Knowledge (XXG)

Plate detector (radio)

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passed through a plate load impedance chosen to produce the desired amplification in conjunction with the tube characteristics. A capacitor of low impedance at the carrier frequency and high impedance at audio frequencies is provided between the tube plate and cathode, to minimize amplification of the carrier frequency and remove carrier frequency variations from the recovered modulation waveform. The allowable peak 100% modulated input signal voltage is limited to the magnitude of the bias voltage, corresponding to an unmodulated carrier peak voltage of half the bias voltage magnitude.
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suited to the higher radio frequency signal level than the plate detector. Diode detectors also became popular during the later 1920s because, unlike plate detector circuits, they could also provide automatic gain control voltage (A.V.C.) for the radio frequency amplifier stages of the receiver. However, the
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In the Infinite-Impedance detector, the load resistance is placed in series with the cathode, rather than the plate, and the demodulated output is taken from the cathode. The circuit is operated in the region where grid current does not occur during any portion of the carrier frequency cycle, thus
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Plate detector circuits were most commonly used from the 1920s until the start of World War II. In 1927, the advent of screen grid tubes permitted much more radio frequency amplification before the detector stage than previously practically possible. The previously used grid leak detector was less
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As with the standard plate detector, the device is biased almost completely off. The positive-going 180 degrees of the carrier input signal causes a substantial increase of cathode or source current above the amount set by the bias, and the negative-going 180 degrees of the carrier cycle causes a
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transformer. An incoming signal will cause the plate current to increase much more during the positive 180 degrees of the carrier frequency cycle than it decreases during the negative 180 degrees. The plate current variation will include the original modulation frequencies. The plate current is
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Plate detector circuits usually do not produce A.V.C. voltage for the radio frequency (R.F.) stages of the receiver. In these receivers, volume control is often accomplished by providing variable cathode bias of one or more stages prior to the detector. A potentiometer is used to implement the
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A potentiometer (typically 500 kΩ audio taper) where the high end and center wiper are connected as above, but where the low end is connected to the control grid of audio output tube. (In this circuit, the potentiometer replaces the bias resistor for the output tube's control
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or cathode bias may be used for the plate detector. When cathode bias is implemented, a capacitor of low impedance at the carrier frequency and high impedance at audio frequencies bypasses the cathode resistor. Cathode bias reduces the amplification obtainable.
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To set a limit on the ability of the volume control to reduce the bias on the stages that it controls, the potentiometer is often equipped with a mechanical rotation limit facility that prevents the resistance from being reduced below a specific amount.
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to follow the modulation envelope. Negative feedback takes place at the recovered modulation frequencies, reducing distortion. The infinite impedance detector can demodulate higher modulation percentages with less distortion than the plate detector.
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The other end of the potentiometer is connected to the cathode of at least one R.F. amplifier (in T.R.F. receivers) or the cathode of the converter and/or the I.F. amplifier (in superheterodyne receivers).
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Because the volume control in non-A.V.C. receivers adjusts R.F. signal levels rather than A.F. signal levels, the volume control must be manipulated while tuning the radio in order to find weak signals.
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circuit in which an amplifying tube having a control grid is operated in a non-linear region of its grid voltage versus plate current transfer characteristic, usually near plate current cutoff, to
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costs that were as much as twice the cost of the tubes commonly used as plate detectors. This made plate detector circuits more practical for low-priced radios sold during the depths of the
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A linear taper potentiometer connected to the antenna (high end), ground (low end) and the antenna transformer primary or first tuned circuit (center wiper).
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Negative bias is applied to the grid to bring the plate current almost to cutoff. The grid is connected directly to the secondary of a radio frequency or
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the name "Infinite Impedance Detector". An example schematic diagram of an implementation using a field effect transistor is shown.
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A linear taper potentiometer that adjusts the screen grid voltages of the R.F. amplifiers (if they are tetrodes or pentodes);
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variable cathode bias. The most common connection of the potentiometer (typically 4 kΩ to 15 kΩ linear taper) is as follows:
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Plate detector circuit with cathode bias. Cathode bias RC time constant three times period of lowest carrier frequency. C
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time constant is much shorter than the period of the highest modulating frequency, permitting the voltage across C
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values of 100 to 500 picofarads being typical. The low pass filter in the V+ power supply line, C4 and the RFC (
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coupling through the power supply to other circuitry and does not contribute to the function of the detector.
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01A, 1H4G, 6C6, 6J7, 6SJ7, 12F5, 12J5, 12J7, 12SF5, 12SJ7, 24, 24A, 27, 30, 36, 37, 56, 57, 76, 77, 201A, 301A
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The wiper is connected to ground (in A.C. receivers) or B minus (in A.C./D.C. receivers);
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H. A. Robinson, "The Operating Characteristics of Vacuum Tube Detectors", Part 1.
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and dual-diode/pentode tubes commonly used for detection/A.V.C. circuits had bulk
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is chosen to be several times the period of the lowest carrier frequency, with C
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values of 50,000 to 150,000 ohms are typical for tubes. The time constant of C
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One end of the potentiometer is connected to the antenna coupling component;
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Two typical superheterodyne radios with a triode plate detector. Sold by
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very little decrease of cathode current below the level set by the bias. C
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Circuit description of a typical JFET-based infinite impedance detector.
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is charged to a dc voltage determined by the carrier amplitude. C
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A typical T.R.F. radio with a pentode plate detector. Sold by
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Other volume control circuits in non-A.V.C. receivers include:
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JFET-based infinite impedance detector for AM-demodulation
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amplitude modulated carrier signal. This differs from the
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Infinite-Impedance Detector (Modern JFET Implementation)
546:(from crystal sets to mass-produced transistor radios) 624:, Chandler, AZ: Sonoran Publishing LLC, 2007, p. 336 638:, London: The Amalgamated Press LTD., 1933, p. 115 597:, 2nd ed. New York: McGraw-Hill, 1937, pp. 433-446 725:Schematic of "Silvertone" models 6114 and 6115. 687:B. Goodman, "The Infinite Impedance Detector", 662:, no. 905, vol. XL, no. 1, Jan. 1st 1937, p. 6 152:Comparison with Alternative Envelope Detectors 715:Schematics of Packard Bell models 35A and 65. 582:, New York: John Wiley and Sons, 1943, p. 105 8: 622:Radiola: the Golden Age of RCA, 1919 - 1929 222:) shown in the diagram, minimizes unwanted 233: 561: 34:anode bend detector, grid bias detector 658:W. N. Weeden, "New Detector Circuit", 139:Tubes commonly used as plate detectors 677:, New York: McGraw-Hill, 1947, p. 710 573: 571: 569: 567: 565: 407:(unless bias is applied to overcome V 7: 611:, vol. XIV, no. 8, p. 27, Aug. 1930 14: 693:, vol. XXIII, p. 21, Oct. 1939 1: 675:Electronic Circuits and Tubes 580:The Technique of Radio Design 419:(depends on op-amp employed) 182:can only be discharged via R 243:Infinite-impedance detector 157:Infinite-Impedance Detector 24:is typically around 250 pF. 777: 636:The Manual of Modern Radio 673:Cruft Electronics Staff, 595:Communication Engineering 527: 505: 487:(with appropriate diodes) 452:Maximum usable frequency 451: 425: 359:Loading of tuned circuit 332: 316:(offset voltage too high) 298:(offset voltage too high) 286: 256: 236: 531:Old short-wave receivers 528:Most commonly found in: 94:Controlling volume level 534:High fidelity AM tuners 539:regenerative receivers 230:Summary of Differences 166: 79:intermediate frequency 25: 164: 19: 648:W.L. Everitt, p. 434 252:Precision Rectifier 721:in the early 1930s. 506:Circuit Complexity 333:Typical Distortion 634:J. Scott-Taggart, 543:Most AM receivers 386:Quiescent current 246:Grid-leak detector 167: 46:grid leak detector 28:In electronics, a 26: 554: 553: 547: 501: 488: 465: 421: 412: 318: 309: 300: 59:dual-diode/triode 768: 756:Radio technology 703: 702:B. Goodman, 1939 700: 694: 685: 679: 670: 664: 655: 649: 646: 640: 631: 625: 618: 612: 605: 599: 590: 584: 575: 545: 493: 485: 456: 417: 406: 314: 307:(positive-going) 305: 296: 234: 67:Great Depression 776: 775: 771: 770: 769: 767: 766: 765: 751:Analog circuits 741: 740: 711: 706: 701: 697: 686: 682: 671: 667: 656: 652: 647: 643: 632: 628: 619: 615: 606: 602: 593:W. L. Everitt, 591: 587: 576: 563: 559: 550:Test equipment 544: 492: 486: 468:can be used at 457: 444: 416: 410: 405: 313: 304: 295: 259:Directly-Heated 232: 217: 213: 209: 205: 197: 193: 189: 185: 181: 177: 159: 154: 141: 96: 75: 54: 23: 12: 11: 5: 774: 772: 764: 763: 758: 753: 743: 742: 739: 738: 732: 722: 710: 709:External links 707: 705: 704: 695: 680: 665: 660:Wireless World 650: 641: 626: 620:E. P. Wenaas, 613: 600: 585: 560: 558: 555: 552: 551: 548: 541: 535: 532: 529: 525: 524: 521: 516: 513: 510: 507: 503: 502: 489: 477: 474: 466: 453: 449: 448: 441: 438: 433: 430: 427: 423: 422: 413: 408: 400: 397: 392: 387: 383: 382: 376: 373: 370: 365: 360: 356: 355: 350: 347: 344: 339: 334: 330: 329: 324: 319: 310: 301: 292: 284: 283: 280: 275: 270: 267: 262: 254: 253: 250: 249:Diode detector 247: 244: 241: 240:Plate detector 238: 231: 228: 215: 211: 207: 203: 195: 191: 187: 183: 179: 175: 158: 155: 153: 150: 149: 148: 140: 137: 132: 131: 130: 129: 126: 123: 111: 110: 107: 104: 95: 92: 74: 71: 53: 50: 30:plate detector 21: 13: 10: 9: 6: 4: 3: 2: 773: 762: 759: 757: 754: 752: 749: 748: 746: 736: 733: 730: 729:Sears Roebuck 726: 723: 720: 716: 713: 712: 708: 699: 696: 692: 691: 684: 681: 678: 676: 669: 666: 663: 661: 654: 651: 645: 642: 639: 637: 630: 627: 623: 617: 614: 610: 604: 601: 598: 596: 589: 586: 583: 581: 578:E.E. Zepler, 574: 572: 570: 568: 566: 562: 556: 549: 542: 540: 536: 533: 530: 526: 522: 520: 517: 514: 511: 508: 504: 500: 498: 490: 484: 482: 478: 475: 473: 472: 467: 464: 462: 461:Miller effect 454: 450: 447: 442: 439: 437: 434: 431: 428: 426:Voltage Gain 424: 420: 414: 404: 401: 398: 396: 393: 391: 388: 385: 384: 381: 377: 374: 371: 369: 366: 364: 361: 358: 357: 354: 351: 348: 345: 343: 340: 338: 335: 331: 328: 325: 323: 320: 317: 311: 308: 302: 299: 293: 290: 287:Suitable for 285: 281: 279: 276: 274: 271: 268: 266: 263: 260: 257:Suitable for 255: 251: 248: 245: 242: 239: 235: 229: 227: 225: 221: 200: 171: 163: 156: 151: 147: 143: 142: 138: 136: 127: 124: 120: 119: 117: 116: 115: 108: 105: 102: 101: 100: 93: 91: 88: 85:Either fixed 83: 80: 72: 70: 68: 64: 60: 51: 49: 47: 43: 39: 35: 31: 18: 761:Vacuum tubes 719:Packard Bell 698: 688: 683: 674: 668: 659: 653: 644: 635: 629: 621: 616: 608: 603: 594: 588: 579: 537:Single-tube 518: 494: 479: 469: 463:limitations) 458: 445: 435: 418: 402: 394: 389: 379: 367: 362: 352: 341: 336: 326: 321: 315: 306: 297: 277: 272: 264: 201: 172: 168: 145: 133: 112: 97: 84: 76: 55: 33: 29: 27: 403:Low or None 291:production 38:vacuum tube 745:Categories 557:References 483:and beyond 42:demodulate 497:slew rate 446:(usually) 380:(Usually) 282:Unlikely 237:Detector: 73:Operation 63:wholesale 731:in 1939. 523:Highest 499:limited) 395:Very low 390:Very low 342:Very low 220:RF Choke 378:Medium 52:History 36:) is a 519:Lowest 443:Unity 429:Medium 372:Medium 349:Medium 346:Medium 261:tubes 210:with R 122:grid); 455:High 432:Unity 415:High 411:drop) 491:Low 476:High 436:High 399:High 375:High 87:bias 690:QST 609:QST 515:Low 512:Low 509:Low 481:UHF 471:VHF 440:Low 368:Low 363:Low 353:Low 337:Low 327:Yes 322:Yes 312:No 303:No 294:No 289:AGC 278:Yes 273:Yes 265:Yes 747:: 564:^ 269:No 224:RF 69:. 495:( 459:( 409:f 216:2 212:1 208:2 204:1 202:R 196:2 192:1 190:R 188:2 184:1 180:2 176:2 144:' 32:( 22:L

Index


vacuum tube
demodulate
grid leak detector
dual-diode/triode
wholesale
Great Depression
intermediate frequency
bias

RF Choke
RF
Directly-Heated
AGC
Miller effect
VHF
UHF
slew rate
regenerative receivers





E.E. Zepler, The Technique of Radio Design, New York: John Wiley and Sons, 1943, p. 105
W. L. Everitt, Communication Engineering, 2nd ed. New York: McGraw-Hill, 1937, pp. 433-446
J. Scott-Taggart, The Manual of Modern Radio, London: The Amalgamated Press LTD., 1933, p. 115
W. N. Weeden, "New Detector Circuit", Wireless World, no. 905, vol. XL, no. 1, Jan. 1st 1937, p. 6
Cruft Electronics Staff, Electronic Circuits and Tubes, New York: McGraw-Hill, 1947, p. 710
QST

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