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Separatrix (mathematics)

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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
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on the vertical axis – see the thumbnail to the right. The type of resulting curve depends upon the value of
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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
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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
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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: â€“  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:)

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Separatrix (dynamical systems)

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"Separatrix" mathematics
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mathematics
differential equation
pendulum
gravitational acceleration
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phase space

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FitzHugh–Nagumo model
separatrix
stable manifold
Separatrix
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Dynamical systems

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