Broadband Communications Using High Voltage Transmission Lines – a Review
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Analysis and Study the Performance of Coaxial Cable Passed on Different Dielectrics
International Journal of Applied Engineering Research ISSN 0973-4562 Volume 13, Number 3 (2018) pp. 1664-1669 © Research India Publications. http://www.ripublication.com Analysis and Study the Performance of Coaxial Cable Passed On Different Dielectrics Baydaa Hadi Saoudi Nursing Department, Technical Institute of Samawa, Iraq. Email:[email protected] Abstract Coaxial cable virtually keeps all the electromagnetic wave to the area inside it. Due to the mechanical properties, the In this research will discuss the more effective parameter is coaxial cable can be bent or twisted, also it can be strapped to the type of dielectric mediums (Polyimide, Polyethylene, and conductive supports without inducing unwanted currents in Teflon). the cable. The speed(S) of electromagnetic waves propagating This analysis of the performance related to dielectric mediums through a dielectric medium is given by: with respect to: Dielectric losses and its effect upon cable properties, dielectrics versus characteristic impedance, and the attenuation in the coaxial line for different dielectrics. The C: the velocity of light in a vacuum analysis depends on a simple mathematical model for coaxial cables to test the influence of the insulators (Dielectrics) µr: Magnetic relative permeability of dielectric medium performance. The simulation of this work is done using εr: Dielectric relative permittivity. Matlab/Simulink and presents the results according to the construction of the coaxial cable with its physical properties, The most common dielectric material is polyethylene, it has the types of losses in both the cable and the dielectric, and the good electrical properties, and it is cheap and flexible. role of dielectric in the propagation of electromagnetic waves. -
Wireless Power Transmission
International Journal of Scientific & Engineering Research, Volume 5, Issue 10, October-2014 125 ISSN 2229-5518 Wireless Power Transmission Mystica Augustine Michael Duke Final year student, Mechanical Engineering, CEG, Anna university, Chennai, Tamilnadu, India [email protected] ABSTRACT- The technology for wireless power transfer (WPT) is a varied and a complex process. The demand for electricity is much higher than the amount being produced. Generally, the power generated is transmitted through wires. To reduce transmission and distribution losses, researchers have drifted towards wireless energy transmission. The present paper discusses about the history, evolution, types, research and advantages of wireless power transmission. There are separate methods proposed for shorter and longer distance power transmission; Inductive coupling, Resonant inductive coupling and air ionization for short distances; Microwave and Laser transmission for longer distances. The pioneer of the field, Tesla attempted to create a powerful, wireless electric transmitter more than a century ago which has now seen an exponential growth. This paper as a whole illuminates all the efficient methods proposed for transmitting power without wires. —————————— —————————— INTRODUCTION Wireless power transfer involves the transmission of power from a power source to an electrical load without connectors, across an air gap. The basis of a wireless power system involves essentially two coils – a transmitter and receiver coil. The transmitter coil is energized by alternating current to generate a magnetic field, which in turn induces a current in the receiver coil (Ref 1). The basics of wireless power transfer involves the inductive transmission of energy from a transmitter to a receiver via an oscillating magnetic field. -
Transmission Line Characteristics
IOSR Journal of Electronics and Communication Engineering (IOSR-JECE) e-ISSN: 2278-2834, p- ISSN: 2278-8735. PP 67-77 www.iosrjournals.org Transmission Line Characteristics Nitha s.Unni1, Soumya A.M.2 1(Electronics and Communication Engineering, SNGE/ MGuniversity, India) 2(Electronics and Communication Engineering, SNGE/ MGuniversity, India) Abstract: A Transmission line is a device designed to guide electrical energy from one point to another. It is used, for example, to transfer the output rf energy of a transmitter to an antenna. This report provides detailed discussion on the transmission line characteristics. Math lab coding is used to plot the characteristics with respect to frequency and simulation is done using HFSS. Keywords - coupled line filters, micro strip transmission lines, personal area networks (pan), ultra wideband filter, uwb filters, ultra wide band communication systems. I. INTRODUCTION Transmission line is a device designed to guide electrical energy from one point to another. It is used, for example, to transfer the output rf energy of a transmitter to an antenna. This energy will not travel through normal electrical wire without great losses. Although the antenna can be connected directly to the transmitter, the antenna is usually located some distance away from the transmitter. On board ship, the transmitter is located inside a radio room and its associated antenna is mounted on a mast. A transmission line is used to connect the transmitter and the antenna The transmission line has a single purpose for both the transmitter and the antenna. This purpose is to transfer the energy output of the transmitter to the antenna with the least possible power loss. -
A Novel Single-Wire Power Transfer Method for Wireless Sensor Networks
energies Article A Novel Single-Wire Power Transfer Method for Wireless Sensor Networks Yang Li, Rui Wang * , Yu-Jie Zhai , Yao Li, Xin Ni, Jingnan Ma and Jiaming Liu Tianjin Key Laboratory of Advanced Electrical Engineering and Energy Technology, Tiangong University, Tianjin 300387, China; [email protected] (Y.L.); [email protected] (Y.-J.Z.); [email protected] (Y.L.); [email protected] (X.N.); [email protected] (J.M.); [email protected] (J.L.) * Correspondence: [email protected]; Tel.: +86-152-0222-1822 Received: 8 September 2020; Accepted: 1 October 2020; Published: 5 October 2020 Abstract: Wireless sensor networks (WSNs) have broad application prospects due to having the characteristics of low power, low cost, wide distribution and self-organization. At present, most the WSNs are battery powered, but batteries must be changed frequently in this method. If the changes are not on time, the energy of sensors will be insufficient, leading to node faults or even networks interruptions. In order to solve the problem of poor power supply reliability in WSNs, a novel power supply method, the single-wire power transfer method, is utilized in this paper. This method uses only one wire to connect source and load. According to the characteristics of WSNs, a single-wire power transfer system for WSNs was designed. The characteristics of directivity and multi-loads were analyzed by simulations and experiments to verify the feasibility of this method. The results show that the total efficiency of the multi-load system can reach more than 70% and there is no directivity. Additionally, the efficiencies are higher than wireless power transfer (WPT) systems under the same conductions. -
Introduction to Transmission Lines
INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012 http://www.empowermentresources.com/stop_cointelpro/electromagnetic_warfare.htm RF Design ¨ In RF circuits RF energy has to be transported ¤ Transmission lines ¤ Connectors ¨ As we transport energy energy gets lost ¤ Resistance of the wire à lossy cable ¤ Radiation (the energy radiates out of the wire à the wire is acting as an antenna We look at transmission lines and their characteristics Transmission Lines A transmission line connects a generator to a load – a two port network Transmission lines include (physical construction): • Two parallel wires • Coaxial cable • Microstrip line • Optical fiber • Waveguide (very high frequencies, very low loss, expensive) • etc. Types of Transmission Modes TEM (Transverse Electromagnetic): Electric and magnetic fields are orthogonal to one another, and both are orthogonal to direction of propagation Example of TEM Mode Electric Field E is radial Magnetic Field H is azimuthal Propagation is into the page Examples of Connectors Connectors include (physical construction): BNC UHF Type N Etc. Connectors and TLs must match! Transmission Line Effects Delayed by l/c At t = 0, and for f = 1 kHz , if: (1) l = 5 cm: (2) But if l = 20 km: Properties of Materials (constructive parameters) Remember: Homogenous medium is medium with constant properties ¨ Electric Permittivity ε (F/m) ¤ The higher it is, less E is induced, lower polarization ¤ For air: 8.85xE-12 F/m; ε = εo * εr ¨ Magnetic Permeability µ (H/m) Relative permittivity and permeability -
Recommendations for Transmitter Site Preparation
RECOMMENDATIONS FOR TRANSMITTER SITE PREPARATION IS04011 Original Issue.................... 01 July 1998 Issue 2 ..............................11 May 2001 Issue 3 ................... 22 September 2004 Nautel Limited 10089 Peggy's Cove Road, Hackett's Cove, NS, Canada B3Z 3J4 T.+1.902.823.2233 F.+1.902.823.3183 [email protected] U.S. customers please contact: Nautel Maine, Inc. 201 Target Industrial Circle, Bangor ME 04401 T.+1.207.947.8200 F.+1.207.947.3693 [email protected] e-mail: [email protected] www.nautel.com Copyright 2003 NAUTEL. All rights reserved. THE INFORMATION PRESENTED IN THIS DOCUMENT IS BELIEVED TO BE ACCURATE AND RELIABLE. IT IS INTENDED TO AUGMENT COMPETENT SITE ENGINEERING. IF THERE IS A CONFLICT BETWEEN THE RECOMMENDATIONS OF THIS DOCUMENT AND LOCAL ELECTRICAL CODES, THE REQUIREMENTS OF THE LOCAL ELECTRICAL CODE SHALL HAVE PRECEDENCE. Table of Contents 1 INTRODUCTION 1.1 Potential Threats 1.2 Advantages 2 LIGHTNING THREATS 2.1 Air Spark Gap 2.2 Ground Rods 2.2.1 Ground Rod Depth 2.3 Static Drain Choke 2.4 Static Drain Resistors 2.5 Series Capacitors 2.6 Single Point Ground 2.7 Diversion of Transients on RF Feed Coaxial Cable 2.8 Diversion/Suppression of Transients on AC Power Wiring 2.9 Shielded Isolation Transformer 3 ELECTROMAGNETIC SUSCEPTIBILITY 3.1 Shielded Building 3.2 Routing of RF Feed Coaxial Cable 3.3 Ferrites for Rejection of Common Mode Signals 3.4 EMI Filters 3.5 AC Power Sources Not Recommended for Use 4 HIGH VOLTAGE BREAKDOWN CONCERNS 4.1 RF Transmission Systems 4.2 High Voltage Feed Throughs 4.2.1 Insulator -
Lecture 2 - Transmission Line Theory Microwave Active Circuit Analysis and Design
Lecture 2 - Transmission Line Theory Microwave Active Circuit Analysis and Design Clive Poole and Izzat Darwazeh Academic Press Inc. © Poole-Darwazeh 2015 Lecture 2 - Transmission Line Theory Slide1 of 54 Intended Learning Outcomes I Knowledge I Understand that electrical energy travels at a finite speed in any medium, and the implications of this. I Understand the behaviour of lossy versus lossless transmission lines. I Understand power flows on a transmission line and the effect of discontinuities. I Skills I Be able to determine the location of a discontinuity in a transmission line using time domain refractometry. I Be able to apply the telegrapher’s equations in a design context. I Be able to calculate the reflection coefficient, standing wave ratio of a transmission line of known characteristic impedance with an arbitrary load. I Be able to calculate the input impedance of a transmission line of arbitrary physical length, and terminating impedance. I Be able to determine the impedance of a load given only the voltage standing wave ratio and the location of voltage maxima and minima on a line. © Poole-Darwazeh 2015 Lecture 2 - Transmission Line Theory Slide2 of 54 Table of Contents Propagation and reflection on a transmission line Sinusoidal steady state conditions : standing waves Primary line constants Derivation of the Characteristic Impedance Transmission lines with arbitrary terminations The effect of line losses Power Considerations © Poole-Darwazeh 2015 Lecture 2 - Transmission Line Theory Slide3 of 54 Propagation and reflection on a transmission line Let us consider a simple lossless transmission line, which could be simply a pair of parallel wires, terminated in a resistive load and connected to a DC source, such as a battery having a finite internal resistance, RS. -
Microwave Transmission Lines
Microwave Transmission Lines An Introduction to the Basics Debapratim Ghosh Department of Electrical Engineering Indian Institute of Technology Bombay Abstract This document presents an introduction to the basics of microwave transmission lines. It is important to understand the principles underlying the propagation and transmission of high-frequency signals, which are vital in areas such as communications circuit design as well as in high-frequency processor cores, and it is a well known fact that contemporary processors are clocked by frequencies as high as 3GHz! Designs at such high frequencies require careful consideration so as to minimize losses and to ensure maximum power transmission. This document starts by giving an insight into the basics of transmission lines and wave propagation theory. This is then followed by different transmission line technologies adopted in modern electronic systems for fabrication. Chapter 1 Introduction Microwaves are a part of the electromagnetic spectrum. Usually, waves with wavelengths ranging from as low as a few millimeters to almost a metre are classified as microwaves. Conventional definition for the microwave frequency range is from 300MHz 300GHz. A very important question is the reason behind − studying microwaves. What do these have to offer, and how are they advantageous? The answer is that most of modern electronic communication engineering make use of microwaves. Then again, what do mi- crowaves have that makes them suitable for use in comminication engineering? Let us consider for example, a mobile phone, an indispensable communication tool for all. Supposing that a mobile uses the GSM1800 band, i.e. it makes use of communication frequencies of about 1800MHz. -
A Communication Scheduling Scheme for UHV Transmission Line Construction and Security Mechanism Research Shuhao Zhang , Gangjun
2nd International Conference on Electronic & Mechanical Engineering and Information Technology (EMEIT-2012) A Communication Scheduling Scheme for UHV Transmission Line Construction and Security Mechanism Research Shuhao Zhang1,2,a, Gangjun Gong3,b, Xiangping Ni2,c and Yadi Zhang2,d 1 Wuhan University of Technology, 122 Luoshi Road, Wuhan, Hubei, China 430070 2 State Grid AC Engineering Construction Company, Beijing, China 100052 3School of Electronic and Electric Engineering, North China Electric Power Univ., Beijing, China 102206 [email protected], [email protected], [email protected], [email protected] Keywords: UHV transmission line, Chain-relay network, Broadband wireless, Security mechanism, System encryption Abstract: The constructions of the UHV transmission line are mostly located in remote place without public network coverage, and there are few effective com-munication means. This paper proposes a new scheme which adopts wireless Mesh Wi-Fi network and Digital Microwave Communication Technology based on COFDM, and analyzes their technical characteristics, networking modes and application respectively. Furthermore, this paper presents a merged scheme and the security mechanism which can provide the voice, data and video service for the constructions of the UHV transmission line. Introduction The State Grid Corporation of China is planning to build the UHV backbone grid called "three horizontal three longitudinal and two centers", which connects the large-scale energy bases and load centers, to achieve the purposes of the power from west to east and the power from north to east. While the construction of substations, the assembling of double-circuit steel pipe towers and stringing are long period, complex process and difficult construction, which adopt lots of new equipments for the first time. -
Transmission Lines
Chapter 2 Transmission Lines ECE 130a ZLocosbl + j Z sin bl ZLo+ j Z tan bl ZlZinaf-= o = Zo ZljZloLcosbb+ sin ZjZloL+ tan b Examples of Transmission Lines: (Chapter 2) Parallel Strip Line: metal conductors d w Coaxial Line: metal radius b metal radius a dielectric Parallel Wire Line: Air Line Dielectric Line D ε r conductor radius a Microstrip Line: w Dielectric Metal d There is a simple way to view the guided wave on a transmission line. z Iztaf, Vztaf, Iztaf, The potential difference (voltage) between the metal conductors with equal and opposite current flowing in them are circuit concepts, except they depend not only on time, but also on the distance z. So we describe the wave as voltage and current waves. itza , f + generator vtza , f load - Length L >>2πβ/ = λ Other guiding structures: 1. Waveguides -- consist of a single hollow metal tube of various cross- sectional geometry. An EM wave propagates longitudinally inside the hollow structure. The wave propagation in waveguides is not transverse (not TEM). That is, it has longitudinal field component(s). Transverse spatial depen- dence is fairly complicated. The propagation constant β of a waveguide wave is not equal to that of plane waves, and velocity of propagation thus is not the same as light. 2. Optical Fibers -- are used at optical frequencies, at infrared, and at visi- ble wavelengths. An optical fiber consists of a very thin (50-300 mm) dielectric circular cross section cylinder. The material is usually glass or plastic. Inner and outer portions have different dielectric constants (index of refraction), as shown below. -
Practical Antennas and Transmission Lines
Practical Antennas and Transmission Lines Tuesday, March 4, 14 1 This talk covers antenna properties, transmission line characteristics, radio cable connectors and adapters, and shows examples of different kinds of commercial and do-it-yourself antennas. Goals Antennas are the interface between guided waves (from a cable) and unguided waves (in space). ‣ To understand the various properties of antennas, so as to be able to choose the proper antenna for a particular application. ‣ Realize that not all kinds of cable are appropriate for use with wireless systems. ‣ Identify different kinds of cable connectors and understand when each kind is needed. 2 Tuesday, March 4, 14 2 Antennas are very important for the overall wireless system performance, and there are many different types. It is crucial to understand the effect of their features to optimize the performance of the wireless system. Transmission lines must couple the radio to the antenna introducing as little attenuation as possible. Transmission lines & antennas ‣ A transmission line is the device used to guide radio frequency (RF) energy from one point to another (for example a coaxial cable). ‣ An antenna is the structure associated with the region of transition from a guided wave to a free space wave, radiating RF energy. 3 Tuesday, March 4, 14 3 Think of antennas as an interface between the guided wave in the transmission line and the unguided wave in space. Antennas are passive devices. They cannot add power, they only focus it in a particular area. Bifilar transmission lines P ‣ Bifilar transmission lines are formed by two conducting wires separated by a dielectric. -
Radio-Frequency Interference (RFI) from Extra-High-Voltage (EHV)
Radio-Frequency Interference (RFI) From Extra-High- Voltage (EHV) Transmission Lines Patrick C. Crane 22 March 2010 1. Introduction The subject of radio-frequency interference (RFI) generated by high-voltage transmission lines has long been of both academic and commercial interest because of concerns about static on AM radio. Today audible noise is of greater concern because many states, counties, and municipalities have noise ordinances and transmission lines are designed to reduce audible noise, while people now expect static on AM radio (Chartier 2009). The subject is of interest today because of the proliferation around the world of low-frequency radio telescopes – including the Low Frequency Array (LOFAR), the Giant Metrewave Radio Telescope (GMRT), the Murchison Widefield Array (MWA), and the Long Wavelength Array (LWA), which is particular interest to the author. The present discussion will concern high-voltage alternating-current (HVAC) transmission lines; high-voltage direct-current (HVDC) transmission lines will be addressed in Appendix A. As described by Pakala and Chartier (1971) power lines are divided into two classes with respect to radio noise: (1) lines with voltages below 70 kV and (2) lines with voltages above 110 kV. Lines in the first class in general exhibit only gap-type discharges and lines in the second class principally exhibit corona discharge. Gap-type discharges are essentially a maintenance issue; corona discharges are a design issue. Extra-high-voltage (EHV) transmission lines have operating voltages of 345 kV or greater. The possibility of interference from such a transmission line first impinged significantly upon radio astronomy (in the United States, at least) in 1984 when the El Paso Electric Company proposed building a 345-kV transmission line from Red Hill, NM to Deming, NM which would run east along US60 to its junction with NM78 (now NM52) and then south along NM78.