Radial Beam Power Tetrode 4Cx20,000C
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Tube Number Systems
Frank's Electron tube Pages Tube Number Systems European system after 1934 Philips system before 1934 Mazda numbering system Russian numbering system Brimar type designation code Tesla numbering system European system after 1934 (pro-electron) See also: Type Designation Code from "Preferred Types of Electron Tubes 1967". 1st letter heater indication 0 tubes without filament A 4 V AC parallel connection B 180 mA DC C 200 mA AC/DC series or parallel connection D <= 1.4 V DC dry-battery, parallel connection E 6.3 V AC or carbattery, parallel connection F 13 V carbattery G 5V AC parallel connection H early: 4V DC battery. later: 150mA AC/DC series connection I 20V AC/DC parallel connection K 2 V battery O 150 mA AC/DC series connection P 300 mA AC/DC series connection U 100 mA AC/DC series connection V 50mA AC/DC series connection X 600 mA AC/DC series connection Y 450 mA AC/DC series connection 2nd+next letters tube systems A single detection diode B double detection diode C small-signal triode D power triode E small-signal tetrode (or 2nd emmission tube EE1) F small-signal pentode H hexode or heptode K octode L power pentode or power tetrode M indicator tube N thyratron Q enneode W single gasfilled rectifier diode X double gasfilled rectifier diode Y single vacuum rectifier diode Z double vacuum rectifier diode digits socket & order x P (some are V) (except U-series (e.g.UBL1), those are octal) 1x Y8A 2x W8A, Loctal (except D-series (e.g. -
Electron Optics
Chapter 5.1 Electron Optics Sol Sherr Jerry C. Whitaker, Editor-in-Chief 5.1.1 Introduction The electron gun is basic to the structure and operation of any cathode-ray device, specifically display devices. In its simplest schematic form, an electron gun may be represented by the dia- gram in Figure 5.1.1, which shows a triode gun in cross section. Electrons are emitted by the cathode, which is heated by the filament to a temperature sufficiently high to release the elec- trons. Because this stream of electrons emerges from the cathode as a cloud rather than a beam, it is necessary to accelerate, focus, deflect, and otherwise control the electron emission so that it becomes a beam, and can be made to strike a phosphor at the proper location, and with the desired beam cross section. 5.1.2 Electron Motion The laws of motion for an electron in a uniform electrostatic field are obtained from Newton’s second law. The velocity of an emitted electron is given by 1 2eV 2 v = m (5.1.1) Where: e = 1.6 × 10–19C m = 9.1 × 10–28g V = –Ex, the potential through which the electron has fallen When practical units are substituted for the values in the previous equation, the following results: 5-7 5-8 Electron Optics and Deflection No. 1 grid No. 2 grid Heater Defining aperture Figure 5.1.1 Triode electron gun structure. 1 vV=×5.93 105 2 m/s (5.1.2) This expression represents the velocity of the electron. -
Vacuum Tube Theory, a Basics Tutorial – Page 1
Vacuum Tube Theory, a Basics Tutorial – Page 1 Vacuum Tubes or Thermionic Valves come in many forms including the Diode, Triode, Tetrode, Pentode, Heptode and many more. These tubes have been manufactured by the millions in years gone by and even today the basic technology finds applications in today's electronics scene. It was the vacuum tube that first opened the way to what we know as electronics today, enabling first rectifiers and then active devices to be made and used. Although Vacuum Tube technology may appear to be dated in the highly semiconductor orientated electronics industry, many Vacuum Tubes are still used today in applications ranging from vintage wireless sets to high power radio transmitters. Until recently the most widely used thermionic device was the Cathode Ray Tube that was still manufactured by the million for use in television sets, computer monitors, oscilloscopes and a variety of other electronic equipment. Concept of thermionic emission Thermionic basics The simplest form of vacuum tube is the Diode. It is ideal to use this as the first building block for explanations of the technology. It consists of two electrodes - a Cathode and an Anode held within an evacuated glass bulb, connections being made to them through the glass envelope. If a Cathode is heated, it is found that electrons from the Cathode become increasingly active and as the temperature increases they can actually leave the Cathode and enter the surrounding space. When an electron leaves the Cathode it leaves behind a positive charge, equal but opposite to that of the electron. In fact there are many millions of electrons leaving the Cathode. -
Eimac Care and Feeding of Tubes Part 3
SECTION 3 ELECTRICAL DESIGN CONSIDERATIONS 3.1 CLASS OF OPERATION Most power grid tubes used in AF or RF amplifiers can be operated over a wide range of grid bias voltage (or in the case of grounded grid configuration, cathode bias voltage) as determined by specific performance requirements such as gain, linearity and efficiency. Changes in the bias voltage will vary the conduction angle (that being the portion of the 360° cycle of varying anode voltage during which anode current flows.) A useful system has been developed that identifies several common conditions of bias voltage (and resulting anode current conduction angle). The classifications thus assigned allow one to easily differentiate between the various operating conditions. Class A is generally considered to define a conduction angle of 360°, class B is a conduction angle of 180°, with class C less than 180° conduction angle. Class AB defines operation in the range between 180° and 360° of conduction. This class is further defined by using subscripts 1 and 2. Class AB1 has no grid current flow and class AB2 has some grid current flow during the anode conduction angle. Example Class AB2 operation - denotes an anode current conduction angle of 180° to 360° degrees and that grid current is flowing. The class of operation has nothing to do with whether a tube is grid- driven or cathode-driven. The magnitude of the grid bias voltage establishes the class of operation; the amount of drive voltage applied to the tube determines the actual conduction angle. The anode current conduction angle will determine to a great extent the overall anode efficiency. -
For Reference
u \) Presented at 6th Symposium on LBL-4418 Engineering Problems of Fusion Research, c:.' San Diego, CA, November 18-21, 1975 ) -. THE POWER SUPPLY FOR THE LBL 40 keV NEUTRAL BEAM SOURCE >l W. R. Baker, M. L. Fitzgerald, andV. J. Honey November 1975 Prepared for the U. S. Energy Research and Development Administration under Contract W-7405-ENG-48 For Reference Not to be taken from this room DISCLAIMER This document was prepared as an account of work sponsored by the United States Government. While this document is believed to contain correct information, neither the United States Government nor any agency thereof, nor the Regents of the University of California, nor any of their employees, makes any warranty, express or implied, or assumes any legal responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by its trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof, or the Regents of the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof or the Regents of the University of California. 0 0 0 0 9 3 LBL-4418 /{, THE POWER SUPPLY FOR THE LBL 40 keV NEUTRAL BEAM SOURCE * W. R. Baker, M. L. Fitzgerald, V. J. Honey Lawrence Berkeley Laboratory Berkeley, California 94720 Summary To accomplish this the system must have fast voltage rise and current interrupt which means that the capa A 20 keV, 50 Amp, 10 millisec pulse oo Neutral citance to ground of the Source and its associated Beam Sourcel at the Lawrence Berkeley Laboratory that power supplies and equipment must be held to a mini serves as the prototype for 12 similar sources now in mum. -
HANDBOOK Mixer and Converter Tubes 79 Stituted for the Plate of a Triode
HANDBOOK Mixer and Converter Tubes 79 stituted for the plate of a triode. p5g denotes The Effect of The current equations show how the ratio of a change in grid voltage to a Grid Current the total cathode current in change in screen voltage, each of which will triodes, tetrodes, and pentodes produce the same change in screen current. is a function of the potentials applied to the Expressed as an equation: various electrodes. If only one electrode is positive with respect to the cathode (such as AE,, would be the case in a triode acting as a Ps: 1 sg = constant, A = small class A amplifier) all the cathode current goes AE, increment to the plate. But when both screen and plate are positive in a tetrode or pentode, the cath- The grid- screen mu factor is important in ode current divides between the two elements. determining the operating bias of a tetrode Hence the screen current is taken from the or pentode tube. The relationship between con- total cathode current, while the balance goes trol -grid potential and screen potential deter- to the plate. Further, if the control grid in a mines the plate current of the tube as well as tetrode or pentode is operated at a positive the screen current since the plate current is potential the total cathode current is divided essentially independent of the plate voltage between all three elements which have a posi- in tubes of this type. In other words, when tive potential. In a tube which is receiving a the tube is operated at cutoff bias as deter- large excitation voltage, it may be said that mined by the screen voltage and the grid - the control grid robs electrons from the output screen mu factor (determined in the same way electrode during the period that the grid is as with a triode, by dividing the operating positive, making it always necessary to limit voltage by the mu factor) the plate current the peak -positive excursion of the control will be substantially at cutoff, as will be the grid. -
Valve Types and Char
‘Technical Shorts’ by Gerry O’Hara, VE7GUH/G8GUH ‘Technical Shorts’ is a series of (fairly) short articles prepared for the Eddystone User Group (EUG) website, each focussing on a technical issue of relevance in repairing, restoring or using Eddystone valve radios. However, much of the content is also applicable to non-Eddystone valve receivers. The articles are the author’s personal opinion, based on his experience and are meant to be of interest or help to the novice or hobbyist – they are not meant to be a definitive or exhaustive treatise on the topic under discussion…. References are provided for those wishing to explore the subjects discussed in more depth. The author encourages feedback and discussion on any topic covered through the EUG forum. Valve Types and Characteristics Introduction The Technical Short on ‘Valve Lore’ deals with using valves in receivers in general terms – their evolution through the years, types and general application in Eddystone receivers, as well as tips on sourcing valves and testing them. The Technical Shorts on ‘Eddystone Circuit Elements’ and ‘Receiver Front-Ends’ take a closer look at how valves are selected and used in particular circuits within Eddystone valve receivers. In preparing these articles, it occurred to me that an insight into some of the basics underlying the selection of a particular valve for an application in a receiver would be useful. In order to do this, some consideration of valve ‘fundamentals’ is necessary and how these influence their application and use in receivers. So here I deal mainly with the basics of valve construction and design and then their electrical parameters and important operating characteristics. -
Valve Type Numbers
Valve Type Numbers The information in this document has been gathered and assembled from various sources including Radio Bygones magazine No. 9 (February/March 1991). Pro-Electron/Mullard Code This are probably the most commonly encountered numbering system in the UK - and the most informative. It consists of two or more letters followed by a number (normally two digits). Examples - UL41, ECC85, UABC80. The first letter gives heater rating: Character Heater Rating A 4V B 180mA C 200mA D 0 - 1.5V (previously 1.4V) E 6.3V F 12.6V G Misc. (previously 5V) H 150mA K 2V L 450mA P 300mA T 7.4V U 100mA V 50mA W 600mA X 450mA The remaining letters give the types of device in the valve. They are normally listed in alphabetical order. Character Device Type A Signal Diode B Double Diode C Signal Triode D Power Triode E Signal Tetrode F Signal Pentode H Hexode or Heptode (Hexode type) K Octode or Heptode (Octode type) L Output Tetrode or Pentode M Magic Eye (Tuning Indicator) N Gas-filled Triode (Thyrathon) Q Nonode X Gas-filled Full-wave Rectifier Y Half-wave Rectifier Z Full-Wave Rectifier The first digit indicates the base type. Where there is only one digit this is assumed to be the second digit, and be preceded by a zero. For example, EM4 should be interpreted as EM04. Digit Base Type 0 and 1 Miscellaneous Bases (P-Base, Side Contact etc) 2 B10B (previously B8B/B8G (Loctal)) 3 International Octal (8-pin with centre locating spigot) 4 B8A (8 pin with locating pip on side) 5 B9G and B9D (wire ended) 6 and 7 Subminatures 8 B9A (9-pin glass) 9 B7G (7-pin glass) The remaining digit(s) are used to differentiate between valves that would otherwise have identical numbers:- • One digit for early valves • Two figures for later entertainment valves • Three or Four figures for later professional types GEC Code (also used on Marconi and Osram valves) This consists of one or two letters followed by a number (normally two digits). -
Unusual Tubes
Unusual Tubes Tom Duncan, KG4CUY March 8, 2019 Tubes On Hand GAS-FILLED HIGH-VACUUM • Neon Lamp (NE-51) • Photomultiplier • Cold-cathode Voltage (931A) Regulator (0B2) • Magic Eye (1629) • Hot-cathode Thyratron • Low-voltage (12DY8) (884) • Space Charge (12K5) 2 Timeline of Related Events 1876, 1902 William Crookes Cathode Rays, Glow Discharge 1887 [1921] Hertz, Einstein Photoelectric Effect 1897 [1906] J. J. Thomson Electron identified 1920 Daniel Moore (GE) Voltage Regulator 1923 Joseph Slepian Secondary Emission (Westinghouse) 1928 Albert Hull, Irving Thyratron Langmuir (GE) [1928] Owen Richardson Thermionic Emission 1936 Vladimir Zworykin Photomultiplier (RCA) 1937 Allen DuMont Magic Eye 3 Neon Bulbs • Based on glow-discharge (coronal discharge) effect noticed by William Crookes around 1902. • Exhibit a negative incremental resistance over part of the operating range. • Light-sensitive: photo-ionization causes the ionization voltage to decrease with illumination (not generally a desirable characteristic). • Used as indicators , voltage regulators, relaxation oscillators , and the larger ones for illumination . 4 Neon Lamp/VR Tube Curves 80 Normal Abnormal Glow Glow 70 60 Townsend Discharge 50 Negative Resistance 40 Region 30 Volts across Device across Volts 20 10 Conduction Destroys Lamp Destroys Arc Conduction Arc Chart details (coronal) Glow depend on -5 element 10 -20 10 -15 10 -10 10 1 geometry and Current through Device (A) gas mixture. 5 Cold-Cathode Voltage Regulator Tubes • Very similar to neon bulbs: attention paid to increasing current-carrying capability and ensuring a constant forward voltage. • Gas sometimes includes radio-isotopes to reduce sensitivity to photo-ionization. • Developed at General Electric Research Labs by Daniel Moore around 1920. -
Accuracy of Tetrode Spike Separation As Determined by Simultaneous Intracellular and Extracellular Measurements
Accuracy of Tetrode Spike Separation as Determined by Simultaneous Intracellular and Extracellular Measurements KENNETH D. HARRIS, DARRELL A. HENZE, JOZSEF CSICSVARI, HAJIME HIRASE, AND GYORGY¨ BUZSAKI´ Center for Molecular and Behavioral Neuroscience, Rutgers, The State University of New Jersey, Newark, New Jersey 07102 Received 10 December 1999; accepted in final form 6 April 2000 Harris, Kenneth D., Darrell A. Henze, Jozsef Csicsvari, Hajime of recording electrodes in a small amount of tissue without Hirase, and Gyo¨rgy Buzsa´ki. Accuracy of tetrode spike separation significant tissue damage and efficient isolation of action po- as determined by simultaneous intracellular and extracellular mea- tentials emanating from individual neurons. Action potentials surements. J Neurophysiol 84: 401–414, 2000. Simultaneous record- generated by neurons (“unit” or “spike” activity) can be mon- ing from large numbers of neurons is a prerequisite for understanding itored by extracellular glass pipettes, single etched (sharp) their cooperative behavior. Various recording techniques and spike separation methods are being used toward this goal. However, the electrodes, or multiple-site probes. The closer the electrode to error rates involved in spike separation have not yet been quantified. the soma of a neuron, the larger the size of the extracellularly We studied the separation reliability of “tetrode” (4-wire electrode)- recorded spikes. Whereas glass pipettes and high-impedance recorded spikes by monitoring simultaneously from the same cell sharp metal -
Tetrode and Pentode RF Power Amplifier Information
Tetrode and Pentode RF Power Amplifier Information By Larry E. Gugle K4RFE, RF Design, Manufacture, Test & Service Engineer (Retired) Tune-Up Procedure When adjusting a RF Power Amplifier using either a Power Tetrode or Power Pentode, for proper excitation and loading, it will be noticed that the procedure is different, depending upon whether the Screen Grid Voltage is taken from a, Fixed Screen Grid Power Supply with good regulation, or from a Dropping Resistor from the Plate Power Supply with poor regulation. If the Screen Grid Voltage is taken from a Fixed Screen Grid Power Supply with good regulation; 1. The Current is almost entirely controlled by the RF excitation. One should first vary excitation until the desired Current flows. 2. The loading is then varied until the maximum power output is obtained. 3. Following these adjustments the excitation is then trimmed along with the loading until the desired Control Grid Current, and Screen Grid Current is obtained. If the Screen Grid Voltage is taken from a Dropping Resistor from the Plate Power Supply with poor regulation; 1. The stage will tune very much like a Power Triode RF Power Amplifier. 2. The Current will be adjusted principally by varying the Loading, and the excitation will be trimmed to give the desired Control Grid Current. 3. In this case the Screen Grid Current will be almost entirely set by the choice of the dropping resistor. It will be found that excitation and loading will vary the Screen Grid Voltage considerably and these should be trimmed to give about normal Screen Grid Voltage. -
Valves Revisited
Valves Revisited by Bengt Grahn, SM0YZI (Low Resolution Sample) RSGB © Radio Society of Great Britain Published by the Radio Society of Great Britain, 3 Abbey Court, Fraser Road, Priory Business Park, Bedford, MK44 3WH. First published 2011 © Radio Society of Great Britain 2011. All rights reserved. No part of this publica- tion may be reproduced, stored in a retrieval system, or transmitted in any form, or by any means, electronic, mechanical, photocopying, recording or otherwise, without the prior written agreement of the Radio Society of Great Britain. ISBN 9781 9050 8670 9 Publisher’s note The opinions expressed in this book are those of the author and not necessarily those of the RSGB. While the information presented is believed to be correct, the author, publisher and their agents cannot accept responsibility for consequences arising from any inaccuracies or omissions. Cover design: Kim Meyern Typography, editing and design: Mike Dennison, G3XDV of Emdee Publishing Production: Mark Allgar,RSGB M1MPA ©Printed in Great Britain by Nuffield Press Ltd of Abingdon Contents 1 Evolution of the Valve . 1 2 How does a Valve Work? . 7 3 Characteristics of Valves . 25 4 Connecting Stages Together . 41 5 Tuned Circuits . 53 6 Amplifiers . 69 7 Modulation . 95 8 Receivers . 103 9 The Superhet in Detail . 113 10 Designing a Receiver . .141 11 Hi-fi Amplifiers . .147 12 Construction with Valves . .175 13 The Power Supply . .RSGB . .181 14 Oscillators . .193 15 A Signal Generator . .205 16 Measurements . .223 17 Fault Finding© . .239 18 Transmitters . .249 19 Further Information on the Web . .257 Appendix: European Valve Designations .