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All-pass filter

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The phase equaliser based on T topology is the unbalanced equivalent of the lattice filter and has the same phase response. While the circuit diagram may look like a low pass filter it is different in that the two inductor branches are mutually coupled. This results in transformer action between
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relationship among various frequencies. Most types of filter reduce the amplitude (i.e. the magnitude) of the signal applied to it for some values of frequency, whereas the all-pass filter allows all frequencies through without changes in level.
2079:{\displaystyle H(z)={\frac {z^{-1}-{\overline {z_{0}}}}{1-z_{0}z^{-1}}}\times {\frac {z^{-1}-z_{0}}{1-{\overline {z_{0}}}z^{-1}}}={\frac {z^{-2}-2\Re (z_{0})z^{-1}+\left|{z_{0}}\right|^{2}}{1-2\Re (z_{0})z^{-1}+\left|z_{0}\right|^{2}z^{-2}}},\ } 1178: 2319: 513: 372: 840: 1352:, is a filter composed of lattice, or X-sections. With single element branches it can produce a phase shift up to 180°, and with resonant branches it can produce phase shifts up to 360°. The filter is an example of a 1544: 1034: 1259:ω=1/RC of the high-pass filter (i.e., when input frequency is 1/(2πRC)), the circuit introduces a 90° phase lead (i.e., output is in quadrature with input; the output appears to be advanced by a quarter 1660:
can be rotated in the complex plane by any angle and retain its all-pass magnitude characteristic. Complex pole-zero pairs in all-pass filters help control the frequency where phase shifts occur.
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They are generally used to compensate for other undesired phase shifts that arise in the system, or for mixing with an unshifted version of the original to implement a notch
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designs. In other applications where inductors are readily available, all-pass filters can be implemented entirely without active components. There are a number of circuit
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or mixed-phase filters to create a stable or minimum-phase filter without changing the magnitude response of the system. For example, by proper choice of
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typically consists of two, four or six of these phase-shifting sections connected in tandem and summed with the original. A low-frequency oscillator (
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To create an all-pass implementation with real coefficients, the complex all-pass filter can be cascaded with an all-pass that substitutes
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filter with an equivalent magnitude response or an unstable filter into a stable filter with an equivalent magnitude response.
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In fact, the phase shift of the all-pass filter is double the phase shift of the high-pass filter at its non-inverting input.
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In fact, the phase shift of the all-pass filter is double the phase shift of the low-pass filter at its non-inverting input.
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to implement a voltage-controlled phase shifter; the voltage on the gate adjusts the phase shift. In electronic music, a
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magnitude for all ω. The filter introduces a different delay at each frequency and reaches input-to-output
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magnitude for all ω. The filter introduces a different delay at each frequency and reaches input-to-output
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The bridged T topology is used for delay equalisation, particularly the differential delay between two
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shift as a function of frequency. Generally, the filter is described by the frequency at which the
2314:{\displaystyle y-2\Re (z_{0})y+\left|z_{0}\right|^{2}y=x-2\Re (z_{0})x+\left|z_{0}\right|^{2}x,\,} 1388: 1315: 1231: 1188: 577: 523: 508:{\displaystyle |H(i\omega )|=1\quad {\text{and}}\quad \angle H(i\omega )=-2\arctan(\omega RC).\,} 2655: 2545: 2526: 2522: 2464: 1619: 1207: 1064: 944: 612: 538: 402: 367:{\displaystyle H(s)=-{\frac {s-{\frac {1}{RC}}}{s+{\frac {1}{RC}}}}={\frac {1-sRC}{1+sRC}},\,} 238: 93: 2644: 2639: 2629: 2484: 2479: 2469: 1256: 1199: 1052: 940: 852: 587: 390: 177: 158: 2566: 2412: 1700: 1636: 1414: 2624: 2474: 1357: 1284: 889: 234: 162: 1622:. The pole and zero sit at the same angle but have reciprocal magnitudes (i.e., they are 2406: 2385: 2356: 2327: 651: 173: 923: 835:{\displaystyle e^{-sT}={\frac {e^{-sT/2}}{e^{sT/2}}}\approx {\frac {1-sT/2}{1+sT/2}},} 2668: 2459: 1627: 1223: 1060: 1056: 846: 554: 398: 394: 199: 195: 169: 145: 1245: 569: 1392: 2437: 1725: 1630: 1408: 1396: 188: 35: 1322:
that can be used for this. The following are the most commonly used circuits.
17: 181: 2582: 1260: 1241: 1219: 1215: 591: 565: 550: 546: 141: 1291:) ramps the control voltage to produce the characteristic swooshing sound. 1539:{\displaystyle H(z)={\frac {z^{-1}-{\overline {z_{0}}}}{1-z_{0}z^{-1}}}\ } 1384: 1311: 1399:) over a wide bandwidth and is the reason for choosing this topology. 1029:{\displaystyle H(s)={\frac {s-{\frac {1}{RC}}}{s+{\frac {1}{RC}}}},\,} 1369:
the two inductors and an all-pass response even at high frequency.
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An op-amp base all-pass filter incorporating a high-pass filter.
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Williams, A.B.; Taylor, F.J., Electronic Filter Design Handbook
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An op-amp base all-pass filter incorporating a low-pass filter.
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circuit shown in the adjacent figure implements a single-pole
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broadcasts. This application requires that the filter has a
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crosses 90° (i.e., when the input and output signals go into
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implementation of an all-pass filter with a complex pole at
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production is in the design of an effects unit known as a "
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circuit shown in adjacent figure implements a single-pole
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at the non-inverting input of the opamp. The filter's
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expansion of the numerator and denominator. By setting
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is complex frequency. This can be approximated using a
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Op Amps for Everyone, Ron Mancini, Newnes 780750677011
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can be canceled and reflected inside the unit circle.
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Interpretation as a Padé approximation to a pure delay
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at the non-inverting input of the opamp. The filter's
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Unsourced material may be challenged and removed. 2428: 2394: 2374: 2345: 2313: 2078: 1716: 1689: 1652: 1610: 1583: 1538: 1430: 1302:The benefit to implementing all-pass filters with 1172: 1028: 907: 878: 834: 688: 660: 637: 606:The Laplace transform of a pure delay is given by 533:This implementation uses a low-pass filter at the 507: 366: 2405:Filters such as the above can be cascaded with 2598: 8: 2605: 2591: 2583: 2420: 2414: 2387: 2358: 2329: 2310: 2289: 2279: 2240: 2179: 2169: 2130: 2100: 2058: 2048: 2038: 2017: 2004: 1977: 1966: 1961: 1944: 1931: 1906: 1899: 1884: 1869: 1863: 1849: 1833: 1826: 1811: 1801: 1778: 1772: 1760: 1753: 1736: 1708: 1702: 1676: 1670: 1668: 1644: 1638: 1626:of each other across the boundary of the 1598: 1596: 1570: 1564: 1559: 1554: 1521: 1511: 1488: 1482: 1470: 1463: 1446: 1422: 1416: 1334:An all-pass filter using lattice topology 1169: 1109: 1097: 1077: 1075: 1025: 1004: 981: 972: 955: 891: 868: 854: 818: 796: 781: 766: 759: 745: 735: 729: 714: 708: 682: 681: 673: 653: 620: 614: 561:(i.e., 180° phase shift) with unity gain. 504: 447: 435: 415: 413: 363: 322: 301: 278: 269: 249: 120:Learn how and when to remove this message 1395:response with frequency (i.e., constant 1329: 1252:(i.e., 180° phase lead) with unity gain. 2501: 2578:filter-solutions.com: All-pass filters 530:at ω=1/RC (i.e., phase shift is 90°). 180: – when there is a quarter 1584:{\displaystyle 1/{\overline {z_{0}}}} 1195:at ω=1/RC (i.e., phase lead is 90°). 919:Implementation using high-pass filter 7: 1275:The resistor can be replaced with a 213:Implementation using low-pass filter 58:adding citations to reliable sources 2382:is the input at discrete time step 1690:{\displaystyle {\overline {z_{0}}}} 1360:is constant over all frequencies). 194:They may also be used to convert a 2230: 2120: 1994: 1921: 1115: 453: 25: 1271:Voltage controlled implementation 689:{\displaystyle s\in \mathbb {C} } 144:equally in gain, but changes the 2567:JOS@Stanford on all-pass filters 2517:Maheswari, L.K.; Anand, M.M.S., 1314:, which are bulky and costly in 1206:to generate the phase shift and 939:all-pass filter that features a 537:to generate the phase shift and 233:all-pass filter that features a 34: 1611:{\displaystyle {\overline {z}}} 1114: 1108: 452: 446: 45:needs additional citations for 2369: 2363: 2340: 2334: 2304: 2298: 2264: 2252: 2246: 2233: 2221: 2209: 2200: 2188: 2154: 2142: 2136: 2123: 2111: 2105: 2010: 1997: 1937: 1924: 1747: 1741: 1457: 1451: 1163: 1151: 1130: 1121: 1098: 1094: 1085: 1078: 966: 960: 902: 896: 668:is the delay (in seconds) and 498: 486: 468: 459: 436: 432: 423: 416: 260: 254: 1: 2572:ECE 209 Phase-Shifter Circuit 1298:Passive analog implementation 1875: 1784: 1682: 1603: 1576: 1494: 1310:is that they do not require 206:Active analog implementation 168:It does this by varying its 2089:which is equivalent to the 1354:constant-resistance network 1198:This implementation uses a 2701: 1376: 1337: 2685:Digital signal processing 2680:Filter frequency response 2653: 2620: 2614:Signal-processing filters 2450:Bridged T delay equaliser 1379:Bridged T delay equaliser 1051:of each other across the 389:of each other across the 1373:Bridged T-section filter 1047:at 1/RC (i.e., they are 638:{\displaystyle e^{-sT},} 385:at 1/RC (i.e., they are 184:of delay between them). 157:A common application in 138:signal processing filter 27:Signal processing filter 2455:Lattice phase equaliser 1346:lattice phase equaliser 1340:Lattice phase equaliser 1240:At low frequencies and 583:(i.e., no phase shift). 564:At low frequencies and 2630:High-pass filter (HPF) 2430: 2396: 2376: 2347: 2315: 2080: 1718: 1691: 1654: 1612: 1585: 1540: 1432: 1403:Digital implementation 1335: 1308:operational amplifiers 1248:and the circuit is an 1244:, the capacitor is an 1237:(i.e., no phase lead). 1174: 1030: 928: 909: 880: 879:{\displaystyle RC=T/2} 836: 690: 662: 639: 568:, the capacitor is an 509: 368: 222: 2625:Low-pass filter (LPF) 2525:, PHI Learning, 2009 2490:Lattice delay network 2431: 2429:{\displaystyle z_{0}} 2397: 2377: 2348: 2316: 2081: 1719: 1717:{\displaystyle z_{0}} 1692: 1655: 1653:{\displaystyle z_{0}} 1613: 1586: 1541: 1433: 1431:{\displaystyle z_{0}} 1333: 1226:, thereby creating a 1175: 1031: 933:operational amplifier 926: 910: 881: 837: 691: 663: 640: 510: 369: 227:operational amplifier 220: 2544:, McGraw-Hill, 1995 2413: 2386: 2357: 2328: 2099: 1735: 1701: 1667: 1637: 1595: 1553: 1549:which has a zero at 1445: 1415: 1074: 954: 908:{\displaystyle H(s)} 890: 853: 707: 672: 652: 613: 412: 248: 54:improve this article 2091:difference equation 1250:inverting amplifier 1204:non-inverting input 1061:magnitude and phase 559:inverting amplifier 535:non-inverting input 399:magnitude and phase 153:Common applications 2519:Analog Electronics 2426: 2392: 2372: 2353:is the output and 2343: 2311: 2076: 1724:, leading to the 1714: 1687: 1650: 1608: 1581: 1536: 1428: 1389:stereophonic sound 1336: 1316:integrated circuit 1170: 1063:of H(iω) for some 1026: 929: 905: 876: 832: 686: 658: 635: 505: 401:of H(iω) for some 364: 223: 2662: 2661: 2656:Electronic filter 2465:Hilbert transform 2395:{\displaystyle k} 2375:{\displaystyle x} 2346:{\displaystyle y} 2075: 2068: 1894: 1878: 1821: 1787: 1685: 1620:complex conjugate 1606: 1579: 1535: 1531: 1497: 1304:active components 1208:negative feedback 1112: 1065:angular frequency 1043:at -1/RC and one 1020: 1017: 994: 945:transfer function 827: 776: 661:{\displaystyle T} 539:negative feedback 450: 403:angular frequency 381:at -1/RC and one 358: 317: 314: 291: 239:transfer function 130: 129: 122: 104: 69:"All-pass filter" 16:(Redirected from 2692: 2645:Band-stop filter 2640:Band-pass filter 2607: 2600: 2593: 2584: 2554: 2540: 2534: 2515: 2509: 2506: 2485:Band-pass filter 2480:Band-stop filter 2470:High-pass filter 2435: 2433: 2432: 2427: 2425: 2424: 2401: 2399: 2398: 2393: 2381: 2379: 2378: 2373: 2352: 2350: 2349: 2344: 2320: 2318: 2317: 2312: 2294: 2293: 2288: 2284: 2283: 2245: 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filter 914: 912: 911: 906: 885: 883: 882: 877: 872: 841: 839: 838: 833: 828: 826: 822: 804: 800: 782: 777: 775: 774: 770: 754: 753: 749: 730: 725: 724: 698:Padé approximant 695: 693: 692: 687: 685: 667: 665: 664: 659: 644: 642: 641: 636: 631: 630: 594:from the input). 588:corner frequency 514: 512: 511: 506: 451: 448: 439: 419: 373: 371: 370: 365: 359: 357: 340: 323: 318: 316: 315: 313: 302: 293: 292: 290: 279: 270: 159:electronic music 140:that passes all 125: 118: 114: 111: 105: 103: 62: 38: 30: 21: 2700: 2699: 2695: 2694: 2693: 2691: 2690: 2689: 2665: 2664: 2663: 2658: 2649: 2635:All-pass filter 2616: 2611: 2563: 2558: 2557: 2541: 2537: 2516: 2512: 2507: 2503: 2498: 2475:Low-pass filter 2446: 2416: 2411: 2410: 2384: 2383: 2355: 2354: 2326: 2325: 2275: 2271: 2270: 2236: 2165: 2161: 2160: 2126: 2097: 2096: 2054: 2034: 2030: 2029: 2013: 2000: 1984: 1962: 1957: 1956: 1940: 1927: 1902: 1901: 1880: 1865: 1856: 1845: 1829: 1828: 1807: 1797: 1790: 1774: 1756: 1755: 1733: 1732: 1728:implementation 1704: 1699: 1698: 1672: 1665: 1664: 1640: 1635: 1634: 1593: 1592: 1566: 1551: 1550: 1517: 1507: 1500: 1484: 1466: 1465: 1443: 1442: 1418: 1413: 1412: 1405: 1387:being used for 1381: 1375: 1366: 1358:image impedance 1342: 1328: 1300: 1294: 1273: 1183:The filter has 1072: 1071: 1009: 997: 986: 974: 952: 951: 921: 888: 887: 851: 850: 805: 783: 755: 731: 710: 705: 704: 670: 669: 650: 649: 616: 611: 610: 604: 518:The filter has 410: 409: 341: 324: 306: 294: 283: 271: 246: 245: 235:low-pass filter 215: 208: 155: 134:all-pass filter 126: 115: 109: 106: 63: 61: 51: 39: 28: 23: 22: 18:All pass filter 15: 12: 11: 5: 2698: 2696: 2688: 2687: 2682: 2677: 2675:Linear filters 2667: 2666: 2660: 2659: 2654: 2651: 2650: 2648: 2647: 2642: 2637: 2632: 2627: 2621: 2618: 2617: 2612: 2610: 2609: 2602: 2595: 2587: 2581: 2580: 2575: 2569: 2562: 2561:External links 2559: 2556: 2555: 2535: 2510: 2500: 2499: 2497: 2494: 2493: 2492: 2487: 2482: 2477: 2472: 2467: 2462: 2457: 2452: 2445: 2442: 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2227: 2224: 2218: 2215: 2212: 2206: 2203: 2197: 2194: 2191: 2185: 2180: 2175: 2170: 2166: 2162: 2157: 2151: 2148: 2145: 2139: 2131: 2127: 2117: 2114: 2108: 2102: 2095: 2094: 2093: 2092: 2070: 2062: 2059: 2055: 2049: 2044: 2039: 2035: 2031: 2026: 2021: 2018: 2014: 2005: 2001: 1991: 1988: 1985: 1978: 1973: 1967: 1963: 1958: 1953: 1948: 1945: 1941: 1932: 1928: 1918: 1915: 1910: 1907: 1903: 1896: 1888: 1885: 1881: 1870: 1866: 1860: 1857: 1850: 1846: 1842: 1837: 1834: 1830: 1823: 1815: 1812: 1808: 1802: 1798: 1794: 1791: 1779: 1775: 1769: 1764: 1761: 1757: 1750: 1744: 1738: 1731: 1730: 1729: 1727: 1709: 1705: 1677: 1673: 1661: 1645: 1641: 1632: 1629: 1625: 1621: 1600: 1571: 1567: 1560: 1556: 1525: 1522: 1518: 1512: 1508: 1504: 1501: 1489: 1485: 1479: 1474: 1471: 1467: 1460: 1454: 1448: 1441: 1440: 1439: 1423: 1419: 1410: 1402: 1400: 1398: 1394: 1390: 1386: 1380: 1372: 1370: 1363: 1361: 1359: 1355: 1351: 1347: 1341: 1332: 1325: 1323: 1321: 1317: 1313: 1309: 1305: 1297: 1295: 1292: 1290: 1286: 1282: 1278: 1270: 1268: 1262: 1258: 1254: 1251: 1247: 1243: 1239: 1236: 1233: 1229: 1225: 1224:short circuit 1221: 1217: 1213: 1212: 1211: 1209: 1205: 1201: 1196: 1194: 1190: 1186: 1166: 1160: 1157: 1154: 1148: 1145: 1142: 1139: 1136: 1133: 1127: 1124: 1118: 1105: 1102: 1091: 1088: 1082: 1070: 1069: 1068: 1066: 1062: 1058: 1057:complex plane 1054: 1050: 1046: 1042: 1022: 1013: 1010: 1006: 1001: 998: 990: 987: 983: 978: 975: 969: 963: 957: 950: 949: 948: 947:is given by: 946: 942: 938: 934: 925: 918: 916: 899: 893: 873: 869: 865: 862: 859: 856: 848: 847:Taylor series 829: 823: 819: 815: 812: 809: 806: 801: 797: 793: 790: 787: 784: 778: 771: 767: 763: 760: 756: 750: 746: 742: 739: 736: 732: 726: 721: 718: 715: 711: 703: 702: 701: 699: 678: 675: 655: 632: 627: 624: 621: 617: 609: 608: 607: 601: 599: 593: 589: 585: 582: 579: 575: 572:, creating a 571: 567: 563: 560: 556: 555:short circuit 552: 548: 544: 543: 542: 540: 536: 531: 529: 525: 521: 501: 495: 492: 489: 483: 480: 477: 474: 471: 465: 462: 456: 443: 440: 429: 426: 420: 408: 407: 406: 404: 400: 396: 395:complex plane 392: 388: 384: 380: 360: 354: 351: 348: 345: 342: 337: 334: 331: 328: 325: 319: 310: 307: 303: 298: 295: 287: 284: 280: 275: 272: 266: 263: 257: 251: 244: 243: 242: 241:is given by: 240: 236: 232: 228: 219: 212: 210: 205: 203: 201: 200:minimum phase 197: 192: 190: 185: 183: 179: 175: 171: 166: 164: 160: 152: 150: 147: 143: 139: 135: 124: 121: 113: 102: 99: 95: 92: 88: 85: 81: 78: 74: 71: –  70: 66: 65:Find sources: 59: 55: 49: 48: 43:This article 41: 37: 32: 31: 19: 2634: 2543: 2538: 2518: 2513: 2504: 2404: 2323: 2088: 1662: 1623: 1618:denotes the 1548: 1406: 1393:linear phase 1382: 1367: 1349: 1345: 1343: 1301: 1293: 1280: 1274: 1266: 1246:open circuit 1197: 1192: 1182: 1055:axis of the 1048: 1038: 930: 915:from above. 844: 647: 605: 597: 570:open circuit 532: 527: 517: 393:axis of the 386: 376: 224: 209: 193: 186: 167: 156: 133: 131: 116: 107: 97: 90: 83: 76: 64: 52:Please help 47:verification 44: 2523:pp. 213-214 2438:unit circle 1726:Z-transform 1631:unit circle 1624:reflections 1409:Z-transform 1397:group delay 1356:(i.e., its 1216:frequencies 1049:reflections 886:we recover 547:frequencies 387:reflections 196:mixed phase 189:comb filter 174:phase shift 142:frequencies 2669:Categories 2552:, p. 10.7. 2550:0070704414 2496:References 1320:topologies 1281:ohmic mode 1193:quadrature 528:quadrature 182:wavelength 178:quadrature 110:March 2009 80:newspapers 2259:− 2231:ℜ 2225:− 2216:− 2195:− 2149:− 2121:ℜ 2115:− 2060:− 2019:− 1995:ℜ 1989:− 1946:− 1922:ℜ 1916:− 1908:− 1886:− 1876:¯ 1861:− 1843:− 1835:− 1824:× 1813:− 1795:− 1785:¯ 1770:− 1762:− 1683:¯ 1604:¯ 1577:¯ 1523:− 1505:− 1495:¯ 1480:− 1472:− 1385:landlines 1312:inductors 1220:capacitor 1155:ω 1149:⁡ 1140:− 1137:π 1128:ω 1116:∠ 1092:ω 1053:imaginary 979:− 788:− 779:≈ 737:− 716:− 679:∈ 622:− 551:capacitor 490:ω 484:⁡ 475:− 466:ω 454:∠ 430:ω 391:imaginary 329:− 276:− 267:− 2444:See also 2407:unstable 1591:, where 1214:At high 545:At high 1628:complex 1279:in its 1255:At the 1202:at the 1059:). The 586:At the 397:). The 94:scholar 2548:  2529:  2324:where 2074:  1534:  1350:filter 1285:phaser 1261:period 1218:, the 1146:arctan 1067:ω are 937:active 648:where 592:period 549:, the 481:arctan 405:ω are 231:active 163:phaser 96:  89:  82:  75:  67:  1348:, or 1306:like 1228:unity 1222:is a 1185:unity 574:unity 553:is a 520:unity 170:phase 146:phase 136:is a 101:JSTOR 87:books 2546:ISBN 2527:ISBN 1697:for 1344:The 1232:gain 1189:gain 1045:zero 1041:pole 931:The 578:gain 524:gain 383:zero 379:pole 225:The 73:news 1438:is 1289:LFO 1277:FET 1111:and 449:and 132:An 56:by 2671:: 2521:, 2402:. 1407:A 1242:DC 1210:. 566:DC 541:. 191:. 2606:e 2599:t 2592:v 2533:. 2422:0 2418:z 2390:k 2370:] 2367:k 2364:[ 2361:x 2341:] 2338:k 2335:[ 2332:y 2308:, 2305:] 2302:k 2299:[ 2296:x 2291:2 2286:| 2281:0 2277:z 2273:| 2268:+ 2265:] 2262:1 2256:k 2253:[ 2250:x 2247:) 2242:0 2238:z 2234:( 2228:2 2222:] 2219:2 2213:k 2210:[ 2207:x 2204:= 2201:] 2198:2 2192:k 2189:[ 2186:y 2181:2 2176:| 2171:0 2167:z 2163:| 2158:+ 2155:] 2152:1 2146:k 2143:[ 2140:y 2137:) 2132:0 2128:z 2124:( 2118:2 2112:] 2109:k 2106:[ 2103:y 2071:, 2063:2 2056:z 2050:2 2045:| 2040:0 2036:z 2032:| 2027:+ 2022:1 2015:z 2011:) 2006:0 2002:z 1998:( 1992:2 1986:1 1979:2 1974:| 1968:0 1964:z 1959:| 1954:+ 1949:1 1942:z 1938:) 1933:0 1929:z 1925:( 1919:2 1911:2 1904:z 1897:= 1889:1 1882:z 1871:0 1867:z 1858:1 1851:0 1847:z 1838:1 1831:z 1816:1 1809:z 1803:0 1799:z 1792:1 1780:0 1776:z 1765:1 1758:z 1751:= 1748:) 1745:z 1742:( 1739:H 1710:0 1706:z 1678:0 1674:z 1646:0 1642:z 1601:z 1572:0 1568:z 1561:/ 1557:1 1526:1 1519:z 1513:0 1509:z 1502:1 1490:0 1486:z 1475:1 1468:z 1461:= 1458:) 1455:z 1452:( 1449:H 1424:0 1420:z 1230:- 1187:- 1167:. 1164:) 1161:C 1158:R 1152:( 1143:2 1134:= 1131:) 1125:i 1122:( 1119:H 1106:1 1103:= 1099:| 1095:) 1089:i 1086:( 1083:H 1079:| 1023:, 1014:C 1011:R 1007:1 1002:+ 999:s 991:C 988:R 984:1 976:s 970:= 967:) 964:s 961:( 958:H 903:) 900:s 897:( 894:H 874:2 870:/ 866:T 863:= 860:C 857:R 830:, 824:2 820:/ 816:T 813:s 810:+ 807:1 802:2 798:/ 794:T 791:s 785:1 772:2 768:/ 764:T 761:s 757:e 751:2 747:/ 743:T 740:s 733:e 727:= 722:T 719:s 712:e 683:C 676:s 656:T 633:, 628:T 625:s 618:e 576:- 522:- 502:. 499:) 496:C 493:R 487:( 478:2 472:= 469:) 463:i 460:( 457:H 444:1 441:= 437:| 433:) 427:i 424:( 421:H 417:| 361:, 355:C 352:R 349:s 346:+ 343:1 338:C 335:R 332:s 326:1 320:= 311:C 308:R 304:1 299:+ 296:s 288:C 285:R 281:1 273:s 264:= 261:) 258:s 255:( 252:H 123:) 117:( 112:) 108:( 98:· 91:· 84:· 77:· 50:. 20:)

Index

All pass filter

verification
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"All-pass filter"
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scholar
JSTOR
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signal processing filter
frequencies
phase
electronic music
phaser
phase
phase shift
quadrature
wavelength
comb filter
mixed phase
minimum phase

operational amplifier
active
low-pass filter
transfer function
pole

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