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Self-oscillation

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17: 353:, this makes the populations of predators of that species decline, the reduced level of predation allows the herbivore population to increase, this allows the predator population to increase, etc. Closed loops of time-lagged differential equations are a sufficient explanation for such cycles - in this case the delays are caused mainly by the breeding cycles of the species involved. 202:
criteria. The amplitude of the oscillation of an unstable system grows exponentially with time (i.e., small oscillations are negatively damped), until nonlinearities become important and limit the amplitude. This can produce a steady and sustained oscillation. In some cases, self-oscillation can be
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designs when the vehicle was traveling at a speed which was between the ideal speeds of 2 gears. In these situations the transmission system would switch almost continuously between the 2 gears, which was both annoying and hard on the transmission. Such behavior is now inhibited by introducing
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Many early radio systems tuned their transmitter circuit, so the system automatically created radio waves of the desired frequency. This design has given way to designs that use a separate oscillator to provide a signal that is then amplified to the desired power.
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is the generation and maintenance of a periodic motion by a source of power that lacks any corresponding periodicity. The oscillator itself controls the phase with which the external power acts on it. Self-oscillators are therefore distinct from
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The same phenomenon is sometimes labelled as "maintained", "sustained", "self-exciting", "self-induced", "spontaneous", or "autonomous" oscillation. Unwanted self-oscillations are known in the mechanical engineering literature as
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There are many examples of self-exciting oscillation caused by delayed course corrections, ranging from light aircraft in a strong wind to erratic steering of road vehicles by a driver who is inexperienced or drunk.
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that acts on the oscillator. If the power is modulated in phase with the oscillator's velocity, a negative damping is established and the oscillation grows until limited by nonlinearities.
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considered various instances of mechanical and acoustic self-oscillations (which he called "maintained vibration") and offered a simple mathematical model for them.
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that he showed correspond to electrical oscillations with frequencies of hundreds of millions of cycles per second. Hertz's work led to the development of
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between the oscillation and the modulation of the external source of power. The amplitude and waveform of steady self-oscillations are determined by the
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Alicki, Robert; Horodecki, Michal; Jenkins, Alejandro; Lobejko, Marcin; Suarez, Gerardo (2023). "The Josephson junction as a quantum engine".
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Simple mathematical models of self-oscillators involve negative linear damping and positive non-linear damping terms, leading to a
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is connected to a capacitor and the shaft turns above synchronous speed, it operates as a self-excited induction generator.
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can cause an uncomfortable wobbling effect, which in extreme cases can derail trains and cause cars to lose grip.
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term, which causes small perturbations to grow exponentially in amplitude. This negative damping is due to a
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produce the human voice. Another instance of self-oscillation, associated with the unstable operation of
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were guilty of self-exciting oscillation because they responded too quickly. The problem was overcome by
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The term "self-oscillation" (also translated as "auto-oscillation") was coined by the Soviet physicist
83: 549: 157: 372: 292: 233: 191: 161: 129:. The first detailed theoretical work on such electrical self-oscillation was carried out by 173: 153: 118: 49: 20:
Schematic representation of a self-oscillation as a positive feedback loop. The oscillator
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Self-oscillation is manifested as a linear instability of a dynamical system's static
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is one such model that has been used extensively in the mathematical literature.
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Self-oscillations are important in physics, engineering, biology, and economics.
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Interest in the subject of self-oscillation was also stimulated by the work of
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The study of self-oscillators dates back to the early 1830s, with the work of
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For example, a reduction in population of an herbivore species because of
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Steering of vehicles when course corrections are delayed
102:in 1867. In the second edition of his treatise on 531: 244: 32:uses this signal to modulate the external power 338: 270: 324: 405: 403: 401: 399: 397: 395: 393: 291:Self-exciting oscillation occurred in early 333: 207:system, which makes the change in variable 468:Proceedings of the Royal Society of London 466:Maxwell, J. Clerk (1867). "On Governors". 286: 239: 506: 426: 390: 77: 15: 465: 409: 313:SEIG (self-excited induction generator) 203:seen as resulting from a time lag in a 117:, starting in 1887, in which he used a 69:nonlinear characteristics of the system 532: 459: 179: 186:Oscillation (differential equation) 13: 14: 591: 486: 98:, was studied mathematically by 575:Ordinary differential equations 221:evaluated at an earlier time. 90:on the mechanism by which the 1: 445:10.1016/j.physrep.2012.10.007 383: 245:Railway and automotive wheels 413:(2013). "Self-oscillation". 339:Population cycles in biology 7: 356: 271:Central heating thermostats 133:in the early 20th century. 24:produces a feedback signal 10: 596: 342: 325:Self-exciting transmitters 214:dependent on the variable 183: 517:10.1088/1367-2630/ad06d8 334:Examples in other fields 172:, and in electronics as 345:Lotka–Volterra equation 287:Automatic transmissions 240:Examples in engineering 164:in the 20th century. 495:New Journal of Physics 373:Van der Pol oscillator 293:automatic transmission 275:Early central heating 234:van der Pol oscillator 228:and the appearance of 174:parasitic oscillations 162:Philippe Le Corbeiller 78:History of the subject 37: 565:Mechanical vibrations 343:Further information: 154:Balthasar van der Pol 119:spark-gap transmitter 106:, published in 1896, 96:centrifugal governors 50:parametric resonators 28:. The controller at 19: 158:Alfred-Marie LiĂ©nard 142:structural stability 437:2013PhR...525..167J 250:Hunting oscillation 127:wireless telegraphy 104:The Theory of Sound 100:James Clerk Maxwell 88:George Biddell Airy 570:Physical phenomena 411:Jenkins, Alejandro 378:Hidden oscillation 180:Mathematical basis 138:Aleksandr Andronov 38: 560:Nonlinear systems 555:Dynamical systems 300:into the system. 146:dynamical systems 65:positive feedback 587: 521: 520: 510: 490: 484: 483: 463: 457: 456: 430: 407: 363:Hopf bifurcation 226:Hopf bifurcation 41:Self-oscillation 595: 594: 590: 589: 588: 586: 585: 584: 530: 529: 525: 524: 491: 487: 464: 460: 415:Physics Reports 408: 391: 386: 359: 347: 341: 336: 327: 319:induction motor 315: 306: 289: 273: 247: 242: 219: 212: 188: 182: 80: 12: 11: 5: 593: 583: 582: 577: 572: 567: 562: 557: 552: 550:Systems theory 547: 542: 523: 522: 485: 458: 421:(2): 167–222. 388: 387: 385: 382: 381: 380: 375: 370: 365: 358: 355: 340: 337: 335: 332: 326: 323: 314: 311: 305: 302: 288: 285: 272: 269: 263:in automotive 246: 243: 241: 238: 217: 210: 184:Main article: 181: 178: 131:Henri PoincarĂ© 115:Heinrich Hertz 79: 76: 57:linear systems 9: 6: 4: 3: 2: 592: 581: 578: 576: 573: 571: 568: 566: 563: 561: 558: 556: 553: 551: 548: 546: 543: 541: 538: 537: 535: 528: 518: 514: 509: 504: 500: 496: 489: 481: 477: 473: 469: 462: 454: 450: 446: 442: 438: 434: 429: 424: 420: 416: 412: 406: 404: 402: 400: 398: 396: 394: 389: 379: 376: 374: 371: 369: 366: 364: 361: 360: 354: 352: 346: 331: 322: 320: 310: 301: 299: 294: 284: 282: 278: 268: 266: 262: 258: 255: 251: 237: 235: 231: 227: 222: 220: 213: 206: 201: 197: 196:Routh–Hurwitz 193: 187: 177: 175: 171: 165: 163: 159: 155: 151: 150:AndrĂ© Blondel 147: 143: 139: 134: 132: 128: 124: 120: 116: 111: 109: 108:Lord Rayleigh 105: 101: 97: 93: 89: 85: 84:Robert Willis 75: 72: 70: 66: 62: 58: 53: 51: 47: 42: 35: 31: 27: 23: 18: 526: 498: 494: 488: 471: 467: 461: 418: 414: 348: 328: 316: 307: 290: 274: 248: 230:limit cycles 223: 215: 208: 189: 166: 135: 121:to generate 112: 103: 81: 73: 54: 40: 39: 33: 29: 25: 21: 540:Oscillators 474:: 270–283. 368:Limit cycle 277:thermostats 205:closed loop 192:equilibrium 123:radio waves 92:vocal cords 545:Amplifiers 534:Categories 508:2302.04762 501:: 113013. 384:References 298:hysteresis 281:hysteresis 453:227438422 428:1109.6640 351:predation 580:Feedback 357:See also 433:Bibcode 254:railway 232:. The 200:Nyquist 170:hunting 61:damping 480:112510 478:  451:  317:If an 261:shimmy 257:wheels 160:, and 46:forced 503:arXiv 476:JSTOR 449:S2CID 423:arXiv 265:tires 259:and 198:and 86:and 71:. 48:and 513:doi 441:doi 419:525 252:in 218:t-1 144:of 55:In 536:: 511:. 499:25 497:. 472:16 470:. 447:. 439:. 431:. 417:. 392:^ 176:. 156:, 152:, 527:. 519:. 515:: 505:: 482:. 455:. 443:: 435:: 425:: 216:x 211:t 209:x 34:S 30:R 26:B 22:V

Index


forced
parametric resonators
linear systems
damping
positive feedback
nonlinear characteristics of the system
Robert Willis
George Biddell Airy
vocal cords
centrifugal governors
James Clerk Maxwell
Lord Rayleigh
Heinrich Hertz
spark-gap transmitter
radio waves
wireless telegraphy
Henri Poincaré
Aleksandr Andronov
structural stability
dynamical systems
André Blondel
Balthasar van der Pol
Alfred-Marie Liénard
Philippe Le Corbeiller
hunting
parasitic oscillations
Oscillation (differential equation)
equilibrium
Routh–Hurwitz

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