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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. -
Lawrence Berkeley National Laboratory Recent Work
Lawrence Berkeley National Laboratory Recent Work Title TESTING TECHNIQUES USED IN THE QUALITY SELECTION OF RCA 6810 MULTIPLIER PHOTOTUBES Permalink https://escholarship.org/uc/item/5jv0v3kb Author Kirsten, Frederick A. Publication Date 1956-10-16 eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA ' TWO-WEEK LOAN COPY This is a Library Circulating Copy which may be borrowed for two weeks. For a personal retention copy, call Tech. Info. Diuision, Ext. 5545 BERKELEY, CALIFORNIA 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. · UCRL- 3430(rev.) Engineering Distribution UNIVERSITY OF CALIFORNIA Radiation Laboratory Berkeley,. California Contract No. W -7405-eng-48 • •·l TESTING TECHNIQUES USED IN THE QUALITY SELECTION OF RCA 6810 MULTIPLIER PHOTOTUBES . -
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. -
Iii. Modern Electronic Techniques Applied to Physics and Engineering
_~__~~n~~____ I_~__ III. MODERN ELECTRONIC TECHNIQUES APPLIED TO PHYSICS AND ENGINEERING A. DESIGN AND CONSTRUCTION OF A MICROWAVE ACCELERATOR Staff: Professor J. C. Slater Professor A. F. Kip Dr. W. H. Bostick R. J. Debs P. T. Demos M. Labitt L. Maier S. J. Mason I. Polk J. R. Terrall Since the last progress report, primary emphasis has been on con- struction of additional lengths of accelerating cavity and the associated equipment necessary for operation. Primary design work has been finished on all components necessary for operation of the accelerator and most com- ponents are in the process of being assembled. The following items include recent developments and design details which have not been mentioned earlier. Delivery on the 2-Mev Van de Graaff machine is expected at an early date. A pulsing circuit to modulate the electron beam from the Van de Graaff machine has been designed and built. Since this circuit is to be placed in the dome of the machine at high pres- sure, all component parts have been subjected to 400 lb/in2 pressure to ensure that they have the necessary strength. Machining work on the one-foot accelerator sections is essentially completed. Assembly and brazing of the parts are now in progress. The final design for the 20-foot accelerator tube has been slightly modified in that it has been divided into three sections which are isolated from each other rf-wise by short drift tubes which act as waveguides beyond cut-off. The primary purpose of this procedure is to allow for tuning each section to optimum frequency independently. -
Nojivw&Ohn? *Joto Omaj
Dec. 18, 1962 W. R. SLOAN 3,069,681 SYSTEM FOR LARGE-AREA DISPLAY OF TWO-COLOR INFORMATION Filed March la, l960 3 Sheets-Sheet 1. r LIMAS9.NIHO BOHABO ??31=== IWWBO-BNI-NOI.-OL SV78EWIlCJE OMAJ.*JOTOO NOJIVW&JOHN? MABIA9.NI BOV-38ñS [] [] INVENTOR. WILLIAM R. SLOAN BY ????????? ? ???? AT TORNEYS Dec. 18, 1962 W. R, SLOAN 3,069,681 SYSTEM FOR LARGE-AREA DISPLAY OF TWO-COLOR INFORMATION Filed March 14, 1960 3. Sheets-Sheet 2 GN2&#OTOO ea? ?——?? AT TORNEYS Dec. 18, 1962 W. R. SOAN 3,069,681 SYSTEM FOR LARGE-AREA DISPLAY OF TWO-COLOR INFORMATION Filed March 14, 1960 3 Sheets-Sheet 3 – E. T =-4 HORIZONAL ? SWEEP GENERATOR 44 68 256 K.C. GENERATORPULSE ( BSTABLE BSTABLE B|STABLE ? B|STABLE BSTABLE ??? ? ??82 m232 -- 198 lost 3 -- SAS JS JAAYeASeSYe SAuSJSJASJLLLTLTMSTTLTTTLLLSLLSS LL LLL LLLLLL DISPLAY SURFACE HORIZONTAL SWEEP GENERATOR INVENTOR. WLLAM R. SOAN ATTORNEYS 3,069,681 United States Patent Office Patented Dec. 18, 1962 2 3,069,681 when the electrodes are respectively pulsed. Each of the SYSTEM FOR LARGE-AREA DISPLAY OF pluralities of electrodes is in spaced-apart alignment along TWO,-COLOR ENSFORMATION one dimension of the sheet and the two pluralities of William R. Sloan, Fort Wayne, Ind., assignor to Inter electrodes are respectively spaced-apart along the other national Telephone and Telegraph Corporation dimension of the sheet. Means are provided for moving Filed Mar. 14, 1960, Ser. No. 14,743 the sheet with respect to the electrodes along the other 9 Claims. (Cl, 346-74) dimension. First switching means is provided sequen tially coupling the first electrodes to the converting means This invention relates to a system for presenting in for sampling one of the color-responsive signals at dis two colors alpha-numeric information, i.e., words and Crete intervals and for pulsing the first electrodes respon numbers, and graphical information, such as maps, sive to the presence of the one color signal at the respec graphs, etc., visually on a large-area display for group tive intervals. -
X-Ray Spectra from a Brass-Target Plasma Triode Abstract in This
X-ray Spectra from a Brass-target Plasma Triode Eiichi SATO, Haruo OBARA, Toshiyuki ENOMOTO, Etsuro TANAKA Hidezo MORI, Toshiaki KAWAI, Toshio ICHIMARU, Akira OGAWA Shigehiro SATO, Kazuyoshi TAKAYAMA Jun ONAGAWA I) Department of Physics , Iwate Medical University 2) Department of Radiological Technology , College of Medical Science, Tohoku University 3) The 3rd Department of Surge ry, Toho University School of Medicine 4) Department of Nutrition al Science, Faculty of Applied Bioscience, Tokyo University of Agriculture 5) Department of Cardiac Physiology , National Cardiovascular Center Research Institute 6) Electron Tube Division #2, Hamamatsu Photonics K. K. 7) Department of Radiologi cal Technology, School of Health Sciences, Hirosaki University 8) Department of Neurosurgery , School of Medicine, Iwate Medical University 9) Department of Microbiolog y, School of Medicine, Iwate Medical University 10) Tohoku University Biomedical Engineering Research Organization II) Department of Electronics , Faculty of Engineering, Tohoku Gakuin University Research Code No.: 200, 204.1 Keywords:Flash x-ray,Brass target, Weaklyionized linear plasma, Characteristicx-rays, Absorptionof zinc Kj3rays Abstract In this paper, we describe a recentlydeveloped table-top plasma x-ray generator utilizing a brass-targettriode, which we used in preliminary experiments for the superpositionof K-series characteristicx-rays in weakly ionized plasma and for producing their higher harmonics. In the plasma flash x-raygenerator, a 200 nF condenser was charged,and flash x-rays were producedby discharging.The x-ray tube was a demountabletriode with a brass target containing65% copper and 35% zinc by weight, and a turbomolecularpump evacuatedair from the tube with a pressure of 1 mPa. Targetevaporation led to the formationof weakly ionized linear plasma, consistingof metal ions and electrons,around the rod target, and intense characteristicx-rays were produced. -
Commissioning of the Mice Rf System* A
5th International Particle Accelerator Conference IPAC2014, Dresden, Germany JACoW Publishing ISBN: 978-3-95450-132-8 doi:10.18429/JACoW-IPAC2014-WEPME020 COMMISSIONING OF THE MICE RF SYSTEM* A. Moss, A. Wheelhouse, T. Stanley, C. White, STFC, Daresbury Laboratory, Warrington, UK K. Ronald, C.G. Whyte, A.J. Dick, D.C. Speirs, SUPA, Dept.of Physics, University of Strathclyde, Glasgow, UK S. Alsari, Imperial College of Science and Technology, London, UK on behalf of the MICE Collaboration Abstract feature adjustable sections to change the response of the cavity to both input line and resistive load. On the output The Muon Ionisation Cooling Experiment (MICE) is of the amplifier, the cavity length and hence its resonant being constructed at Rutherford Appleton Laboratory in frequency can be adjusted, whilst a stub tuner is located in the UK. The muon beam will be cooled using multiple the output coax section to alter the coupling factor into hydrogen absorbers then reaccelerated using an RF cavity the output coax so that the amplifier may be used to drive system operating at 201MHz. This paper describes recent a range of different load conditions. For use in the MICE progress in commissioning the amplifier systems at their system the 4616 operates in long pulse mode using grid design operation conditions, installation and operation as pulsed operation and can provide up to 250kW RF output part of the MICE project. power. INTRODUCTION 4616 Power Supply The muon ionisation cooling experiment is a The power supply for the tetrode amplifier consists of a demonstration of practical cooling for future muon TDK-Lambda 500A capacitor charger power supply acceleration schemes. -
Teelllliedi Siteeifieatittil CONTENTS
'. INTERACTIVE GRAPHIC SYSTEMS t;DSn teellllieDI Siteeifieatittil CONTENTS Section Page Section Page 1 Introducing GDS II ........................................... 1-1 4 Specifications ................................................ 4-1 2 General Description .......................................... 2-1 4.1 Database Features ....................................... 4-1 4.2 Input/Editing ............................................ 4-1 2.1 The Problems of VLSI .................................... 2-1 4.3 Display Control .......................................... 4-3 2.2 The Solution - GDS II .................................... 2-1 4.4 Background Programs ................................... 4-4 2.3 Exploiting the Latest Technology .................. , ...... 2-2 4.5 Application Programming Tools .......................... 4-5 4.6 Hardware ............................................... 4-6 3 System Operation ............................................ 3-1 5 Software ..................................................... 5-1 3.1 Database Extensibility ................................... 3-1 3.2 Database Elements ...................................... 3-1 5.1 Multiground RDOS ...................................... 5-1 3.3 Database Construction ................................... 3-2 5.2 Database Management System ........................... 5-3 3.4 Menu Operations ........................................ 3-2 5.3 GPL™ ................................................... 5-7 3.5 Graphic Display ......................................... 3-2 -
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. -
The National Valve Museum
The National Valve Museum Updates August 2016 Added one article:- Focusing Cathode-Rays Added one timeline feature:- October 1966 – Captain H J Round Obituary. Added 108 vintage adverts:- adv-1007 Hivac XFW40 adv-1008 English Electric CRT T901A adv-1009 Osram Audio Output Valves adv-1010 Brimar 12AT7 adv-1011 Mullard 61SV adv-1012 Ediswan Photo-multiplier advert adv-1013 Mazda Brand Advert adv-1014 GEC Brand Advert adv-1015 Hivac Difference Diode Advert adv-1016 Osram Band III TV Valves Advert adv-1017 Ediswan Aluminized TV Tubes Advert adv-1018 Mullard PL81 Advert adv-1019 Ediswan 12E1 Advert adv-1020 Mullard QV06-20 Advert adv-1021 Ediswan Photo-multiplier advert adv-1022 Hivac Flat Sub-miniature Range Advert adv-1023 EMI RK6112 Klystron Advert adv-1024 GEC Rectangular TV Tubes Advert adv-1025 Ediswan Aluminised Television CRT's Advert adv-1026 Mullard EF80 Advert adv-1027 Mullard Valves for VHF Advert adv-1028 Brimar Brand Advert adv-1029 Hivac XR4 Advert adv-1030 Ediswan Glass-Metal Seals Advert adv-1031 Hivac XE2 Advert. adv-1032 Commercial Mullard 5-10 Amplifier Advert adv-1033 English Electric Image Orthicon Advert adv-1034 Thomson-CSF CRTs Advert adv-1035 Brimar M14-100 CRT Advert adv-1036 English Electric 0A2WA Advert adv-1037 English Electric RF Heating Valves Advert adv-1038 GEC New KT88 Advert adv-1039 Brimar D18-130 Advert adv-1040 English Electric CRTs Advert adv-1041 Ferranti Handbooks Advert adv-1042 Mullard Directly-heated Miniatures Advert adv-1043 STC 5A/170K Advert adv-1044 Ferranti Ceramic Valves Advert adv-1045 Westinghouse -
7.4 UV, Visible and Near IR Detectors
7.4 UV, Visible and Near IR Detectors • in the photoelectric effect light ejects an electron from a metal surface • a vacuum phototube converts a light flux into an electrical current, and is useful for detecting high levels of light • a photomultiplier converts a single photon into a current pulse, and is useful for detecting low levels of light • photodiodes are based on the promotion of electrons from the valence band to the conduction band of semiconductors, and are useful for detecting both high and low levels of light 7.4 : 1/8 Photoelectric Effect • because metals contain free electrons they can absorb UV, visible, and near IR radiation • if the energy of the absorbed photon is greater than the ______ ________ of the metal, an electron is ejected into the vacuum • the energy of the photon equals the work function of the metal plus the kinetic energy of the electron hc1 hc =+mv2 ωλ = λ 2 0 ω where ω is the work function, and λ0 is the wavelength that just barely ejects an electron • alkali metals are commonly used in detectors metal Li Na K Rb Cs ω 2.9 eV 2.75 2.3 2.16 2.14 λ0 428 nm 451 539 574 579 • mixtures of alkali metals can give λ0 as high as ______ nm • because __________ energy can combine with optical energy, the onset of photo-ejection is gradual 7.4 : 2/8 Vacuum Phototube A metallic surface with a low work function is placed inside an evacuated tube. When light interacts with the metal, electrons are photo-ejected. -
Of 38 an Inexpensive VTCT Adapter for All Tektronix Scts Version. 1.04.1
Page 1 of 38 An Inexpensive VTCT Adapter for All Tektronix SCTs Version. 1.04.1 Page 2 of 38 An Inexpensive VTCT Adapter for All Tektronix SCTs Version. 1.04.1 Figure 1 Front cover—Tektronix 577 Semiconductor Curve Tracer displaying the characteristic curves of a TRIODE VACUUM TUBE. Page 3 of 38 An Inexpensive VTCT Adapter for All Tektronix SCTs Version. 1.04.1 AN INEXPENSIVE VACUUM TUBE CURVE TRACER ADAPTER FOR ALL TEKTRONIX SEMICONDUCTOR CURVE TRACERS © Dennis Tillman W7pF, [email protected], Version 1.04.1, Mar. 10, 2020 CONTENTS INTRODUCTION ................................................................................................................................... 5 TEKTRONIX CURVE TRACER FEATURE COMPARISON .................................................................. 6 TEKTRONIX CURVE TRACERS .......................................................................................................... 6 VACUUM TUBE TESTER FEATURE COMPARISON .......................................................................... 8 THEORY OF OPERATION .................................................................................................................. 11 EICO 667 MODIFICATIONS................................................................................................................ 13 WHAT CAN I EXPECT WITH THE CURVE TRACER I MAY ALREADY OWN? ................................ 13 WHAT YOU WILL NEED TO MAKE THIS VTCT ................................................................................ 14 TWO CHARACTERISTIC CURVES