theorem 9.8 Picard–Lindelöf

open in the book · parts/02-mathematical-methods/07-odes-sturm-liouville.tex:260 · p. 275

Rests on

Supports

Neighborhood

Every logical edge within two steps of this node.

theorem 9.8: Picard–Lindelöf9.8definition 9.4: Lipschitz condition9.4equation 9.3: eq:slt-ode-system9.3lemma 9.6: Weierstrass M-test; uniform limits are continuous9.6corollary 32.5: Trajectories do not cross32.5corollary 9.9: Linear equations: existence on the whole interval9.9proposition 32.4: The flow is a one-parameter group32.4proposition 10.16: Cauchy's characteristic strips10.16proposition 20.7: Terminal speed and the approach to it20.7proposition 9.11: Continuous dependence on the initial data9.11proposition 9.142: The differential equation of the sine amplitude9.142theorem A.74: Flow of a time-dependent vector fieldA.74theorem 13.125: Existence, uniqueness and smoothness of the flow13.125theorem 9.34: Poincaré–Bendixson; quoted9.34proof : ch:07-odes-sturm-liouville@proof-2proofdefinition A.438: Momentum variable and the accessory systemA.438definition 7.20: Continuity at a point7.20proposition 7.47: Comparison; absolute convergence7.47proposition 9.139: Series for the complete integral of the first kind9.139proposition 9.22: The exponential and its derivative9.22proof : ch:07-odes-sturm-liouville@proof-1proofdefinition 32.29: Limit cycle32.29definition 32.38: Poincaré section and return map32.38theorem 32.30: Poincaré–Bendixson, restated from Part II32.30proof : ch:15-nonlinear-dynamics-chaos@proof-2proofdefinition 9.2: Linear equation; homogeneity9.2remark 9.3: Normal form and first-order systems9.3definition 9.37: Fundamental matrix9.37lemma A.439: Existence, uniqueness, and the structure of the zerosA.439proposition 20.9: Linear resistance: exact motion, and the lost range20.9proposition 9.103: The positive zeros and their spacing9.103proposition 9.18: The linear equation: integrating factor9.18theorem 9.23: Solution of a constant-coefficient system9.23theorem 9.13: Dimension of the solution space9.13proof : ch:07-odes-sturm-liouville@proof-3proofdefinition 32.3: Dynamical system, phase space, flow32.3proof : ch:15-nonlinear-dynamics-chaos@proof-1proofproposition 7.105: Clairaut–Schwarz7.105proposition 10.15: Method of characteristics, first order10.15proof : ch:08-pdes@proof-6proofneighborhood truncated

Edges

typedirectionnode provenancewhere
depends_on Lipschitz condition declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:271
depends_on eq:slt-ode-system declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:271
depends_on Weierstrass $M$-test; uniform limits are continuous declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:271
depends_on Trajectories do not cross declared parts/03-classical-mechanics/15-nonlinear-dynamics-chaos.tex:154
depends_on Linear equations: existence on the whole interval declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:364
depends_on The flow is a one-parameter group declared parts/03-classical-mechanics/15-nonlinear-dynamics-chaos.tex:131
depends_on Cauchy's characteristic strips declared parts/02-mathematical-methods/08-pdes.tex:480
depends_on Terminal speed and the approach to it declared parts/03-classical-mechanics/03-exp-projectile-motion.tex:474
depends_on Continuous dependence on the initial data declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:437
depends_on The differential equation of the sine amplitude declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:5409
depends_on Flow of a time-dependent vector field declared appendices/A-long-proofs.tex:4682
depends_on Existence, uniqueness and smoothness of the flow declared parts/02-mathematical-methods/11-manifolds-tensors-curvature.tex:5704
depends_on Poincaré–Bendixson; quoted declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:1268
proves ch:07-odes-sturm-liouville@proof-2 declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:274