671:
454:
662:. It separates — hence the name — the phase space into two distinct areas, each with a distinct type of motion. The region inside the separatrix has all those phase space curves which correspond to the pendulum oscillating back and forth, whereas the region outside the separatrix has all the phase space curves which correspond to the pendulum continuously turning through vertical planar circles.
33:
385:
238:
580:
495:
620:
586:
which is nearly circular for small H and becomes "eye" shaped when H approaches the upper bound. These curves correspond to the pendulum swinging periodically from side to side.
660:
752:. Since when solving for the trajectories forwards in time, trajectories diverge from the separatrix, when solving backwards in time, trajectories converge to the separatrix.
524:
444:
723:
415:
305:
261:
281:
316:
50:
741:. Trajectories to the left of the separatrix converge to the left stable equilibrium, and similarly for the right. The separatrix itself is the
164:
97:
536:
116:
69:
76:
138:
54:
737:, when the linear nullcline pierces the cubic nullcline at the left, middle, and right branch once each, the system has a
83:
812:
284:
65:
734:
464:
307:
the angle between the pendulum and vertically downwards. In this system there is a conserved quantity H (the
592:
446:
on the vertical axis – see the thumbnail to the right. The type of resulting curve depends upon the value of
43:
670:
632:
622:
then the curve is open, and this corresponds to the pendulum forever swinging through complete circles.
308:
500:
420:
677:
725:, we can easily see the separatrix and the two basins of attraction by solving for the trajectories
453:
90:
17:
400:
290:
246:
742:
527:
266:
806:
380:{\displaystyle H={\frac {{\dot {\theta }}^{2}}{2}}-{\frac {g}{\ell }}\cos \theta .}
394:
130:
32:
792:
796:
748:
The separatrix is clearly visible by numerically solving for trajectories
233:{\displaystyle {d^{2}\theta \over dt^{2}}+{g \over \ell }\sin \theta =0.}
155:
154:
Consider the differential equation describing the motion of a simple
745:
for the saddle point in the middle. Details are found in the page.
669:
583:
452:
575:{\displaystyle -{\frac {g}{\ell }}<H<{\frac {g}{\ell }}}
26:
782:, 3rd Ed., 2006, John Wiley and Sons, Hoboken, NJ, pg. 65.
137:
is the boundary separating two modes of behaviour in a
680:
635:
595:
539:
503:
467:
423:
403:
319:
293:
269:
249:
167:
389:
With this defined, one can plot a curve of constant
57:. Unsourced material may be challenged and removed.
771:, 4th ed., 2012, Brooks/Cole, Boston, MA, pg. 469.
717:
654:
614:
574:
518:
489:
438:
409:
379:
299:
275:
255:
232:
8:
397:of system. The phase space is a graph with
697:
679:
642:
634:
596:
594:
562:
543:
538:
505:
504:
502:
477:
466:
425:
424:
422:
402:
355:
341:
330:
329:
326:
318:
292:
268:
248:
205:
193:
175:
168:
166:
117:Learn how and when to remove this message
490:{\displaystyle H<-{\frac {g}{\ell }}}
760:
615:{\displaystyle {\frac {g}{\ell }}<H}
582:then the curve will be a simple closed
457:The phase space for the simple pendulum
7:
655:{\displaystyle H={\frac {g}{\ell }}}
263:denotes the length of the pendulum,
55:adding citations to reliable sources
25:
629:is the curve that corresponds to
519:{\displaystyle {\dot {\theta }}}
439:{\displaystyle {\dot {\theta }}}
31:
718:{\displaystyle b=2,I_{ext}=3.5}
42:needs additional citations for
497:then no curve exists (because
417:along the horizontal axis and
18:Separatrix (dynamical systems)
1:
66:"Separatrix" mathematics
829:
285:gravitational acceleration
410:{\displaystyle \theta }
300:{\displaystyle \theta }
769:Differential Equations
730:
719:
656:
616:
576:
520:
491:
458:
440:
411:
381:
301:
277:
257:
234:
735:FitzHugh–Nagumo model
720:
673:
666:FitzHugh–Nagumo model
657:
617:
577:
521:
492:
456:
441:
412:
382:
311:), which is given by
302:
278:
258:
256:{\displaystyle \ell }
235:
139:differential equation
678:
633:
593:
537:
501:
465:
421:
401:
317:
291:
267:
247:
165:
51:improve this article
780:Applied Mathematics
625:In this system the
731:
715:
652:
612:
572:
516:
487:
459:
436:
407:
377:
297:
273:
253:
230:
813:Dynamical systems
778:Logan, J. David,
767:Blanchard, Paul,
750:backwards in time
650:
604:
570:
551:
513:
485:
433:
363:
350:
338:
276:{\displaystyle g}
213:
200:
127:
126:
119:
101:
16:(Redirected from
820:
772:
765:
724:
722:
721:
716:
708:
707:
661:
659:
658:
653:
651:
643:
621:
619:
618:
613:
605:
597:
581:
579:
578:
573:
571:
563:
552:
544:
525:
523:
522:
517:
515:
514:
506:
496:
494:
493:
488:
486:
478:
445:
443:
442:
437:
435:
434:
426:
416:
414:
413:
408:
386:
384:
383:
378:
364:
356:
351:
346:
345:
340:
339:
331:
327:
306:
304:
303:
298:
282:
280:
279:
274:
262:
260:
259:
254:
239:
237:
236:
231:
214:
206:
201:
199:
198:
197:
184:
180:
179:
169:
122:
115:
111:
108:
102:
100:
59:
35:
27:
21:
828:
827:
823:
822:
821:
819:
818:
817:
803:
802:
789:
775:
766:
762:
758:
743:stable manifold
693:
676:
675:
668:
631:
630:
591:
590:
535:
534:
499:
498:
463:
462:
419:
418:
399:
398:
328:
315:
314:
289:
288:
265:
264:
245:
244:
189:
185:
171:
170:
163:
162:
152:
150:Simple pendulum
147:
123:
112:
106:
103:
60:
58:
48:
36:
23:
22:
15:
12:
11:
5:
826:
824:
816:
815:
805:
804:
801:
800:
788:
787:External links
785:
784:
783:
774:
773:
759:
757:
754:
714:
711:
706:
703:
700:
696:
692:
689:
686:
683:
667:
664:
649:
646:
641:
638:
611:
608:
603:
600:
569:
566:
561:
558:
555:
550:
547:
542:
512:
509:
484:
481:
476:
473:
470:
432:
429:
406:
376:
373:
370:
367:
362:
359:
354:
349:
344:
337:
334:
325:
322:
296:
272:
252:
241:
240:
229:
226:
223:
220:
217:
212:
209:
204:
196:
192:
188:
183:
178:
174:
151:
148:
146:
143:
125:
124:
107:September 2012
39:
37:
30:
24:
14:
13:
10:
9:
6:
4:
3:
2:
825:
814:
811:
810:
808:
798:
794:
791:
790:
786:
781:
777:
776:
770:
764:
761:
755:
753:
751:
746:
744:
740:
736:
728:
712:
709:
704:
701:
698:
694:
690:
687:
684:
681:
672:
665:
663:
647:
644:
639:
636:
628:
623:
609:
606:
601:
598:
587:
585:
567:
564:
559:
556:
553:
548:
545:
540:
531:
529:
510:
507:
482:
479:
474:
471:
468:
455:
451:
449:
430:
427:
404:
396:
392:
387:
374:
371:
368:
365:
360:
357:
352:
347:
342:
335:
332:
323:
320:
312:
310:
294:
286:
270:
250:
227:
224:
221:
218:
215:
210:
207:
202:
194:
190:
186:
181:
176:
172:
161:
160:
159:
157:
149:
144:
142:
140:
136:
132:
121:
118:
110:
99:
96:
92:
89:
85:
82:
78:
75:
71:
68: –
67:
63:
62:Find sources:
56:
52:
46:
45:
40:This article
38:
34:
29:
28:
19:
779:
768:
763:
749:
747:
738:
732:
726:
626:
624:
588:
532:
460:
447:
390:
388:
313:
242:
153:
134:
128:
113:
104:
94:
87:
80:
73:
61:
49:Please help
44:verification
41:
395:phase space
309:Hamiltonian
131:mathematics
793:Separatrix
756:References
739:separatrix
627:separatrix
135:separatrix
77:newspapers
797:MathWorld
727:backwards
648:ℓ
602:ℓ
568:ℓ
549:ℓ
541:−
528:imaginary
511:˙
508:θ
483:ℓ
475:−
431:˙
428:θ
405:θ
372:θ
369:
361:ℓ
353:−
336:˙
333:θ
295:θ
251:ℓ
222:θ
219:
211:ℓ
182:θ
807:Category
729:in time.
526:must be
156:pendulum
145:Examples
733:In the
393:in the
91:scholar
243:where
93:
86:
79:
72:
64:
795:from
674:When
584:curve
98:JSTOR
84:books
607:<
560:<
554:<
472:<
287:and
283:the
133:, a
70:news
713:3.5
589:If
533:If
530:).
461:If
366:cos
216:sin
129:In
53:by
809::
450:.
228:0.
158::
141:.
799:.
710:=
705:t
702:x
699:e
695:I
691:,
688:2
685:=
682:b
645:g
640:=
637:H
610:H
599:g
565:g
557:H
546:g
480:g
469:H
448:H
391:H
375:.
358:g
348:2
343:2
324:=
321:H
271:g
225:=
208:g
203:+
195:2
191:t
187:d
177:2
173:d
120:)
114:(
109:)
105:(
95:·
88:·
81:·
74:·
47:.
20:)
Text is available under the Creative Commons Attribution-ShareAlike License. Additional terms may apply.