Fundamental Characteristics of Thyristors Application Note
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TRIAC Overvoltage Protection Using a Transil™
AN1966 Application note TRIAC overvoltage protection using a Transil™ Introduction In most of their applications, TRIACs are directly exposed to overvoltages coming from the mains, as described in IEC 61000-4-5 or IEC 61000-4-4 standards. When TRIACs are used to drive resistive loads (ex: temperature regulation), it is essential to provide them with efficient overvoltage protection to prevent any turn-on in breakover mode that could lead to device damage. A traditional method to clamp the voltage is to use a varistor in parallel across the TRIAC. But with high power loads (a few kW), the current through the varistor is very high in case of surge voltages (a few hundred amperes). The varistor is then not efficient enough, due to its dynamic resistor, to limit the TRIAC voltage to a low value. We present here a solution that can be used for these kinds of applications and also for all applications where TRIAC voltage protection is required. It should be noted that the overvoltages could also come from the overvoltages that appear at device turn-off due to the TRIAC holding current. This phenomenon occurs mainly with TRIACs controlling low rms current (15-50 mA), high inductive loads like valves. For more information about such behavior, please refer to AN1172. Contents 1 Why overvoltage protection is required . 2 2 Overvoltage protection solution . 3 3 Transil choice for efficient TRIAC voltage protection . 6 3.1 Normal operation: check VRM voltage . 6 3.2 Surge voltage clamping: check max VCL voltage . 6 4 Experimental validation example . 8 5 Conclusion . -
Thyristor Switches
CHAPTER 5 Thyristor Switches Limits of the traditional contactor switched banks • High inrush current and over voltages • Risk of over voltages due to the arc breaking • Longer reconnecting time: more than 30 sec • More demanding maintenance compared with static switches. General advantages of Power Factor Correction • Reduced losses on mains and power transformers • Increase of plant available power • Less voltage drop in the plant Thyristor switched capacitor bank benefits include: • Minimises network disturbances such as Voltage Drop and Flicker Thyristor switched capacitor bank is the best and sometimes • No moving parts therefore reduced maintenance (i.e. no the sole choice when it is necessary to compensate loads Electro-magnetic contactors) over short periods of time. Examples are steel companies, • Enhanced capacitor life expectancy. lifting apparatus (cranes, quay cranes, etc), cable makers (extruders, etc), welding machines, robots, compressors, In general there is a comprehensive PLANT EFFICIENCY; skiing lift stations, LV industrial networks (chemical plants, because power factor correction is fast, the power paper mills, automotive suppliers). Thyristor switched transformer and line design can be done considering only capacitor bank are also an ergonomic solution where noise the actual load. can be problematic, like hotels, banks, offices, service Therefore longer working life and reliability of plant. infrastructures (telecommunications board, informatics Static switches allow unlimited operations. ’boards, hospitals, malls). Steps switching is also done limiting transient phenomena that inside normal plants stresses the capacitors reducing their working life. General Characteristics ICAR SINCHRO FAST SWITCH FEATURES are Further ADVANTAGES described below: 1. 1Possibility to use SFS with ICAR RPE 12BTA regulator. • Switching speed: 60ms 2. -
Present Status and Future Prospects for Power Semiconductors
Present Status and Future Prospects for Power Semiconductors Ken’ya Sakurai 1. Introduction (1) Devices related to multimedia ① High-voltage silicon diodes and damper diodes From the viewpoint of a highly information-orient- with high-speed switching performance to im- ed society in the coming 21st century, the social prove the picture quality of the CRT (cathode infrastructure will undergo rapid repairs and reforma- ray tube) display monitors and televisions tions. What will bring us to a society where computers ② Low on-resistance SOP-8 power MOSFETs and communications are closely intertwined? Techni- that extend the battery life of portable elec- cal innovations have always brought us advantages as tronic appliances such as notebook computers well as disadvantages. Any future technical innova- (2) Vehicles and rolling stock tions must definitely exclude disadvantages. ① Intelligent power MOSFETs that decrease the A highly information-oriented society will result in size and improve reliability of car electronics a great increase in electric energy consumption. Prob- systems lems of the global environment, social environment, ② High-voltage, high-power NPT (non punch- and energy resources must be improved through more through)-IGBT modules and flat IGBTs that serious consideration, with electrical manufactures reduce rolling stock size, weight, and energy leading these technical innovations. Development of consumption high power generation and conversion efficiency and (3) Power conversion (inverter control) energy-saving technology for electron devices are core ① Molded IGBTs, IGBT modules, and IGBT-IPMs technologies. More specifically, power electronics that for applications including NC (numerical con- control electric energy increases in importance, and trol) equipment, general-purpose inverters, especially power semiconductor devices as the key servo mechanisms, welding machines, and devices are required for further advances in perfor- UPSs (uninterruptible power system) mance and functions. -
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. -
Triac Control with a Microcontroller Powered from a Positive Supply
AN440 Application note Triac control with a microcontroller powered from a positive supply Introduction This application note explains how to implement a control circuit to drive an AC switch (Triac, ACS or ACST) in case the microcontroller unit (MCU) is supplied with a positive voltage. The driving circuit will also depends on the kind of Triac used and also if other supplies (positive or negative) are available. We also deal about the case of insulated or non-insulated supplies. It is recommended to refer to AN4564 which explains why positive supplies are usually implemented and how simple solutions can be implemented to get a negative supply. Refer also to AN3168 for information about AC switch control circuits in case the microcontroller is supplied with a negative power supply. AN440 - Rev 4 - March 2020 www.st.com For further information contact your local STMicroelectronics sales office. AN440 Positive supply defintion and AC switch triggering quadrants 1 Positive supply defintion and AC switch triggering quadrants 1.1 Positive power supply A positive power supply is a supply where its reference level (VSS) is connected to the mains (line or neutral). The VDD level is then above the mains terminal as shown in Figure 1. If the supply is a 5 V power supply, then VDD is 5 V above the mains reference. This is why such a supply is called a positive supply (compared to a negative supply as shown in AN3168). Figure 1. Positive supply basic schematic 1.2 AC switch triggering quadrants To switch-on an AC switch, like any bipolar device, a gate current must be applied between its gate pin (G) and its drive reference terminal (refer also to AN3168). -
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. -
An Application of TRIAC to Capacitor Motor for Hermetic Compressor K
Purdue University Purdue e-Pubs International Compressor Engineering Conference School of Mechanical Engineering 1984 An Application of TRIAC to Capacitor Motor for Hermetic Compressor K. Nakane Y. Tozaki H. Sakamoto Follow this and additional works at: https://docs.lib.purdue.edu/icec Nakane, K.; Tozaki, Y.; and Sakamoto, H., "An Application of TRIAC to Capacitor Motor for Hermetic Compressor" (1984). International Compressor Engineering Conference. Paper 449. https://docs.lib.purdue.edu/icec/449 This document has been made available through Purdue e-Pubs, a service of the Purdue University Libraries. Please contact [email protected] for additional information. Complete proceedings may be acquired in print and on CD-ROM directly from the Ray W. Herrick Laboratories at https://engineering.purdue.edu/ Herrick/Events/orderlit.html AN APPLICA'l'ION OF 'l'RIAC TO CAPACI'l'OR 1-10'l'OR FOR lll~Rt~IC'riC COMPRSSO!l Ka.zuhiro Nakane, Yasuhiro To?.nki,. Ilirota.ka Sakamoto Shizuoka. Worlw, Mitsubishi Electri.c Corporation Shizuoka City , Ja.pan ABSTRACT oncy and output rati.ngo are 100 V ,50/60 J!v. and 100 11. It is a. 1mi 1 t-in motor for the rotary type This paper refers to a.n n.pplication study of 'l'lUAC hermetic compressor shown in Ji'ie;. 2. 'l'hore are to PSC motor for thft hermetic compessor. It is three types of the wirings of the starting device 1-1ell lcnown that 'l'HIAC rlel nys pharJa ane,le of the for thifl motor,as shown i.n lcig, 3. A shows CSR current and has no losses if it is consider(\ as moto:r,n shows P'l'C asoist CSR motor and C sho~1s ideal flwitch. -
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. -
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. -
Thyristors & Triacs
APPLICATION NOTE Thyristors & Triacs - Ten Golden Rules for Success In Your Application. This Technical Publication aims to provide an threshold current IGT, within a very short time known as interesting, descriptive and practical introduction to the the gate-controlled turn-on time, tgt, the load current can golden rules that should be followed in the successful flow from ’a’ to ’k’. If the gate current consists of a very use of thyristors and triacs in power control applications. narrow pulse, say less than 1µs, its peak level will have to increase for progressively narrower pulse widths to Thyristor guarantee triggering. A thyristor is a controlled rectifier where the When the load current reaches the thyristor’s latching unidirectional current flow from anode to cathode is current IL, load current flow will be maintained even after initiated by a small signal current from gate to cathode. removal of the gate current. As long as adequate load current continues to flow, the thyristor will continue to akconduct without the gate current. It is said to be latched ON. Note that the VGT,IGT and IL specifications given in data g are at 25 ˚C. These parameters will increase at lower temperatures, so the drive circuit must provide adequate Fig. 1. Thyristor. voltage and current amplitude and duration for the The thyristor’s operating characteristic is shown in lowest expected operating temperature. Fig. 2. Rule 1. To turn a thyristor (or triac) ON, a gate current On-state ≥ Forward IGT must be applied until the load current is current characteristic ≥ IL. This condition must be met at the lowest expected operating temperature.