A Tesla-Blumlein PFL-Bipolar Pulsed Power Generator Laurent Pecastaing, Meng Wang

Total Page:16

File Type:pdf, Size:1020Kb

A Tesla-Blumlein PFL-Bipolar Pulsed Power Generator Laurent Pecastaing, Meng Wang A Tesla-Blumlein PFL-Bipolar Pulsed Power Generator Laurent Pecastaing, Meng Wang To cite this version: Laurent Pecastaing, Meng Wang. A Tesla-Blumlein PFL-Bipolar Pulsed Power Generator. Electro- magnetism. Loughborough University, 2016. English. tel-02372305 HAL Id: tel-02372305 https://hal-univ-pau.archives-ouvertes.fr/tel-02372305 Submitted on 20 Nov 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Meng Wang A Tesla-Blumlein PFL-Bipolar Pulsed Power Generator by Meng Wang, MSc, BEng A Doctoral Thesis submitted in partial fulfilment of the requirements for the award of Doctor of Philosophy of Loughborough University, UK March 2016 © Meng Wang, 2016 Meng Wang Acknowledgements I would like to express my sincere gratitude and to acknowledge the assistance and continuous support received from my supervisor Professor Bucur Novac, who was a constant source of inspiration and expert advice during my research work. I am very fortunate to have been associated with him. Special thanks are also due to thank Professor Ivor Smith for his efforts and I am also grateful to him for his reviews and advice throughout the writing of the thesis. I am very grateful to Mr. Keith Stanley for his technical assistance in designing and constructing the experimental systems and his advice related to numerous mechanical problems. Without his help none of the systems described would have been built. I would also like to thank Mr. Peter Senior and other colleagues in the Plasma and Pulsed Power Group at Loughborough University, for providing friendly help. I must reserve a special thank you for my parents Mr. Xuemin Wang and Mrs Shegai Li who supported me during the course of this degree, without their support none of the work described would have been possible. I would like to thank my husband Mr. Long Yu for his unconditional constant support and patience during this period. He has shared all the achievements and frustrations. Finally, I would like to thank all my other friends who helped to keep my confidence up and to be there when I needed them. i Meng Wang Abstract A Tesla-Blumlein PFL-Bipolar pulsed power generator, has been successfully designed, manufactured and demonstrated. The compact Tesla transformer that it employs has successfully charged capacitive loads to peak voltages up to 0.6 MV with an overall energy efficiency in excess of 90% . The Tesla–driven Blumlein PFL generator is capable of producing a voltage impulse approaching 0.6 MV with a rise time close to 2 ns, generating a peak electrical power of up to 10 GW for 5 ns when connected to a 30 Ω resistive load. Potentially for medical application, a bipolar former has been designed and successfully implemented as an extension to the system and to enable the generation of a sinusoid-like voltage impulse with a peak-to-peak value reaching 650 kV and having a frequency bandwidth beyond 1 GHz. This thesis describes the application of various numerical techniques used to design a successful generator, such as filamentary modelling, electrostatic and transient (PSpice) circuit analysis, Computer Simulation Technology (CST) simulation. All the major parameters of both the Tesla transformer, the Blumlein pulse forming line and the bipolar former were determined, enabling accurate modelling of the overall unit to be performed. The wide bandwidth and ultrafast embedded sensors used to monitor the dynamic characteristics of the overall system are also presented. Experimental results obtained during this major experimental programme are compared with theoretical predictions and the way ahead towards connecting to an antenna for medical application is considered. ii Meng Wang List of Principal Symbols 퐿푝 primary inductance 퐿푠 secondary inductance 퐶푝 primary capacitance 퐶푠 secondary capacitance 푞푝 electric charge on primary capacitance 푞푠 electric charge on secondary capacitance 휔푝 resonant frequency of primary circuit 휔푠 resonant frequency of secondary circuit k coupling coefficient 휔1 angular resonant frequency of primary circuit 휔2 angular resonant frequency of secondary circuit η energy transfer efficiency 푄푝 quality factor of primary circuit 푄푠 quality factor of secondary circuit τ damping time constant 푀푖,푗 mutual inductance between the 푖푡ℎ and the 푗푡ℎ filaments 푟푝 inner radius of primary winding 푤푝 axial length of primary winding ℎ푝 thickness of primary winding δ skin depth 푝 푍푖 position in axis Z of primary filaments 푝 푅푖 position in axis R of primary filaments K(k) complete elliptic integral of the first kind E(k) complete elliptic integral of the second kind 푟푟 radius of secondary winding iii Meng Wang 푤푠 axial length of secondary winding p axial pitch of the former of secondary rings 푅푠0 radius to bottom of the first ring of secondary winding 푅푠29 radius to bottom of the last ring of secondary winding 푠 푍푖 position in axis Z of secondary filaments 푠 푅푖 position in axis R of secondary filaments 퐸푏 pulse breakdown voltage 푄푖 electric charge of 푖푡ℎ conductor 0 푉푗 potential of 푗푡ℎ conductor relative to conductor 0 퐵푖,푗 Maxwell coefficients between 푖푡ℎ conductor and 푗푡ℎ conductor 푟1 radius of Blumlein PFL outer cylinder 푟2 radius of Blumlein PFL middle cylinder 푟3 radius of Blumlein PFL inner cylinder 푍1 characteristic impedance of Blumlein PFL inner line 푍2 characteristic impedance of Blumlein PFL outer line 푍′ load impedance of Blumlein PFL 휀푟 relative permittivity of dielectric material 휇푟 relative permeability of dielectric material 푙퐵 length of Blumlein PFL v wave propagation velocity 휀0 permittivity of vacuum ρ resistivity of dielectric 푑1 diameter of bipolar former inner electrode 푑2 internal diameter of bipolar former intermediate electrode ′ 푑2 outer diameter of bipolar former intermediate electrode 푑3 internal diameter of bipolar former outer electrode 휆푐 cut-off wavelength iv Meng Wang 푓푐 cut-off frequency v Meng Wang Contents 1. Introduction ............................................................................................................. 1 1.1. Introduction to Pulsed Power technology ....................................................... 1 1.2. Literature review ............................................................................................. 3 History of Pulsed Power .................................................................... 3 Examples of outstanding pulsed power generators ............................ 5 1.3. Applications of Pulsed Power Technology ................................................... 11 1.4. Aim of the thesis ........................................................................................... 15 1.5. Outline of the thesis ....................................................................................... 16 1.6. References ..................................................................................................... 18 2. Tesla transformer .................................................................................................. 22 2.1. Introduction and history of Tesla transformers ............................................. 22 2.2. Tesla transformer theory ............................................................................... 26 Lossless circuit (푹풑 = 푹풔 = ퟎ) ....................................................... 29 Low-loss circuit ............................................................................... 31 2.3. Modelling of Tesla transformer ..................................................................... 34 Filamentary modelling ..................................................................... 34 Electrostatic modelling .................................................................... 43 2.4. References ..................................................................................................... 49 3. Blumlein pulse forming line ................................................................................. 54 3.1. Fundamentals of Blumlein pulse forming line .............................................. 54 vi Meng Wang Introduction of Blumlein pulse forming line ................................... 54 Circuit Analysis ............................................................................... 56 3.2. Design consideration and procedure ............................................................. 59 Design consideration ........................................................................ 59 Dielectric .......................................................................................... 60 Electrostatic modelling .................................................................... 62 3.3. Overall configuration and manufacture ......................................................... 64 3.4. References ..................................................................................................... 66 4. Bipolar former ....................................................................................................... 68 4.1. Introduction of bipolar former ....................................................................... 68 Motivation
Recommended publications
  • Evaluation of Monte Carlo Tools for High Energy Atmospheric Physics
    Evaluation of Monte Carlo tools for high energy atmospheric physics Casper Rutjes1, David Sarria2, Alexander Broberg Skeltved3, Alejandro Luque4, Gabriel Diniz5,6, Nikolai Østgaard3, and Ute Ebert1,7 1Centrum Wiskunde & Informatica (CWI), Amsterdam, The Netherlands 2Astroparticules et Cosmologie, University Paris VII Diderot, CNRS/IN2P3, France 3Department of Physics and Technology, University of Bergen, 5020 Bergen, Norway 4Instituto de Astrofisica de Andalucia (IAA-CSIC), PO Box 3004, Granada, Spain 5Instituto Nacional de Pesquisas Espaciais, Brazil 6Instituto de Física, Universidade de Brasília, Brazil 7Eindhoven University of Technology, Eindhoven, The Netherlands Correspondence to: Casper Rutjes ([email protected]) Abstract. The emerging field of high energy atmospheric physics (HEAP) includes Terrestrial Gamma-ray Flashes, electron- positron beams and gamma-ray glows from thunderstorms. Similar emissions of high energy particles occur in pulsed high voltage discharges. Understanding these phenomena requires appropriate models for the interaction of electrons, positrons and photons of up to 40 MeV energy with atmospheric air. In this paper we benchmark the performance of the Monte Carlo codes 5 Geant4, EGS5 and FLUKA developed in other fields of physics and of the custom made codes GRRR and MC-PEPTITA against each other within the parameter regime relevant for high energy atmospheric physics. We focus on basic tests, namely on the evolution of monoenergetic and directed beams of electrons, positrons and photons with kinetic energies between 100 keV and 40 MeV through homogeneous air in the absence of electric and magnetic fields, using a low energy cut-off of 50 keV. We discuss important differences between the results of the different codes and provide plausible explanations.
    [Show full text]
  • Lecture 09 Closing Switches.Pdf
    High-voltage Pulsed Power Engineering, Fall 2018 Closing Switches Fall, 2018 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University Switch fundamentals The importance of switches in pulsed power systems In high power pulse applications, switches capable of handling tera-watt power and having jitter time in the nanosecond range are frequently needed. The rise time, shape, and amplitude of the generator output pulse depend strongly on the properties of the switches. The basic principle of switching is simple: at a proper time, change the property of the switch medium from that of an insulator to that of a conductor or the reverse. To achieve this effectively and precisely, however, is rather a complex and difficult task. It involves not only the parameters of the switch and circuit but also many physical and chemical processes. 2/44 High-voltage Pulsed Power Engineering, Fall 2018 Switch fundamentals Design of a switch requires knowledge in many areas. The property of the medium employed between the switch electrodes is the most important factor that determines the performance of the switch. Classification Medium: gas switch, liquid switch, solid switch Triggering mechanism: self-breakdown or externally triggered switches Charging mode: Statically charged or pulse charged switches No. of conducting channels: single channel or multi-channel switches Discharge property: volume discharge or surface discharge switches 3/44 High-voltage Pulsed Power Engineering, Fall 2018 Characteristics of typical switches A. Trigger pulse: a fast pulse supplied externally to initiate the action of switching, the nature of which may be voltage, laser beam or charged particle beam.
    [Show full text]
  • CHARGE-Series Instructions
    CHARGE-SERIES operating instructions REV216 Use for models CHARGE1000, CHARGE5000, CHARGE10000 DANGER do not use this unit unless you fully understand high -voltage and its hazards. DANGER A SERIOUS DEADLY SHOCK HAZARD WILL EXIST WHEN USING WITH HIGH ENERGY CAPACITORS ABOVE 50 J You can calculate joules by squaring the charging voltage, then multiplying by one half the capacitance in microfarads and dividing by 1 million. If over 50 J use extreme caution as improper contact can electrocute OR cause serious burns. PLEASE READ THE FOLLOWING VERY CAREFULLY Capacitive energy storage over 1000 joules MUST use for the high-voltage charge feed wire from the unit to the capacitors being SEVERAL FEET of a thin insulated preferably Teflon wire of a gauge that will disintegrate as a fuse between 100-500 amps. This wire should be sleeved into some polyethylene tubing that is available in a hardware store. You may even want to use several telescopic layers as this sleeving to provide a positive voltage rating and good mechanical rigidity. Note on knob Figure 1: Front Panel Controls CHARGE-SERIES ● rev216 © 2014 Information Unlimited www.amazing1.com 1 All rights reserved Figure 2: Back Panel CHARGE-SERIES ● rev216 © 2014 Information Unlimited www.amazing1.com 2 All rights reserved APPLICATIONS Electronic circuit charges up high energy banks of electrolytic, photo flash or other types storage capacitors from 200 to 30,000 V (depending on charger model) . Recommended capacities are between 100 to 10,000 µF. This equates out to many thousands of joules! Note the kinetic energy of a 30-06 is 750 J.
    [Show full text]
  • Arxiv:1701.07063V2 [Physics.Ins-Det] 23 Mar 2017 ACCEPTED by IEEE TRANSACTIONS on PLASMA SCIENCE, MARCH 2017 1
    This work has been accepted for publication by IEEE Transactions on Plasma Science. The published version of the paper will be available online at http://ieeexplore.ieee.org. It can be accessed by using the following Digital Object Identifier: 10.1109/TPS.2017.2686648. c 2017 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, including reprinting/republishing this material for advertising or promotional purposes, collecting new collected works for resale or redistribution to servers or lists, or reuse of any copyrighted component of this work in other works. arXiv:1701.07063v2 [physics.ins-det] 23 Mar 2017 ACCEPTED BY IEEE TRANSACTIONS ON PLASMA SCIENCE, MARCH 2017 1 Review of Inductive Pulsed Power Generators for Railguns Oliver Liebfried Abstract—This literature review addresses inductive pulsed the inductor. Therefore, a coil can be regarded as a pressure power generators and their major components. Different induc- vessel with the magnetic field B as a pressurized medium. tive storage designs like solenoids, toroids and force-balanced The corresponding pressure p is related by p = 1 B2 to the coils are briefly presented and their advantages and disadvan- 2µ tages are mentioned. Special emphasis is given to inductive circuit magnetic field B with the permeability µ. The energy density topologies which have been investigated in railgun research such of the inductor is directly linked to the magnetic field and as the XRAM, meat grinder or pulse transformer topologies. One therefore, its maximum depends on the tensile strength of the section deals with opening switches as they are indispensable for windings and the mechanical support.
    [Show full text]
  • Capillary Discharge XUV Radiation Source M
    Acta Polytechnica Vol. 49 No. 2–3/2009 Capillary Discharge XUV Radiation Source M. Nevrkla A device producing Z-pinching plasma as a source of XUV radiation is described. Here a ceramic capacitor bank pulse-charged up to 100 kV is discharged through a pre-ionized gas-filled ceramic tube 3.2 mm in diameter and 21 cm in length. The discharge current has ampli- tude of 20 kA and a rise-time of 65 ns. The apparatus will serve as experimental device for studying of capillary discharge plasma, for test- ing X-ray optics elements and for investigating the interaction of water-window radiation with biological samples. After optimization it will be able to produce 46.9 nm laser radiation with collision pumped Ne-like argon ions active medium. Keywords: Capillary discharge, Z-pinch, XUV, soft X-ray, Rogowski coil, pulsed power. 1 Introduction column by the Lorentz force FL of a magnetic field B of flowing current I – a Z-pinch. First, the current flows along the In the region of XUV (eXtended Ultra Violet) radiation, walls of the capillary. The flowing current creates a magnetic i.e. in the region of ~ (0.2–100) nm there are two significant field, which affects the charged particles of the plasma by sub-regions. The first is the water-window region (2.3–4.4) a radial force. This force compresses the particles like a nm. Radiation in this region is highly absorbed in carbon, but snowplow till the magnetic pressure is equilibrated by the not much absorbed in water, so it is useful for observing or- plasma pressure.
    [Show full text]
  • The Physics of Streamer Discharge Phenomena
    The physics of streamer discharge phenomena Sander Nijdam1, Jannis Teunissen2;3 and Ute Ebert1;2 1 Eindhoven University of Technology, Dept. Applied Physics P.O. Box 513, 5600 MB Eindhoven, The Netherlands 2 Centrum Wiskunde & Informatica (CWI), Amsterdam, The Netherlands 3 KU Leuven, Centre for Mathematical Plasma-astrophysics, Leuven, Belgium E-mail: [email protected] Abstract. In this review we describe a transient type of gas discharge which is commonly called a streamer discharge, as well as a few related phenomena in pulsed discharges. Streamers are propagating ionization fronts with self-organized field enhancement at their tips that can appear in gases at (or close to) atmospheric pressure. They are the precursors of other discharges like sparks and lightning, but they also occur in for example corona reactors or plasma jets which are used for a variety of plasma chemical purposes. When enough space is available, streamers can also form at much lower pressures, like in the case of sprite discharges high up in the atmosphere. We explain the structure and basic underlying physics of streamer discharges, and how they scale with gas density. We discuss the chemistry and applications of streamers, and describe their two main stages in detail: inception and propagation. We also look at some other topics, like interaction with flow and heat, related pulsed discharges, and electron runaway and high energy radiation. Finally, we discuss streamer simulations and diagnostics in quite some detail. This review is written with two purposes in mind: First, we describe recent results on the physics of streamer discharges, with a focus on the work performed in our groups.
    [Show full text]
  • Subnanosecond Pulsed-DC Ultra-High Gardient Photogun for Bright Relativistic Electron Bunches
    Subnanosecond pulsed-DC ultra-high gardient photogun for bright relativistic electron bunches Citation for published version (APA): Vyuga, D. A. (2006). Subnanosecond pulsed-DC ultra-high gardient photogun for bright relativistic electron bunches. Technische Universiteit Eindhoven. https://doi.org/10.6100/IR612076 DOI: 10.6100/IR612076 Document status and date: Published: 01/01/2006 Document Version: Publisher’s PDF, also known as Version of Record (includes final page, issue and volume numbers) Please check the document version of this publication: • A submitted manuscript is the version of the article upon submission and before peer-review. There can be important differences between the submitted version and the official published version of record. People interested in the research are advised to contact the author for the final version of the publication, or visit the DOI to the publisher's website. • The final author version and the galley proof are versions of the publication after peer review. • The final published version features the final layout of the paper including the volume, issue and page numbers. Link to publication General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal.
    [Show full text]
  • Simulations of the Propagation of Streamers in Electrical Discharges in a 5Mm Water Filled Gap
    Research Article Curr Trends Biomedical Eng & Biosci Volume 9 Issue 4 -september 2017 Copyright © All rights are reserved by Duaa A Uamran DOI: 10.19080/CTBEB.2017.09.555767 Simulations of the Propagation of Streamers in Electrical Discharges in a 5mm Water Filled Gap Thamir H Khalaf1 and Duaa A Uamran1,2* 1Department of Physics, College of Science, University of Baghdad, Iraq 2Department of Physics, College of Science, University of Kerbala, Iraq Submission: August 09, 2017; Published: September 27, 2017 *Corresponding author: Duaa A Uamran, Department of Physics, College of Science, University of Baghdad, Iraq, Email: Abstract This work is devoted to the modeling of streamer discharge, propagation in liquid dielectrics (water) gap using the bubble theory. This of the electrical discharge (streamer) propagating within adielectric liquid subjected to a divergent electric, using finite element method (in thetwo dielectric dimensions). liquid Solution gap and of indicates Laplace’s the equation minimum governs breakdown the voltage voltage andrequired electric for fielda 5mm distributions atmospheric within pressure the dielectricconfiguration, liquid the gap electrode as 22KV. configuration a point (pin) - plane configuration, the plasma channels were followed, step to step. That shows the streamer discharge bridges shown agreement with the streamer growth, according to the simulation development time. The initiated streamer grows and branches toward all elements that satisfy the required conditions. The electric potential and field distributions Keywords: Herbal; Phytochemical; Cytotoxic; Formulations Introduction and slow, heavy ions alter the propagation of discharge channels The breakdown of insulating liquids is not simple to explain [7-9]. and the mechanism responsible for the initiation of breakdown is still open to controversy.
    [Show full text]
  • Type Here the Title of Your Paper
    CIGRE-183 2019 CIGRE Canada Conference Montréal, Québec, September 16-19, 2019 The Research on the Key Equipment for 750kV Fixed Series Compensation in 3000m a.s.l. CHEN Yuanjun,ZHOU Qiwen,WANG Dechang,Gao Jian,Chen Wei, Zhang Daoxiong (1. NR Electric Co., Ltd., Nanjing 211102, China) SUMMARY The Qinghai 750kV fixed series compensation is officially put into operation in December 2018, it is located in the Qaidam area of China where the altitude is 3000m.In this paper, the high-altitude insulation calculation of the main equipment is carried out, and the power frequency withstand voltage, lightning impulse voltage, dry arc distance and creepage distance of each main equipment are proposed. Based on the project, we researched the key equipment such as spark gap and measurement system. According to the ANSYS simulation, the structure of the main electrode of the spark gap is optimized from ball-ball electrode to ball-plate electrode to make the self-trigger voltage be more stable. Considering the self-trigger voltage of the trigatron is up to 60kVpeak, the electrode structure of the trigatron is optimized to the structure with large curvature spherical design. The new trigatron has a better linearity and the maximum standard deviation is less than 0.6. In order to research the triggering characteristics, we completed the self-trigger test in the laboratory where the altitude is 0m, and fit the curve of the main gap air distance and the self-trigger voltage. Considering the altitude correction, we calculate the theoretical value of the main gap air distance according the self-trigger curve.
    [Show full text]
  • Electrical Breakdown in Gases
    High-voltage Pulsed Power Engineering, Fall 2018 Electrical Breakdown in Gases Fall, 2018 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University Gas breakdown: Paschen’s curves for breakdown voltages in various gases Friedrich Paschen discovered empirically in 1889. Left branch Right branch Paschen minimum F. Paschen, Wied. Ann. 37, 69 (1889)] 2/40 High-voltage Pulsed Power Engineering, Fall 2018 Generation of charged particles: electron impact ionization + Proton Electron + + Electric field Acceleration Electric field Slow electron Fast electron Acceleration Electric field Acceleration Ionization energy of hydrogen: 13.6 eV 3/40 High-voltage Pulsed Power Engineering, Fall 2018 Behavior of an electron before ionization collision Electrons moving in a gas under the action of an electric field are bound to make numerous collisions with the gas molecules. 4/40 High-voltage Pulsed Power Engineering, Fall 2018 Electron impact ionization Electron impact ionization + + Electrons with sufficient energy (> 10 eV) can remove an electron+ from an atom and produce one extra electron and an ion. → 2 5/40 High-voltage Pulsed Power Engineering, Fall 2018 Townsend mechanism: electron avalanche = Townsend ionization coefficient ( ) : electron multiplication : production of electrons per unit length along the electric field (ionization event per unit length) = = exp( ) = = 푒 푒 6/40 High-voltage Pulsed Power Engineering, Fall 2018 Townsend 1st ionization coefficient When an electron travels a distance equal to its free path in the direction of the field , it gains an energy of . For the electron to ionize, its gain in energy should be at least equal to the ionization potential of the gas: 1 1 = ≥ st ∝ The Townsend 1 ionization coefficient is equal to the number of free paths (= 1/ ) times the probability of a free path being more than the ionizing length , 1 1 exp exp ∝ − ∝ − = ⁄ − A and B must be experimentally⁄ determined for different gases.
    [Show full text]
  • ZEONICS SYSTECH.Cdr
    TM ZEONICS SYSTECH DEFENCE & AEROSPACE ENGINEERS (P) LTD. e of th ic e N rv a e t S io n n I ” “ 38 YEARS ESTABLISHED IN 1981 BANGALORE INDIA PRODUCT CATALOGUE “ADAR” No.3, 7th Cross, 10th Main, Maruthinagar, New Thippasandra Post, Bengaluru - 560075. Phone : +91-80-25241900, 25241901, 8050092601, 8050092602, 8050092603, 8050092604 Email : [email protected], [email protected] Website : www.zeonicssystech.com / www.systechcapacitors.com ZEONICS SYSTECH DEFENCE & AEROSPACE ENGINEERS (P) LTD. PRODUCT CATALOGUE Pioneers in Military Approved, Compact, Ultra Reliable High Voltage Components, Subassemblies and Systems IN SERVICE OF THE NATION SINCE 1981 “ADAR” No.3, 7th Cross, 10th Main, Maruthinagar, New Thippasandra Post, Bengaluru - 560075. Phone : +91-80-25241900, 25241901, 8050092601, 8050092602, 8050092603, 8050092604 Email : [email protected], [email protected] Website : www.zeonicssystech.com / www.systechcapacitors.com ZEONICS SYSTECH DEFENCE & AEROSPACE ENGINEERS (P) LTD. ABOUT US Zeonics Systech Defence & Aerospace Engineers Private Limited was established by Dr Z H Sholapurwala in the year of 1981 with the specific purpose of manufacturing High Voltage components and systems for the Government of India.We started as micro-scale unit mainly to design, develop and manufacture a wide variety of highly specialized equipment and components used for Defence, Atomic Energy and Strategic Applicaons. Our unit now has one of the most sophiscated R&D Labs in the country, with state of the art equipment and manufacturing facilies, cerfied by DSIR - Department of Scienfic and Industrial Research. The unit has now grown into macro-scale unit with the capability of handling all crical projects which are used for Radar, Missiles, Weapon systems and also food processing as well as medical technology.
    [Show full text]
  • Variable Capacitors in RF Circuits
    Source: Secrets of RF Circuit Design 1 CHAPTER Introduction to RF electronics Radio-frequency (RF) electronics differ from other electronics because the higher frequencies make some circuit operation a little hard to understand. Stray capacitance and stray inductance afflict these circuits. Stray capacitance is the capacitance that exists between conductors of the circuit, between conductors or components and ground, or between components. Stray inductance is the normal in- ductance of the conductors that connect components, as well as internal component inductances. These stray parameters are not usually important at dc and low ac frequencies, but as the frequency increases, they become a much larger proportion of the total. In some older very high frequency (VHF) TV tuners and VHF communi- cations receiver front ends, the stray capacitances were sufficiently large to tune the circuits, so no actual discrete tuning capacitors were needed. Also, skin effect exists at RF. The term skin effect refers to the fact that ac flows only on the outside portion of the conductor, while dc flows through the entire con- ductor. As frequency increases, skin effect produces a smaller zone of conduction and a correspondingly higher value of ac resistance compared with dc resistance. Another problem with RF circuits is that the signals find it easier to radiate both from the circuit and within the circuit. Thus, coupling effects between elements of the circuit, between the circuit and its environment, and from the environment to the circuit become a lot more critical at RF. Interference and other strange effects are found at RF that are missing in dc circuits and are negligible in most low- frequency ac circuits.
    [Show full text]