Valve Type Numbers
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El156 Audio Power
EL156 AUDIO POWER Gerhard Haas Thanks to its robustness, the legendary EL156 audio power pentode has found its way into many professional amplifier units. Its attraction derives not just from its appealing shape, but also from its impressive audio characteristics. We therefore bring you this classical circuit, updated using high- quality modern components. 28 elektor electronics - 3/2005 AMPLIFIER Return of a legend The EL156 was manufactured in the enough to give adequate sensitivity, electrolytic capacitor: this voltage is legendary Telefunken valve factory in even before allowing any margin for further filtered on the amplifier board. Ulm, near the river Danube in Ger- negative feedback. The ECC81 many. The EL156 made amplifiers with (12AT7), however, which has an open- It is not possible to build an ultra-lin- an output power of up to 130 W possi- loop gain of 60 and which can be oper- ear amplifier using the EL156 with a ble, using just two valves in the output ated with anode currents of up to high anode voltage. The same goes for stage and one driver valve. Genuine 10 mA, can be used to build a suitably the EL34. The output transformer is EL156s are no longer available new at low-impedance circuit. therefore connected in such a way that realistic prices, and hardly any are Two EL156s can be used to produce an the impedance of the grid connection available second-hand. The original output power of 130 W with only 6 % to the output valve is much lower than devices used a metal valve base which distortion. -
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. -
Operation, Tetrode, Pentode in the Single-Ended, Class-A
10-76 10. Guitar Amplifiers 10.5.1 Single-ended (class A)-operation, tetrode, pentode In the single-ended, class-A power-stage, one (single) power-tube operates in common- cathode configuration with the output transformer being part of the plate circuit (transformer- coupling). Without AC-drive (“quiescent state”), a stable balance appears – it is called the operating point (OPP). The characteristics shown in Fig. 10.5.2 yield an OPP at 250 V and 48 mA, if a voltage of -7.5 V between (control) grid (g1) and cathode is chosen. This can be done e.g. by using a cathode-resistor of 142 Ω. The cathode-current (the sum of the 48-mA- plate-current and the 5-mA-screen-grid-current) will then generate a positive cathode-voltage of + 7.5 V (relative to ground). With the control-grid at ground-potential (Ug1 = 0) a control- grid-to-cathode-voltage of -7.5 V results (i.e. the control grid is negative vs. the cathode). Fig. 10.5.2: Output characteristics of the EL84, power-stage circuit (single-ended class-A operation). AP = OPP As a drive signal appears (Ug1 ≠ 0), plate-voltage and –current change. As a first approach, it will be sufficient to consider the transformer in the plate-circuit as a large inductance connected in parallel with an ohmic resistor (Chapter 10.6). In this model we have only pure DC flowing through the inductance, and only pure AC flowing through the resistor. With a drive-signal present, the Ua/Ia-point will move along the load-line given in Fig. -
Liste Des Tubes À Vide Il S'agit D'une Liste De Tubes À
Liste des tubes à vide Il s'agit d'une liste de tubes à vide ou vannes thermo-ioniques et basse pression tubes remplis de gaz ou tubes à décharge . Avant l'avènement des semi-conducteurs périphériques, des centaines de types de tubes ont été utilisés dans l'électronique grand public et industriels; aujourd'hui seuls quelques types sont encore utilisés dans des applications spécialisées. Table des matières 1 chauffage ou notes filament 2 embases de tube 3 systèmes de numérotation 3.1 systèmes nord-américain 3.1.1 système RMA (1942) 3.1.2 système RETMA (tubes recevant, 1953) 3.1.3 Chiffre systèmes uniquement 3.2 systèmes d'Europe occidentale 3.2.1 système Marconi-Osram 3.2.2 système Mullard-Philips 3.2.2.1 tubes standard 3.2.2.2 tubes de qualité spéciaux 3.2.2.3 tubes professionnels 3.2.2.4 tubes Transmission 3.2.2.5 Phototubes et des photomultiplicateurs 3.2.2.6 stabilisateurs 3.2.3 systèmes Mazda / Ediswan 3.2.3.1 ancien système 3.2.3.2 tubes de signaux 3.2.3.3 Puissance redresseurs 3.2.4 STC / Brimar système de réception des tubes 3.2.5 Tesla système de tubes de réception 3.3 système de normalisation industrielle japonaise 3.4 systèmes russes 3.4.1 tubes standard 3.4.2 tubes électriques à très haute 3,5 tubes désignation Très-haute puissance (Eitel McCullough et ses dérivés) 3.6 ETL désignation des tubes de calcul 3.7 systèmes de dénomination militaires 3.7.1 Colombie-système nommage CV 3.7.2 US systèmes de dénomination 3.8 Autres systèmes chiffre uniquement 3.9 Autre lettre suivie de chiffres 4 Liste des tubes américains, avec leurs -
Pentodes Connected As Triodes
Pentodes connected as Triodes by Tom Schlangen Pentodes connected as Triodes About the author Tom Schlangen Born 1962 in Cologne / Germany Studied mechanical engineering at RWTH Aachen / Germany Employments as „safety engineering“ specialist and CIO / IT-head in middle-sized companies, now owning and running an IT- consultant business aimed at middle-sized companies Hobby: Electron valve technology in audio Private homepage: www.tubes.mynetcologne.de Private email address: [email protected] Tom Schlangen – ETF 06 2 Pentodes connected as Triodes Reasons for connecting and using pentodes as triodes Why using pentodes as triodes at all? many pentodes, especially small signal radio/TV ones, are still available from huge stock cheap as dirt, because nobody cares about them (especially “TV”-valves), some of them, connected as triodes, can rival even the best real triodes for linearity, some of them, connected as triodes, show interesting characteristics regarding µ, gm and anode resistance, that have no expression among readily available “real” triodes, because it is fun to try and find out. Tom Schlangen – ETF 06 3 Pentodes connected as Triodes How to make a triode out of a tetrode or pentode again? Or, what to do with the “superfluous” grids? All additional grids serve a certain purpose and function – they were added to a basic triode system to improve the system behaviour in certain ways, for example efficiency. We must “disable” the functions of those additional grids in a defined and controlled manner to regain triode characteristics. Just letting them “dangle in vacuum unconnected” will not work – they would charge up uncontrolled in the electron stream, leading to unpredictable behaviour. -
118 Bernards Radio Manuals 5
§ i PRACTICAL 118 voor de Historie v/d Radio iSHB 130. BERNARDS RADIO MANUALS 5/ ■ ■ tUOTHEEK N.V.H.R, i PRACTICAL F.M. CIRCUITS FOR THE HOME CONSTRVCTOR by R. Deschepper BERNARDS (PUBLISHERS) LTD. THE GRAMPIANS WESTERN GATE LONDON, W.6 General Editor Walter J. May First Published in Great Britain, February, 1955. First published in France under the copyright title “ Schemas de recepteurs pour la modulation de “ frequence,” by Societe des Editions Radio, 9, Rue Jacob, Paris (6e) i i ; i i iii THE FREQUENCY MODULATION ERA From its infancy Broadcasting has been considered to fulfill the primary function of conveying to very large audiences the sounds produced in front of the microphone or held in store in the form of recordings. In the early days, the possibility of picking up distant stations appealed strongly to the first amateurs. Long distance records used to be claimed on all sides, and the ‘‘last word” in 1925 was to “receive America.” Although in this way sen sitivity came into the foreground among the principal qualities demanded from a receiver, the density of the traffic through the ether soon brought up the critical problems of selectivity. However, up to 1930, radio remained the privilege of a small group of enthusiasts, since the installation, maintenance and control of a receiver layout (comprising, besides the receiver itself, a frame aerial, a loud speaker, a filament battery together with its charger, and an H.T. battery eventually to be replaced by a “battery eliminator”) necessitated a certain amount of technical knowledge and more than a little patience. -
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. -
History of Thethermionic Tube / Valve / Vacuum
History of theThermionic Tube / Valve / Vacuum Tube – Page 1 The following notes have been assembled by Phil (VK5SRP) from original material and material from several web sites, including Wikipedia for a class run at the North East Radio Club, South Australia January 2016. In electronics, a vacuum tube, an electron tube, or just a tube (North America), or valve (Britain and some other regions) is a device that controls electric current between electrodes in an evacuated container. Vacuum tubes mostly rely on thermionic emission of electrons from a hot filament or a cathode heated by the filament/heater. This type is called a thermionic tube or thermionic valve. A Photo-tube, however, achieves electron emission through the photoelectric effect. Not all electronic circuit valves/electron tubes are vacuum tubes (evacuated). Gas-filled tubes are similar devices containing a gas, typically at low pressure, which exploit phenomena related to electric discharge in gases, usually without a heater. Although thermionic emission was originally reported in 1873 by Frederick Guthrie, it was Thomas Edison's 1883 investigation that spurred future research, the phenomenon thus becoming known as the "Edison effect". Edison patented what he found, but he did not understand the underlying physics, nor did he have an inkling of the potential value of the discovery. It wasn't until the early 20th century that the rectifying property of such a device was utilised, most notably by John Ambrose Fleming, who used the Diode tube to detect (demodulate) radio signals. Lee De Forest's 1906 "Audion" was also developed as a radio detector, and soon led to the development of the Triode tube. -
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. -
A Relatively Simple Device for Recording Radiation Intensities in The
A RELATIVELY SIMPLE DEVICE FOR RECORDING RADIATION INTENSITIES IN HE ULTRAVIOLET PORTION OF THE SPECTRUM by HENRY WALLACE HENDRICKS A THESIS submitted to OREGON STATE COLLEGE in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE June 19S0 APPROVED: Professor of Physics In Charge of Major Chairman of School Graduate Committee Dean of Graduate School ACKN OWLEDGMENT Sincere appreciation and thanks are expressed to Dr. Weniger for his interest and assistance in the preparation of this thesis. TABLE OF CONThNTS a ge I NTROD[JCTION . ..... , . i Statement of . Problem . i Some Basic Information about Ultraviolet, Sun and Sky Radiation, Its Biological Etc. Effectiveness, . 1 INSTRUMLNTS FOR RECORDING ULTRAVIOLET INTENSITIES . 3 DESIGNOONSIDERATIONS. ... .. .. The R e e e i y e . r ....... The . Receiving Circuit . 9 The R e c o e . rd r . 9 . ThePowerSupply . .10 EX>ERIMENTAL . 1)EVELOPMENT . 11 THE FINAL CIRCUIT AND . 7OER SUPPLY . 16 PREPARATION AND SILVERING OF THE QUARTZ PLATES . 20 THERECEIVERUNIT..................23 TESTOFAPPARATtJS . .26 Adjustment8 . 26 Results and Conclusions . 27 . Data . 3]. BILIOGRAPHY . 37 LIST OF ILLUBTRATIONS Figure Page J. Spectral Sensitivfty of the S Photocathode 6 2 OriginalCircuit . 12 3 First Vacuum Tube Circuit . 12 Lj. Variation of the Counts per Minute with Filament Voltage . 11i The Final Circuit . ........ 17 6 The Power Suoply, Counter and Receiver . 22 The 7 Receiver ............... 2)4. 8 Step-diagram from Data ObtaIned on MaylO,l9O ............. 28 9 Step-diagram from Data Obtained on Mayll,l9O ............. 29 10 Step-diagram from Data Obtained on Mayl2,l95O ......... .. 30 A RELATIVELY SIMPLE DEVICE FOR RECORDING RADIATION .LNTENSITIES IN T}IE ULTRAVIOLET PORTION OF THE SPECTRUM INTRODUCTION Statement of Problem The purpose of this thesis is to develop a more or less portable aiaratua that will measure ultraviolet energy in or near the erythemal region.