68 Chapter 9: Thyristors Thyristors Thyristors Are a Class Of
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Unit-1 Mphycc-7 Ujt
UNIT-1 MPHYCC-7 UJT The Unijunction Transistor or UJT for short, is another solid state three terminal device that can be used in gate pulse, timing circuits and trigger generator applications to switch and control either thyristors and triac’s for AC power control type applications. Like diodes, unijunction transistors are constructed from separate P-type and N-type semiconductor materials forming a single (hence its name Uni-Junction) PN-junction within the main conducting N-type channel of the device. Although the Unijunction Transistor has the name of a transistor, its switching characteristics are very different from those of a conventional bipolar or field effect transistor as it can not be used to amplify a signal but instead is used as a ON-OFF switching transistor. UJT’s have unidirectional conductivity and negative impedance characteristics acting more like a variable voltage divider during breakdown. Like N-channel FET’s, the UJT consists of a single solid piece of N-type semiconductor material forming the main current carrying channel with its two outer connections marked as Base 2 ( B2 ) and Base 1 ( B1 ). The third connection, confusingly marked as the Emitter ( E ) is located along the channel. The emitter terminal is represented by an arrow pointing from the P-type emitter to the N-type base. The Emitter rectifying p-n junction of the unijunction transistor is formed by fusing the P-type material into the N-type silicon channel. However, P-channel UJT’s with an N- type Emitter terminal are also available but these are little used. -
Thyristors.Pdf
THYRISTORS Electronic Devices, 9th edition © 2012 Pearson Education. Upper Saddle River, NJ, 07458. Thomas L. Floyd All rights reserved. Thyristors Thyristors are a class of semiconductor devices characterized by 4-layers of alternating p and n material. Four-layer devices act as either open or closed switches; for this reason, they are most frequently used in control applications. Some thyristors and their symbols are (a) 4-layer diode (b) SCR (c) Diac (d) Triac (e) SCS Electronic Devices, 9th edition © 2012 Pearson Education. Upper Saddle River, NJ, 07458. Thomas L. Floyd All rights reserved. The Four-Layer Diode The 4-layer diode (or Shockley diode) is a type of thyristor that acts something like an ordinary diode but conducts in the forward direction only after a certain anode to cathode voltage called the forward-breakover voltage is reached. The basic construction of a 4-layer diode and its schematic symbol are shown The 4-layer diode has two leads, labeled the anode (A) and the Anode (A) A cathode (K). p 1 n The symbol reminds you that it acts 2 p like a diode. It does not conduct 3 when it is reverse-biased. n Cathode (K) K Electronic Devices, 9th edition © 2012 Pearson Education. Upper Saddle River, NJ, 07458. Thomas L. Floyd All rights reserved. The Four-Layer Diode The concept of 4-layer devices is usually shown as an equivalent circuit of a pnp and an npn transistor. Ideally, these devices would not conduct, but when forward biased, if there is sufficient leakage current in the upper pnp device, it can act as base current to the lower npn device causing it to conduct and bringing both transistors into saturation. -
Robust Wireless Power Transfer Using a Nonlinear Parity–Time-Symmetric Circuit Sid Assawaworrarit1, Xiaofang Yu1 & Shanhui Fan1
LETTER doi:10.1038/nature22404 Robust wireless power transfer using a nonlinear parity–time-symmetric circuit Sid Assawaworrarit1, Xiaofang Yu1 & Shanhui Fan1 Considerable progress in wireless power transfer has been made in PT-symmetric systems are invariant under the joint parity and the realm of non-radiative transfer, which employs magnetic-field time reversal operation14,15. In optical systems, where the symmetry coupling in the near field1–4. A combination of circuit resonance conditions can be met by engineering the gain/loss regions and and impedance transformation is often used to help to achieve their coupling, PT-symmetric systems have exhibited unusual efficient transfer of power over a predetermined distance of about properties16–20. A linear PT-symmetric system supports two phases, the size of the resonators3,4. The development of non-radiative depending on the magnitude of the gain/loss relative to the coupling wireless power transfer has paved the way towards real-world strength. In the unbroken or exact phase, eigenmode frequencies applications such as wireless powering of implantable medical remain real and energy is equally distributed between the gain and devices and wireless charging of stationary electric vehicles1,2,5–8. loss regions; in the broken phase, one of the eigenmodes grows expo- However, it remains a fundamental challenge to create a wireless nentially while the other decays exponentially. Recently, the concept power transfer system in which the transfer efficiency is robust of PT symmetry has been extensively explored in laser structures21–24. against the variation of operating conditions. Here we propose Theoretically, the inclusion of nonlinear gain saturation in the analysis theoretically and demonstrate experimentally that a parity–time- of a PT-symmetric system causes that system to reach a steady state symmetric circuit incorporating a nonlinear gain saturation element in a laser-like fashion that still contains the following PT symmetry provides robust wireless power transfer. -
ON Semiconductor Is Depicted in Figure 29
ON Semiconductor Is Now To learn more about onsemi™, please visit our website at www.onsemi.com onsemi and and other names, marks, and brands are registered and/or common law trademarks of Semiconductor Components Industries, LLC dba “onsemi” or its affiliates and/or subsidiaries in the United States and/or other countries. onsemi owns the rights to a number of patents, trademarks, copyrights, trade secrets, and other intellectual property. A listing of onsemi product/patent coverage may be accessed at www.onsemi.com/site/pdf/Patent-Marking.pdf. onsemi reserves the right to make changes at any time to any products or information herein, without notice. The information herein is provided “as-is” and onsemi makes no warranty, representation or guarantee regarding the accuracy of the information, product features, availability, functionality, or suitability of its products for any particular purpose, nor does onsemi assume any liability arising out of the application or use of any product or circuit, and specifically disclaims any and all liability, including without limitation special, consequential or incidental damages. Buyer is responsible for its products and applications using onsemi products, including compliance with all laws, regulations and safety requirements or standards, regardless of any support or applications information provided by onsemi. “Typical” parameters which may be provided in onsemi data sheets and/ or specifications can and do vary in different applications and actual performance may vary over time. All operating parameters, including “Typicals” must be validated for each customer application by customer’s technical experts. onsemi does not convey any license under any of its intellectual property rights nor the rights of others. -
68 Chapter 9: Thyristors Thyristors Thyristors Are a Class Of
Electronic Devices Chapter 9: Thyristors Thyristors Thyristors are a class of semiconductor devices characterized by 4-layers of alternating p- and n-material. Four-layer devices act as either open or closed switches; for this reason, they are most frequently used in control applications such as lamp dimmers, motor speed controls, ignition systems, charging circuits, etc. Thyristors include Shockley diode, silicon-controlled rectifier (SCR), diac and triac. They stay on once they are triggered, and will go off only if current is too low or when triggered off. Some thyristors and their symbols are in figure 1. (a) 4-layer diode (b) SCR (c) Diac (d) Triac (e) SCS Figure 1 Shockley Diode The 4-layer diode (or Shockley diode) is a type of thyristor that acts something like an ordinary diode but conducts in the forward direction only after a certain anode to cathode voltage called the forward-breakover voltage is reached. The basic construction of a 4-layer diode and its schematic symbol are shown in Figure 2. Figure 2: The 4-layer diode. The 4-layer diode has two leads, labeled the anode (A) and the cathode (K). The symbol reminds you that it acts like a diode. It does not conduct when it is reverse-biased. The concept of 4-layer devices is usually shown as an equivalent circuit of a pnp and an npn transistor. Ideally, these devices would not conduct, but when forward biased, if there is sufficient leakage current in the upper pnp device, it can act as base current to the lower npn device causing it to conduct and bringing both transistors into saturation 68 Assist. -
50 Simple L.E.D. Circuits
50 Simple L.E.D. Circuits R.N. SOAR r de Historie v/d Radi OTH'IEK 50 SIMPLE L.E.D. CIRCUITS by R. N. SOAR BABANI PRESS The Publishing Division of Babani Trading and Finance Co. Ltd. The Grampians Shepherds Bush Road London W6 7NI- England Although every care is taken with the preparation of this book, the publishers or author will not be responsible in any way for any errors that might occur. © 1977 BA BAN I PRESS I.S.B.N. 0 85934 043 4 First Published December 1977 Printed and Manufactured in Great Britain by C. Nicholls & Co. Ltd. f t* -i. • v /“ ..... tr> CONTENTS U.V.H.R* Circuit Page No. 1 LED Pilot Light......................................... 7 2 LED Stereo Beacon.................................... 8 3 Stereo Decoder Mono/Sterco Indicator . 9 4 Subminiature LED Torch........................... 10 5 Low Voltage Low Current Supply............ 11 6 Microlight Indicator .................................. 12 7 Ultra Low Current LED Switching Indicator 13 8 LED Stroboscope....................................... 14 9 12 Volt Car Circuit Tester........................... 15 10 Two Colour LED......................................... 16 11 12 Volt Car “Fuse Blown” Indicator.......... 17 12 LED Continuity Tester............................... 17 13 LED Current Overload Indicator.............. 18 14 LED Current Range Indicator................... 20 15 1.5 Volt LED “Zener”................. '............ 22 16 Extending Zener Voltage........................... 22 17 Four Voltage Regulated Supply................. 23 18 PsychaLEDic Display.................................. 24 .19 Dual Colour Display.................................... 25 20 Dual Signal Device....................................... 26 21 LED Triple Signalling.................................. 27 22 Sub-Miniature Light Source for Model Railways . 28 23 Portable Television Protection Circuit . 29 24 Improved Portable TV Protection Circuit 30 25 LED Battery Tester.............................. -
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. -
Shults Robert D 196308 Ms 10
AN INVESTIGATION OF THE INFLUENCE OF CIRCUIT PARAMETERS ON THE OUTPUT WAVESHAPE OF A TUNNEL DIODE OSCILLATOR A THESIS Presented to The Faculty of the Graduate Division by Robert David Shults In Partial Fulfillment of the Requirements for the Degree Master of Science in Electrical Engineering Georgia Institute of Technology June, I963 AN INVESTIGATION OF THE INFLUENCE OF CIRCUIT PARAMETERS ON THE OUTPUT WAVESHAPE OF A TUNNEL DIODE OSCILLATOR Approved: —VY -w/T //'- Dr. W. B.l/Jonesj UJr. (Chairman) _A a t~l — Dry 3* L. Hammond, Jr. V ^^ __—^ '-" ^^ *• Br> J. T. Wang * Date Approved by Chairman: //l&U (A* l/j^Z) In presenting the dissertation as a partial, fulfillment of the requirements for an advanced degree from the Georgia Institute of Technology, I agree that the Library of the Institution shall make it available for inspection and circulation in accordance witn its regulations governing materials of this type. I agree -chat permission to copy from, or to publish from, this dissertation may be granted by the professor under whose direction it was written^ or, in his absence, by the dean of the Graduate Division when luch copying or publication is solely for scholarly purposes ftad does not involve potential financial gain. It is under stood that any copying from, or publication of, this disser tation which involves potential financial gain will not be allowed without written permission. _/2^ d- ii ACKNOWLEDGMEBTTS The author wishes to thank his thesis advisor, Dr. W. B„ Jones, Jr., for his suggestion of the problem and for his continued guidance and encouragement during the course of the investigation. -
The Transistor
Chapter 1 The Transistor The searchfor solid-stateamplification led to the inventionof the transistor. It was immediatelyrecognized that majorefforts would be neededto understand transistorphenomena and to bring a developedsemiconductor technology to the marketplace.There followed a periodof intenseresearch and development, duringwhich manyproblems of devicedesign and fabrication, impurity control, reliability,cost, and manufacturabilitywere solved.An electronicsrevolution resulted,ushering in the eraof transistorradios and economicdigital computers, alongwith telecommunicationssystems that hadgreatly improved performance and that were lower in cost. The revolutioncaused by the transistoralso laid the foundationfor the next stage of electronicstechnology-that of silicon integratedcircuits, which promised to makeavailable to a massmarket infinitely more complexmemory and logicfunctions that could be organizedwith the aid of softwareinto powerfulcommunications systems. I. INVENTION OF THE TRANSISTOR 1.1 Research Leading to the Invention As World War II was drawing to an end, the research management of Bell Laboratories, led by then Vice President M. J. Kelly (later president of Bell Laboratories), was formulating plans for organizing its postwar basic research activities. Solid-state physics, physical electronics, and mi crowave high-frequency physics were especially to be emphasized. Within the solid-state domain, the decision was made to commit major research talent to semiconductors. The purpose of this research activity, according -
The Unijunction Transistor
ASE The Unijunction Transistor The unijunction transistor The unijunction transistor was one of the most attractive, simple and versatile semiconductor devices made available to electronic designers until discrete components were replaced by integrated circuits. The device was introduced in 1955 by General Electric. Here the article from Electronics, March 1955. In the article the device was referred to as a double base diode but soon later the name was changed to unijunction transistor or UJT UJT was a simple device, a silicon N-type bar with two ohmic contacts at both ends and a P-N junction about at two third of its length. The intermediate electrode is called emitter, while the two end contacts are referred to as B1 and B2 bases, B1 being the one farthest from the emitter. The construction of UJT and the related symbol are given in the figure below: Fig. 1 - Symbols used for UJT and internal construction of the device. The interbase resistance is somewhere from 5 and 10 kohms. B2 is normally biased at a positive voltage, Vbb, and B1 is grounded, the silicon bar acting as a voltage divider. No current can pass through the emitter until the P-N junction is reverse- biased. The conduction can take place only at an emitter voltage equal to the voltage existing on the voltage divider plus the direct drop on the junction, 0.67 volt at 25ºC. This value is defined by the intrinsic stand-off ratio, η, which is equivalent to the internal partition ratio. Fig. 2 - Equivalent circuit of UJT and influence of emitter current on Rb1 resistance. -
EC 8252 – ELECTRON DEVICES Department of ECE UNIT V – POWER & DISPLAY DEVICE
EC 8252 – ELECTRON DEVICES Department of ECE UNIT V – POWER & DISPLAY DEVICE UJT (UNIJUNCTION TRANSISTOR) UJT is a three terminal semiconductor switching device. As it has only one PN junction and three leads it is commonly NUTSHELL called as Unijunction Transistor. Three Terminal Basic Structure One PN junction It consists of a lightly doped N – type silicon bar with a heavily doped P – type material alloyed to its one side closer to B2 for producing single PN junction. The emitter leg is drawn at an angle vertical and the arrow indicates the direction of conventional current. Basic StructureCircuit Symbol Equivalent Circuit Characteristics of UJT: Interbase Resistance between B2 and B1of the silicon bar NUTSHELL is . With emitter terminal open, if voltage VBB is applied between the two bases, a voltage gradient is Voltage V1 reverse biased established along the N – type bar. Positive voltage VE Negative voltage VE The voltage drop across RB1 is Intrinsic Stand – off ratio, (typical value of η ranges from 0.56 to 0.75) 2020-2021 Jeppiaar Institute of Technology EC 8252 – ELECTRON DEVICES Department of ECE UNIT V – POWER & DISPLAY DEVICE The voltage V1 reverse biases the PN junction and emitter current is cut – off. But a small leakage current flows from B2 to emitter due to minority carriers. If a positive voltage VE is applied to emitter, the PN junction will remain reverse biased so long as VE < V1. If VE exceeds V1 by the cut – in voltage Vγ, the diode becomes forward biased. Under this condition, holes are injected into the N – type Bar. -
Effect of Load Impedance on the Performance of Microwave Negative Resistance Oscillators
Effect of Load Impedance on the Firas M. Ali , Suhad H. Jasim Issue No. 39/2016 Performance of Microwave… Effect of Load Impedance on the Performance of Microwave Negative Resistance Oscillators Firas Mohammed Ali Al-Raie [email protected] University of Technology - Department of Electrical Engineering - Baghdad - Iraq Suhad Hussein Jasim [email protected] University of Technology - Department of Electrical Engineering - Baghdad - Iraq Abstract: In microwave negative resistance oscillators, the RF transistor presents impedance with a negative real part at either of its input or output ports. According to the conventional theory of microwave negative resistance oscillators, in order to sustain oscillation and optimize the output power of the circuit, the magnitude of the negative real part of the input/output impedance should be maximized. This paper discusses the effect of the circuit’s load impedance on the input negative resistance and other oscillator performance characteristics in common base microwave oscillators. New closed-form relations for the optimum load impedance that maximizes the magnitude of the input negative resistance have been derived analytically in terms of the Z- parameters of the RF transistor. Furthermore, nonlinear CAD simulation is carried out to show the deviation of the large-signal Journal of Al Rafidain University College 427 ISSN (1681-6870) Effect of Load Impedance on the Firas M. Ali , Suhad H. Jasim Issue No. 39/2016 Performance of Microwave… optimum load impedance from its small-signal value. It has been shown also that the optimum load impedance for maximum negative input resistance differs considerably from its value required for maximum output power under large-signal conditions.