Table of Contents
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Table of Contents
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Licensing
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Preface
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About the Book
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1: Introductory Statics - the Catenary and the Arch
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2: The Calculus of Variations
- 2.1: The Catenary and the Soap Film
- 2.2: A Soap Film Between Two Horizontal Rings- the Euler-Lagrange Equation
- 2.3: General Method for the Minimization Problem
- 2.4: An Important First Integral of the Euler-Lagrange Equation
- 2.5: Fastest Curve for Given Horizontal Distance
- 2.6: The Perfect Pendulum
- 2.7: Calculus of Variations with Many Variables
- 2.8: Multivariable First Integral
- 2.9: The Soap Film and the Chain
- 2.10: Lagrange Multipliers
- 2.11: Lagrange Multiplier for the Chain
- 2.12: The Brachistochrone
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3: Fermat's Principle of Least Time
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4: Hamilton's Principle and Noether's Theorem
- 4.1: Introduction- Galileo and Newton
- 4.2: Derivation of Hamilton’s Principle from Newton’s Laws in Cartesian Co-ordinates- Calculus of Variations Done Backwards!
- 4.3: But Why?
- 4.4: Lagrange’s Equations from Hamilton’s Principle Using Calculus of Variations
- 4.5: Generalized Momenta and Forces
- 4.6: Non-uniqueness of the Lagrangian
- 4.7: First Integral- Energy Conservation and the Hamiltonian
- 4.8: Example 1- One Degree of Freedom- Atwood’s Machine
- 4.9: Example 2- Lagrangian Formulation of the Central Force Problem
- 4.10: Conservation Laws and Noether’s Theorem
- 4.11: Momentum Conservation
- 4.12: Center of Mass
- 4.13: Angular Momentum Conservation
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5: Mechanical Similarity and the Virial Theorem
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6: Hamilton’s Equations
- 6.1: A Dynamical System’s Path in Configuration Space and in State Space
- 6.2: Phase Space
- 6.3: Going From State Space to Phase Space
- 6.4: How It's Done in Thermodynamics
- 6.5: Math Note - the Legendre Transform
- 6.6: Hamilton's Use of the Legendre Transform
- 6.7: Checking that We Can Eliminate the q˙i's
- 6.8: Hamilton’s Equations
- 6.9: A Simple Example
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7: Time Evolution in Phase Space- Poisson Brackets and Constants of the Motion
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8: A New Way to Write the Action Integral
- 8.1: Function of Endpoint Position
- 8.2: Function of Endpoint Time
- 8.3: Varying Both Ends
- 8.4: Another Way of Writing the Action Integral
- 8.5: How this Classical Action Relates to Phase in Quantum Mechanics
- 8.6: Hamilton’s Equations from Action Minimization
- 8.7: How Can p, q Really Be Independent Variables?
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9: Maupertuis’ Principle - Minimum Action Path at Fixed Energy
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10: Canonical Transformations
- 10.1: Point Transformations
- 10.2: General and Canonical Transformations
- 10.3: Generating Functions for Canonical Transformations
- 10.4: Generating Functions in Different Variables
- 10.5: Poisson Brackets under Canonical Transformations
- 10.6: Time Development is a Canonical Transformation Generated by the Action
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11: Introduction to Liouville's Theorem
- 11.1: Paths in Simple Phase Spaces - the SHO and Falling Bodies
- 11.2: Following Many Systems- a “Gas” in Phase Space
- 11.3: Liouville’s Theorem- Local Gas Density is Constant along a Phase Space Path
- 11.4: Landau’s Proof Using the Jacobian
- 11.5: Jacobian for Time Evolution
- 11.6: Jacobians 101
- 11.7: Jacobian proof of Liouville’s Theorem
- 11.8: Simpler Proof of Liouville’s Theorem
- 11.9: Energy Gradient and Phase Space Velocity
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12: The Hamilton-Jacobi Equation
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13: Adiabatic Invariants and Action-Angle Variables
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14: Mathematics for Orbits
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15: Keplerian Orbits
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16: Elastic Scattering
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17: Small Oscillations
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18: Driven Oscillator
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19: One-Dimensional Crystal Dynamics
- 19.1: The Model
- 19.2: The Circulant Matrix- Nature of its Eigenstates
- 19.3: Comparison with Raising Operators
- 19.4: Finding the Eigenvectors
- 19.5: Eigenvectors of the Linear Chain
- 19.6: Allowed Wavenumbers from Boundary Conditions
- 19.7: Finding the Eigenvalues
- 19.8: The Discrete Fourier Transform
- 19.9: A Note on the Physics of These Waves
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20: Parametric Resonance
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21: The Ponderomotive Force
- 21.1: Introduction to the Ponderomotive Force
- 21.2: Finding the Effective Potential Generated by the Oscillating Force
- 21.3: Stability of a Pendulum with a Rapidly Oscillating Vertical Driving Force
- 21.4: Hand-Waving Explanation of the Ponderomotive Force
- 21.5: Pendulum with Top Point Oscillating Rapidly in a Horizontal Direction
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22: Resonant Nonlinear Oscillations
- 22.1: Introduction to Resonant Nonlinear Oscillations
- 22.2: Frequency of Oscillation of a Particle is a Slightly Anharmonic Potential
- 22.3: Resonance in a Damped Driven Linear Oscillator- A Brief Review
- 22.4: Damped Driven Nonlinear Oscillator- Qualitative Discussion
- 22.5: Nonlinear Case - Landau’s Analysis
- 22.6: Frequency Multiples
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23: Damped Driven Pendulum- Period Doubling and Chaos
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24: Motion of a Rigid Body - the Inertia Tensor
- 24.1: Definition of Rigid
- 24.2: Rotation of a Body about a Fixed Axis
- 24.3: General Motion of a Rotating Rigid Body
- 24.4: The Inertia Tensor
- 24.5: Tensors 101
- 24.6: Definition of a Tensor
- 24.7: Diagonalizing the Inertia Tensor
- 24.8: Principal Axes Form of Moment of Inertia Tensor
- 24.9: Relating Angular Momentum to Angular Velocity
- 24.10: Symmetries, Other Axes, the Parallel Axis Theorem
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25: Moments of Inertia and Rolling Motion
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26: Rigid Body Moving Freely
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27: Euler Angles
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28: Euler’s Equations
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29: Non-Inertial Frame and Coriolis Effect
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30: A Rolling Sphere on a Rotating Plane
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Index
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Glossary
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Glossary
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Detailed Licensing

