theorem 23.30 Motion in action–angle variables

open in the book · parts/03-classical-mechanics/06-hamilton-jacobi.tex:927 · p. 834

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theorem 23.30: Motion in action–angle variables23.30definition 23.28: Action variables23.28proposition 22.18: The mixed generating functions22.18theorem 22.6: Hamilton's equations22.6example 23.24: Harmonic oscillator23.24theorem 23.34: Adiabatic invariance of the action23.34theorem 23.31: Liouville–Arnold23.31proof : ch:06-hamilton-jacobi@proof-8proofdefinition 16.99: Abbreviated action16.99definition 23.13: Additive separability23.13proposition 23.38: Bohr–Sommerfeld and Einstein–Brillouin–Keller quantization23.38proposition 24.56: The Bohr–Sommerfeld condition is a triviality condition on the prequantum holonomy24.56remark 23.29: Convention23.29remark 29.45: What integrability buys, and where it stops29.45definition 22.15: Canonical transformation22.15equation 22.18: eq:ham-generating22.18definition 23.2: Hamilton's principal function and the Hamilton–Jacobi equation23.2proposition A.556: The Jacobian of the actions is the lattice matrixA.556remark 22.19: Which form exists22.19proof : ch:05-hamiltonian-mechanics@proof-6proofdefinition 22.2: Hamiltonian22.2equation 21.39: eq:lag-el-conservative21.39equation 21.43: eq:lag-generalized-momentum21.43remark 22.8: Non-conservative forces22.8remark 22.7: Which half is kinematics and which is dynamics22.7remark 23.4: What the equation costs and what it buys23.4theorem 23.6: Jacobi23.6proof : ch:05-hamiltonian-mechanics@proof-2proofproposition 28.6: Phase-space area and the action variable28.6equation 22.10: eq:ham-dhdt22.10example 23.35: The slowly stiffened oscillator23.35example 23.27: Charged particle in a uniform magnetic field23.27remark 23.36: How good the invariance really is23.36remark 23.37: Why this matters observationally23.37proof : ch:06-hamilton-jacobi@proof-9proofequation 22.41: eq:ham-poisson-bracket22.41theorem 24.21: Liouville24.21remark 23.33: Integrability is exceptional23.33remark 23.32: What that proof imports23.32theorem 32.51: Kolmogorov–Arnold–Moser, quoted32.51neighborhood truncated

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typedirectionnode provenancewhere
depends_on Action variables declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:940
depends_on The mixed generating functions declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:940
depends_on Hamilton's equations declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:940
depends_on Harmonic oscillator declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:774
depends_on Adiabatic invariance of the action declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:1059
depends_on Liouville–Arnold declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:994
proves ch:06-hamilton-jacobi@proof-8 declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:944