by: Lagrange’s Equations: Every independent set of phase-space coordinate has its own Lagrange equation.
Electromagnetic Lagrangian The Electromagnetic Lagrangian is: With the conjugate momentum:
Hamiltonian Mechanics The conjugate momentum is defined: The Hamiltonian is defined by: When there is no explicit time dependence: The equations of motion are given by:
Poisson Brackets Poisson Brackets are defined: Where pk is the conjugate momentum. With Poisson Brackets we can consider the time dependence of any function of the coordinates: A set of coordinates is canonical iff:
Oscillator Examples Driven Harmonic Oscillator without Damping: Harmonic Oscillator with Damping:
Generating Functions q, Q independent q, P independent q, Q independent p, P independent
Finding Action-Angle Coordinates Method 1 (Position - Momentum): Method 2 (Time - Energy):
11 Accelerator Physics (see Lectures 6-10)
Longitudinal Dynamics Longitudinal Equations of Motion: Synchrotron Motion:
Linear Betatron Motion Betatron Motion: Betatron Tune, Phase-Advance: Courant-Snyder Parameters:
Nonlinear Resonance Accelerator Hamiltonian: Then take Fourier series near a resonance. Sextupole example:
15 Electromagnetism (see Lecture 13-17, Suppl)
Vector Identities Dot Product: Vector Product: Gauss Theorem: Stokes Theorem:
Eikonal Approximation General E&M Wave: Eikonal Approximation: Longitudinal-Transverse Independent: Cylindrically Symmetric:
21 Relativity (See Lecture 15, 18)
Lorentz Coordinate Transformation Relativistic Energy & Momentum
Retarded Time Retarded-Time Potentials:
Fields from a Point Charge Lienard-Wiechert Potentials:
27 Synchrotron Radiation (see Lecture 20, 24)
Radiation Spectrum If ψ= 0: