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Intermittency

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307: 328: 316: 231: 32: 134: 389:, until it gets close to the orbit again and returns to the nearly periodic behaviour. Since the time spent near the periodic orbit depends sensitively on how closely the system entered its vicinity (in turn determined by what happened during the chaotic period) the length of each phase is unpredictable. 415:
flows, intermittency is seen in the irregular dissipation of kinetic energy and the anomalous scaling of velocity increments. Understanding and modeling atmospheric flow and turbulence under such conditions are further complicated by “turbulence intermittency,” which manifests as periods of strong
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Another kind, on-off intermittency, occurs when a previously transversally stable chaotic attractor with dimension less than the embedding space begins to lose stability. Near unstable orbits within the attractor orbits can escape into the surrounding space, producing a temporary burst before
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and other wall bounded shear flows, there are intermittent puffs that are central to the process of transition from laminar to turbulent flow. Intermittent behavior has also been experimentally demonstrated in circuit oscillators and chemical reactions.
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Experimentally, intermittency appears as long periods of almost periodic behavior interrupted by chaotic behavior. As control variables change, the chaotic behavior become more frequent until the system is fully chaotic. This progression is known as the
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showing intermittency. The system spends long periods close to the bright periodic orbit, occasionally moving away for phases of chaotic dynamics that cover the rest of the attractor. This is an example of Pomeau–Manneville
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The intermittency in logistic map can be understood by looking at the cobweb diagram for logistic map (iterated three times). In the cobweb diagram, there are almost-tangencies where the trajectory can be trapped for a long
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and Manneville described three routes to intermittency where a nearly periodic system shows irregularly spaced bursts of chaos. These (type I, II and III) correspond to the approach to a
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turbulent activity interspersed in a more quiescent airflow. It is also seen in the irregular alternation between turbulent and non-turbulent fluid that appear in turbulent
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F. Anselmet, Y. Gagne, E.J. Hopfinger, R.A. Antonia, High-order velocity structure functions in turbulent shear flows, Journal of Fluid Mechanics, vol. 140, 1984, pp. 63-89
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Allouche, Mohammad; Bou-Zeid, Elie; Ansorge, Cedrick; Katul, Gabriel G.; Chamecki, Marcelo; Acevedo, Otavio; Thanekar, Sham; Fuentes, Jose D. (1 April 2022).
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E.Ott and J.C. Sommerer, Blowout bifurcations: the occurrence of riddled basins and on-off intermittency, Physics Letters A, vol. 188, 1994, pp. 39–47
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Yves Pomeau and Paul Manneville, Intermittent Transition to Turbulence in Dissipative Dynamical Systems, Commun. Math. Phys. vol. 74, pp. 189–197 1980
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C. Meneveau and K.R. Sreenivasan, The multifractal nature of turbulent energy dissipation, Journal of Fluid Mechanics, vol. 224, 1991, pp. 429-484
471: 198: 96: 385:. Eventually the system gets far enough away from the periodic orbit to be affected by chaotic dynamics in the rest of the 170: 68: 613: 642: 217: 177: 115: 75: 263: 381:. In the apparently periodic phases the behaviour is only nearly periodic, slowly drifting away from an unstable 434: 352: 184: 82: 53: 49: 17: 559:"The Detection, Genesis, and Modeling of Turbulence Intermittency in the Stable Atmospheric Surface Layer" 166: 64: 378: 661: 626: 449: 439: 397: 370: 144: 42: 306: 315: 260:. The trajectory alternates between almost period-3 trajectories and chaotic trajectories. At 237: 327: 630: 191: 89: 8: 401: 634: 586: 638: 590: 578: 570: 374: 340: 331: 320: 482: 604: 230: 382: 655: 582: 574: 348: 558: 355:), or different forms of chaotic dynamics (crisis-induced intermittency). 452:(blinking) of organic molecules and colloidal quantum dots (nanocrystals) 417: 386: 366: 444: 421: 412: 408: 407:
Intermittent behaviour is commonly observed in fluid flows that are
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is the irregular alternation of phases of apparently periodic and
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Intermittent jumping between two potential wells in the driven
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In crisis-induced intermittency a chaotic attractor suffers a
556: 323:. This is an example of crisis-induced intermittency. 266: 240: 56:. Unsourced material may be challenged and removed. 411:or near the transition to turbulence. In highly 294: 252: 23:Irregular alternation different types of dynamics 653: 295:{\displaystyle r=1+{\sqrt {8}}\approx 3.8284} 620: 510:. Cambridge University Press. p. 323. 505: 420:and other turbulent free shear flows. In 469: 218:Learn how and when to remove this message 116:Learn how and when to remove this message 326: 314: 305: 229: 654: 602: 481:. Taylor & Francis. Archived from 154:Please improve this article by adding 302:a stable period-3 trajectory emerges. 127: 54:adding citations to reliable sources 25: 563:Journal of the Atmospheric Sciences 234:Intermittency in logistic map with 13: 614:Eindhoven University of Technology 470:Mingzhou Ding. Alwyn Scott (ed.). 14: 673: 479:Encyclopedia of Nonlinear Science 623:Intermittency in turbulent flows 132: 30: 41:needs additional citations for 550: 541: 532: 523: 514: 499: 463: 18:Intermittency (disambiguation) 1: 456: 393:returning to the attractor. 156:secondary or tertiary sources 361:intermittency route to chaos 7: 606:Intermittency in Turbulence 428: 379:period-doubling bifurcation 10: 678: 627:Cambridge University Press 621:Vassilicos, J. C. (2000). 508:Chaos in dynamical systems 450:Fluorescence intermittency 440:Crisis (dynamical systems) 435:Pomeau–Manneville scenario 353:Pomeau–Manneville dynamics 15: 253:{\displaystyle r=3.8282} 575:10.1175/JAS-D-21-0053.1 371:saddle-node bifurcation 603:Staicu, A. D. (2002). 336: 324: 312: 303: 296: 254: 143:relies excessively on 330: 318: 309: 297: 255: 233: 264: 238: 50:improve this article 16:For other uses, see 635:2000itf..book.....V 506:Edward Ott (2002). 402:basin of attraction 337: 325: 321:Duffing oscillator 313: 304: 292: 250: 662:Dynamical systems 341:dynamical systems 284: 228: 227: 220: 202: 126: 125: 118: 100: 669: 648: 617: 611: 595: 594: 569:(4): 1171–1190. 554: 548: 545: 539: 536: 530: 527: 521: 518: 512: 511: 503: 497: 496: 494: 493: 487: 476: 467: 377:, or an inverse 375:Hopf bifurcation 373:, a subcritical 332:Lorenz attractor 301: 299: 298: 293: 285: 280: 259: 257: 256: 251: 223: 216: 212: 209: 203: 201: 160: 136: 128: 121: 114: 110: 107: 101: 99: 58: 34: 26: 677: 676: 672: 671: 670: 668: 667: 666: 652: 651: 645: 629:. p. 288. 609: 599: 598: 555: 551: 546: 542: 537: 533: 528: 524: 519: 515: 504: 500: 491: 489: 485: 474: 472:"Intermittency" 468: 464: 459: 431: 279: 265: 262: 261: 239: 236: 235: 224: 213: 207: 204: 167:"Intermittency" 161: 159: 153: 149:primary sources 137: 122: 111: 105: 102: 65:"Intermittency" 59: 57: 47: 35: 24: 21: 12: 11: 5: 675: 665: 664: 650: 649: 643: 618: 597: 596: 549: 540: 531: 522: 513: 498: 461: 460: 458: 455: 454: 453: 447: 445:Turbulent flow 442: 437: 430: 427: 383:periodic orbit 291: 288: 283: 278: 275: 272: 269: 249: 246: 243: 226: 225: 140: 138: 131: 124: 123: 38: 36: 29: 22: 9: 6: 4: 3: 2: 674: 663: 660: 659: 657: 646: 644:0-521-79221-5 640: 636: 632: 628: 624: 619: 615: 608: 607: 601: 600: 592: 588: 584: 580: 576: 572: 568: 564: 560: 553: 544: 535: 526: 517: 509: 502: 488:on 2011-09-27 484: 480: 473: 466: 462: 451: 448: 446: 443: 441: 438: 436: 433: 432: 426: 423: 419: 414: 410: 405: 403: 399: 394: 390: 388: 384: 380: 376: 372: 368: 364: 362: 356: 354: 350: 346: 345:intermittency 342: 333: 329: 322: 317: 308: 289: 286: 281: 276: 273: 270: 267: 247: 244: 241: 232: 222: 219: 211: 200: 197: 193: 190: 186: 183: 179: 176: 172: 169: â€“  168: 164: 163:Find sources: 157: 151: 150: 146: 141:This article 139: 135: 130: 129: 120: 117: 109: 98: 95: 91: 88: 84: 81: 77: 74: 70: 67: â€“  66: 62: 61:Find sources: 55: 51: 45: 44: 39:This article 37: 33: 28: 27: 19: 622: 605: 566: 562: 552: 543: 534: 525: 516: 507: 501: 490:. Retrieved 483:the original 478: 465: 406: 395: 391: 365: 360: 357: 344: 338: 214: 205: 195: 188: 181: 174: 162: 142: 112: 103: 93: 86: 79: 72: 60: 48:Please help 43:verification 40: 387:state space 492:2006-04-07 457:References 351:dynamics ( 178:newspapers 145:references 76:newspapers 591:245955138 583:0022-4928 422:pipe flow 413:turbulent 409:turbulent 335:dynamics. 287:≈ 656:Category 429:See also 208:May 2023 106:May 2023 631:Bibcode 349:chaotic 192:scholar 90:scholar 641:  589:  581:  398:crisis 367:Pomeau 290:3.8284 248:3.8282 194:  187:  180:  173:  165:  92:  85:  78:  71:  63:  610:(PDF) 587:S2CID 486:(PDF) 475:(PDF) 311:time. 199:JSTOR 185:books 97:JSTOR 83:books 639:ISBN 579:ISSN 418:jets 171:news 69:news 571:doi 363:. 339:In 147:to 52:by 658:: 637:. 625:. 612:. 585:. 577:. 567:79 565:. 561:. 477:. 343:, 158:. 647:. 633:: 616:. 593:. 573:: 495:. 282:8 277:+ 274:1 271:= 268:r 245:= 242:r 221:) 215:( 210:) 206:( 196:· 189:· 182:· 175:· 152:. 119:) 113:( 108:) 104:( 94:· 87:· 80:· 73:· 46:. 20:.

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Duffing oscillator
Intermittency
Lorenz attractor
dynamical systems

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