-- card: 7617 from stack: in -- bmap block id: 0 -- flags: 0000 -- background id: 2600 -- name: -- part 2 (button) -- low flags: 00 -- high flags: A003 -- rect: left=279 top=199 right=221 bottom=379 -- title width / last selected line: 0 -- icon id / first selected line: 0 / 0 -- text alignment: 1 -- font id: 0 -- text size: 12 -- style flags: 0 -- line height: 16 -- part name: bagel section ----- HyperTalk script ----- on mouseUp open bin:strange attractors:birkhoff bagel:bagel.strobe end mouseUp -- part 3 (button) -- low flags: 00 -- high flags: A003 -- rect: left=136 top=199 right=221 bottom=236 -- title width / last selected line: 0 -- icon id / first selected line: 0 / 0 -- text alignment: 1 -- font id: 0 -- text size: 12 -- style flags: 0 -- line height: 16 -- part name: bagel traj ----- HyperTalk script ----- on mouseUp open bin:strange attractors:birkhoff bagel:bagel.traj end mouseUp -- part 4 (button) -- low flags: 00 -- high flags: A003 -- rect: left=203 top=273 right=295 bottom=303 -- title width / last selected line: 0 -- icon id / first selected line: 0 / 0 -- text alignment: 1 -- font id: 0 -- text size: 12 -- style flags: 0 -- line height: 16 -- part name: animate ----- HyperTalk script ----- on mouseUp open "Birk 32x200:animate" end mouseUp -- part contents for background part 22 ----- text ----- But if the forcing is larger then the dynamics become chaotic: • this is hard to see in the trajectories and time series; • it may be seen in the Poincare section (taken at constant phase of the forcing). e.g. F=1 The stretching & folding of chaos appears in successive Poincare sections