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RC oscillator

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power supply rails. The net effect is the oscillator amplitude will stabilize when average gain over a cycle is one. If the average loop gain is greater than one, the output amplitude increases until the nonlinearity reduces the average gain to one; if the average loop gain is less than one, then the output amplitude decreases until the average gain is one. The nonlinearity that reduces the gain may also be more subtle than running into a power supply rail.
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in the output signal. If the small-signal gain is just a little bit more than one, then only a small amount of gain compression is needed, so there won't be much harmonic distortion. If the small-signal gain is much more than one, then significant distortion will be present. However the oscillator
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components is unstable with respect to amplitude. As long as the loop gain is exactly one, the amplitude of the sine wave would be constant, but the slightest increase in gain, due to a drift in the value of components will cause the amplitude to increase exponentially without limit. Similarly, the
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together mechanically on the same shaft. The oscillation frequency is proportional to the inverse of the capacitance or resistance, whereas in an LC oscillator the frequency is proportional to inverse square root of the capacitance or inductance. So a much wider frequency range can be covered by a
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works in a similar fashion). The lamp both measures the output amplitude and controls the oscillator gain at the same time. The oscillator's signal level heats the filament. If the level is too high, then the filament temperature gradually increases, the resistance increases, and the loop gain falls
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needed for the LC oscillator become cumbersome, and RC oscillators are used instead. Their lack of bulky inductors also makes them easier to integrate into microelectronic devices. Since the oscillator's frequency is determined by the value of resistors and capacitors, which vary with temperature,
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As the peaks of the sine wave approach the supply rails, the saturation of the amplifier device flattens (clips) the peaks, reducing the gain. For example, the oscillator might have a loop gain of 3 for small signals, but that loop gain instaneously drops to zero when the output reaches one of the
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This makes tuning the circuit to different frequencies more difficult than in other types such as the LC oscillator, in which the frequency is determined by a single LC circuit so only one element must be varied. Although the frequency can be varied over a small range by adjusting a single circuit
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In most ordinary oscillators, the nonlinearity is simply the saturation (clipping) of the amplifier as the amplitude of the sine wave approaches the power supply rails. The oscillator is designed to have a small-signal loop gain greater than one. The higher gain allows an oscillator to start by
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In RC oscillator circuits which use a single inverting amplifying device, such as a transistor, tube, or an op amp with the feedback applied to the inverting input, the amplifier provides 180° of the phase shift, so the RC network must provide the other 180°. Since each capacitor can provide a
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slightest decrease will cause the sine wave to die out exponentially to zero. Therefore, all practical oscillators must have a nonlinear component in the feedback loop, to reduce the gain as the amplitude increases, leading to stable operation at the amplitude where the loop gain is unity.
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to compensate for the energy lost as the signal passes through the feedback network, to create sustained oscillations. As long as the gain of the amplifier is high enough that the total gain around the loop is unity or higher, the circuit will generally oscillate.
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given variable capacitor in an RC oscillator. For example, a variable capacitor that could be varied over a 9:1 capacitance range will give an RC oscillator a 9:1 frequency range, but in an LC oscillator it will give only a 3:1 range.
493:. Together, these circuits form a bridge which is tuned at the desired frequency of oscillation. The signal in the C-R-C branch of the Twin-T filter is advanced, in the R-C-R - delayed, so they may cancel one another for frequency 651:) subtracting a constant, and applying the difference to a multiplier that adjusts the loop gain around an inverter. Such circuits have a near-instant amplitude response to the constant input and extremely low distortion. 200:(the amplification around the feedback loop) is equal to one. The purpose of the feedback RC network is to provide the correct phase shift at the desired oscillating frequency so the loop has 360° phase shift, so the 639:
integrators in a feedback loop, one with the signal applied to the inverting input or two integrators and an invertor. The advantage of this circuit is that the sinusoidal outputs of the two op-amps are 90°
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Wien bridge oscillator with automatic gain control. Rb is a small incandescent lamp. Usually, R1 = R2 = R and C1 = C2 = C. In normal operation, Rb self heats to the point where its resistance is Rf/2.
363: 308: 417: 1159: 467: 1092:, p. 664, "Alternatively, an amplitude-controlled resistor or other passive nonlinear element may be included as part of the amplifier or in the frequency-determining network." 535: 625: 743:. In this circuit, two RC circuits are used, one with the RC components in series and one with the RC components in parallel. The Wien Bridge is often used in audio 561: 204:, after passing through the loop will be in phase with the sine wave at the beginning and reinforce it, resulting in positive feedback. The amplifier provides 751:
or a two section variable potentiometer (which is more easily obtained than a variable capacitor suitable for generation at low frequencies). The archetypical
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the feedback network is three identical cascaded RC sections. In the simplest design the capacitors and resistors in each section have the same value
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Another common design is the "Twin-T" oscillator as it uses two "T" RC circuits operated in parallel. One circuit is an R-C-R "T" which acts as a
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The feedback network has an attenuation of 1/29, so the op-amp must have a gain of 29 to give a loop gain of one for the circuit to oscillate
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element, to tune an RC oscillator over a wide range two or more resistors or capacitors must be varied in unison, requiring them to be
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The Barkhausen criterion mentioned above does not determine the amplitude of oscillation. An oscillator circuit with only
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maximum of 90° of phase shift, RC oscillators require at least two frequency-determining capacitors in the circuit (two
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It is possible to stabilize a quadrature oscillator by squaring the sine and cosine outputs, adding them together, (
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in the small-signal region, the amplitude will build up until the limiter stabilizes the system...."
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Strauss, Leonard (1970), "Almost Sinusoidal Oscillations — the linear approximation",
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to an amplifier, and x>2, the amplifier becomes an oscillator. (Note:
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Some examples of common RC oscillator circuits are listed below:
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is equal to 360° (2π radians) or a multiple of 360°, and the
953:. India: Pearson Education India. pp. 8.2–8.6, 8.11. 685:
So in oscillators that must produce a very low-distortion
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must have gain significantly above one to start reliably.
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RC oscillators do not have as good frequency stability as
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Amplitude of Oscillation—Part II, Automatic Gain Control
489:. The second circuit is a C-R-C "T" which operates as a 1016:, Technical Manuals, Dover, pp. 178–179, TM 11-690 739:
One of the most common gain-stabilized circuits is the
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in the feedback circuit. These oscillators exploit the
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oscillator; they consist of an amplifying device, a
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may be too technical for most readers to understand
974:Eric Coates, 2015, AF Sine Wave Oscillators, p. 10 778:"Application Report SLOA060: Sine-Wave Oscillator" 670:exponentially amplifying some ever-present noise. 619: 555: 529: 461: 411: 357: 302: 184:The frequency of oscillation is determined by the 861:"Oscillators Module 3 - AF Sine Wave Oscillators" 412:{\displaystyle f={\frac {1}{2\pi RC{\sqrt {6}}}}} 108:, for its frequency selective part is called an 1430: 1031:(second ed.), McGraw-Hill, pp. 663–720 755:audio oscillator is a Wien Bridge oscillator. 1160: 888: 775: 654: 96:. A linear oscillator circuit which uses an 947:Rao, B.; Rajeswari, K.; Pantulu, P. (2012). 882: 776:Mancini, Ron; Palmer, Richard (March 2001). 635:The quadrature oscillator uses two cascaded 1014:Basic Theory and Application of Transistors 984: 895:. New Age International. pp. 224–225. 892:Electronics (fundamentals And Applications) 708:of the lamp increases in proportion to its 462:{\displaystyle R_{\mathrm {fb} }=29\cdot R} 1174: 1167: 1153: 978: 916: 914: 912: 834:"Oscillators Module 1 - Oscillator Basics" 800: 798: 677:The result of this gain averaging is some 347: 343: 336: 332: 325: 321: 292: 288: 281: 277: 270: 266: 771: 769: 767: 728: 240: 59:Learn how and when to remove this message 43:, without removing the technical details. 804: 719: 630: 471: 231: 164:and electronic musical instruments. At 1101: 1089: 1077: 1066:Exponential limiting—bipolar transistor 1061: 1049: 1026: 909: 795: 1431: 967: 858: 852: 831: 825: 764: 530:{\displaystyle f={\frac {1}{2\pi RC}}} 1148: 41:make it understandable to non-experts 480: 15: 13: 940: 649:Pythagorean trigonometric identity 441: 438: 84:output signal, are composed of an 14: 1450: 1126: 1033:at page 661, "It follows that if 1233:Armstrong or Meissner oscillator 1132: 1012:Department of the Army (1962) , 160:, in such applications as audio 20: 1111: 1095: 1083: 1071: 1055: 1043: 1020: 1005: 1190:Barkhausen stability criterion 991:. Elsevier. pp. 397–398. 988:Frequency of Self-Oscillations 115: 1: 808:Practical Oscillator Handbook 758: 620:{\displaystyle x=C2/C1=R1/R2} 120:RC oscillators are a type of 1403:Transmission-line oscillator 985:Groszkowski, Janusz (2013). 811:. Elsevier. pp. 49–53. 7: 1205:Nyquist stability criterion 1118:Department of the Army 1962 1029:Wave Generation and Shaping 950:Electronic Circuit Analysis 10: 1455: 1388:Opto-electronic oscillator 889:Chattopadhyay, D. (2006). 732: 655:Low distortion oscillators 563:; if it is connected as a 244: 1370: 1337: 1309: 1281: 1258:Meacham bridge oscillator 1223: 1182: 922:"RC Feedback Oscillators" 805:Gottlieb, Irving (1997). 1357:Pearson–Anson oscillator 236:A phase-shift oscillator 868:Learn About Electronics 838:Learn About Electronics 783:. Texas Instruments Inc 1439:Electronic oscillators 1339:Relaxation oscillators 1301:Wien bridge oscillator 1291:Phase-shift oscillator 1210:Oscillator phase noise 1176:Electronic oscillators 741:Wien bridge oscillator 735:Wien bridge oscillator 729:Wien bridge oscillator 725: 621: 557: 531: 477: 463: 413: 359: 304: 253:phase-shift oscillator 247:Phase-shift oscillator 241:Phase-shift oscillator 237: 1383:Delay-line oscillator 859:Coates, Eric (2015). 832:Coates, Eric (2015). 723: 631:Quadrature oscillator 622: 558: 532: 475: 464: 414: 360: 305: 235: 92:selective element, a 75:electronic oscillator 1141:at Wikimedia Commons 1104:, pp. 706–713, 1064:, pp. 703–706, 926:Electronics tutorial 571: 541: 497: 429: 372: 314: 259: 186:Barkhausen criterion 1408:Klystron oscillator 1398:Robinson oscillator 1347:Blocking oscillator 1243:Colpitts oscillator 1195:Harmonic oscillator 679:harmonic distortion 556:{\displaystyle x=2} 476:A twin-T oscillator 179:crystal oscillators 100:, a combination of 80:, which generate a 1329:Tri-tet oscillator 1311:Quartz oscillators 1253:Lampkin oscillator 1248:Hartley oscillator 1120:, pp. 179–180 749:variable capacitor 726: 617: 553: 527: 478: 459: 409: 355: 354: 300: 299: 238: 1426: 1425: 1378:Cavity oscillator 1324:Pierce oscillator 1319:Butler oscillator 1296:Twin-T oscillator 1268:Vackář oscillator 1263:Seiler oscillator 1200:Leeson's equation 1137:Media related to 745:signal generators 691:incandescent lamp 565:negative feedback 525: 481:Twin-T oscillator 407: 404: 166:radio frequencies 162:signal generators 158:audio frequencies 150:positive feedback 69: 68: 61: 1446: 1413:Cavity magnetron 1238:Clapp oscillator 1169: 1162: 1155: 1146: 1145: 1136: 1121: 1115: 1109: 1099: 1093: 1087: 1081: 1075: 1069: 1059: 1053: 1047: 1041: 1039: 1032: 1024: 1018: 1017: 1009: 1003: 1002: 982: 976: 971: 965: 964: 944: 938: 937: 935: 933: 928:. DAEnotes. 2013 918: 907: 906: 886: 880: 879: 877: 875: 865: 856: 850: 849: 847: 845: 829: 823: 822: 802: 793: 792: 790: 788: 782: 773: 626: 624: 623: 618: 610: 590: 562: 560: 559: 554: 536: 534: 533: 528: 526: 524: 507: 491:high-pass filter 468: 466: 465: 460: 446: 445: 444: 418: 416: 415: 410: 408: 406: 405: 400: 382: 364: 362: 361: 356: 309: 307: 306: 301: 64: 57: 53: 50: 44: 24: 23: 16: 1454: 1453: 1449: 1448: 1447: 1445: 1444: 1443: 1429: 1428: 1427: 1422: 1418:Gunn oscillator 1393:ring oscillator 1366: 1333: 1305: 1277: 1219: 1178: 1173: 1129: 1124: 1116: 1112: 1100: 1096: 1088: 1084: 1076: 1072: 1060: 1056: 1048: 1044: 1034: 1025: 1021: 1010: 1006: 999: 983: 979: 972: 968: 961: 945: 941: 931: 929: 920: 919: 910: 903: 887: 883: 873: 871: 863: 857: 853: 843: 841: 830: 826: 819: 803: 796: 786: 784: 780: 774: 765: 761: 737: 731: 657: 633: 606: 586: 572: 569: 568: 542: 539: 538: 511: 506: 498: 495: 494: 487:low-pass filter 483: 437: 436: 432: 430: 427: 426: 399: 386: 381: 373: 370: 369: 315: 312: 311: 260: 257: 256: 249: 243: 118: 65: 54: 48: 45: 37:help improve it 34: 25: 21: 12: 11: 5: 1452: 1442: 1441: 1424: 1423: 1421: 1420: 1415: 1410: 1405: 1400: 1395: 1390: 1385: 1380: 1374: 1372: 1368: 1367: 1365: 1364: 1359: 1354: 1349: 1343: 1341: 1335: 1334: 1332: 1331: 1326: 1321: 1315: 1313: 1307: 1306: 1304: 1303: 1298: 1293: 1287: 1285: 1283:RC oscillators 1279: 1278: 1276: 1275: 1273:resonant Royer 1270: 1265: 1260: 1255: 1250: 1245: 1240: 1235: 1229: 1227: 1225:LC oscillators 1221: 1220: 1218: 1217: 1212: 1207: 1202: 1197: 1192: 1186: 1184: 1180: 1179: 1172: 1171: 1164: 1157: 1149: 1143: 1142: 1139:RC oscillators 1128: 1127:External links 1125: 1123: 1122: 1110: 1094: 1082: 1070: 1054: 1042: 1019: 1004: 998:978-1483280301 997: 977: 966: 960:978-8131754283 959: 939: 908: 901: 881: 851: 824: 817: 794: 762: 760: 757: 733:Main article: 730: 727: 656: 653: 632: 629: 616: 613: 609: 605: 602: 599: 596: 593: 589: 585: 582: 579: 576: 552: 549: 546: 523: 520: 517: 514: 510: 505: 502: 482: 479: 470: 469: 458: 455: 452: 449: 443: 440: 435: 420: 419: 403: 398: 395: 392: 389: 385: 380: 377: 353: 350: 346: 342: 339: 335: 331: 328: 324: 320: 298: 295: 291: 287: 284: 280: 276: 273: 269: 265: 245:Main article: 242: 239: 117: 114: 67: 66: 28: 26: 19: 9: 6: 4: 3: 2: 1451: 1440: 1437: 1436: 1434: 1419: 1416: 1414: 1411: 1409: 1406: 1404: 1401: 1399: 1396: 1394: 1391: 1389: 1386: 1384: 1381: 1379: 1376: 1375: 1373: 1369: 1363: 1360: 1358: 1355: 1353: 1352:Multivibrator 1350: 1348: 1345: 1344: 1342: 1340: 1336: 1330: 1327: 1325: 1322: 1320: 1317: 1316: 1314: 1312: 1308: 1302: 1299: 1297: 1294: 1292: 1289: 1288: 1286: 1284: 1280: 1274: 1271: 1269: 1266: 1264: 1261: 1259: 1256: 1254: 1251: 1249: 1246: 1244: 1241: 1239: 1236: 1234: 1231: 1230: 1228: 1226: 1222: 1216: 1213: 1211: 1208: 1206: 1203: 1201: 1198: 1196: 1193: 1191: 1188: 1187: 1185: 1181: 1177: 1170: 1165: 1163: 1158: 1156: 1151: 1150: 1147: 1140: 1135: 1131: 1130: 1119: 1114: 1107: 1103: 1098: 1091: 1086: 1079: 1074: 1067: 1063: 1058: 1051: 1046: 1038:β > 1 1037: 1030: 1023: 1015: 1008: 1000: 994: 990: 989: 981: 975: 970: 962: 956: 952: 951: 943: 927: 923: 917: 915: 913: 904: 902:81-224-1780-9 898: 894: 893: 885: 870:. Eric Coates 869: 862: 855: 840:. Eric Coates 839: 835: 828: 820: 814: 810: 809: 801: 799: 779: 772: 770: 768: 763: 756: 754: 750: 746: 742: 736: 722: 718: 715: 711: 707: 704: 700: 696: 692: 688: 683: 680: 675: 671: 667: 664: 663: 652: 650: 645: 643: 638: 628: 614: 611: 607: 603: 600: 597: 594: 591: 587: 583: 580: 577: 574: 566: 550: 547: 544: 521: 518: 515: 512: 508: 503: 500: 492: 488: 474: 456: 453: 450: 447: 433: 425: 424: 423: 401: 396: 393: 390: 387: 383: 378: 375: 368: 367: 366: 351: 348: 344: 340: 337: 333: 329: 326: 322: 318: 296: 293: 289: 285: 282: 278: 274: 271: 267: 263: 254: 248: 234: 230: 227: 224: 218: 216: 210: 207: 203: 199: 195: 194:feedback loop 191: 187: 182: 180: 175: 171: 167: 163: 159: 155: 151: 148:, to achieve 147: 143: 139: 135: 131: 127: 123: 113: 111: 110:RC oscillator 107: 103: 99: 95: 91: 87: 83: 79: 76: 73: 63: 60: 52: 42: 38: 32: 29:This article 27: 18: 17: 1362:basic Royer 1282: 1113: 1105: 1102:Strauss 1970 1097: 1090:Strauss 1970 1085: 1078:Strauss 1970 1073: 1065: 1062:Strauss 1970 1057: 1050:Strauss 1970 1045: 1035: 1028: 1022: 1013: 1007: 987: 980: 969: 949: 942: 930:. 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Index

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make it understandable to non-experts
Learn how and when to remove this message
Linear
electronic oscillator
circuits
sinusoidal
amplifier
frequency
filter
RC network
resistors
capacitors
feedback
transistor
vacuum tube
op-amp
resistors
capacitors
RC network
positive feedback
frequencies
audio frequencies
signal generators
radio frequencies
inductors
capacitors
crystal oscillators
Barkhausen criterion
phase shift

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