Development of Earth Station Receiving Antenna and Digital Filter Design Analysis for C-Band VSAT
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Antenna Tuning for WCDMA RF Front End
Antenna tuning for WCDMA RF front end Reema Sidhwani School of Electrical Engineering Thesis submitted for examination for the degree of Master of Science in Technology. Espoo 20.11.2012 Thesis supervisor: Prof. Olav Tirkkonen Thesis instructor: MSc. Janne Peltonen Aalto University School of Electrical A’’ Engineering aalto university abstract of the school of electrical engineering master's thesis Author: Reema Sidhwani Title: Antenna tuning for WCDMA RF front end Date: 20.11.2012 Language: English Number of pages:6+64 Department of Radio Communications Professorship: Communication Theory Code: S-72 Supervisor: Prof. Olav Tirkkonen Instructor: MSc. Janne Peltonen Modern mobile handsets or so called Smart-phones are not just capable of commu- nicating over a wide range of radio frequencies and of supporting various wireless technologies. They also include a range of peripheral devices like camera, key- board, larger display, flashlight etc. The provision to support such a large feature set in a limited size, constraints the designers of RF front ends to make compro- mises in the design and placement of the antenna which deteriorates its perfor- mance. The surroundings of the antenna especially when it comes in contact with human body, adds to the degradation in its performance. The main reason for the degraded performance is the mismatch of impedance between the antenna and the radio transceiver which causes part of the transmitted power to be reflected back. The loss of power reduces the power amplifier efficiency and leads to shorter battery life. Moreover the reflected power increases the noise floor of the receiver and reduces its sensitivity. -
Multi Application Antenna for Wi-Fi, Wi-Max and Bluetooth for Better Radiation Efficiency
International Journal of Scientific Engineering and Applied Science (IJSEAS) - Volume-1, Issue-4, July 2015 ISSN: 2395-3470 ` www.ijseas.com Multi Application Antenna for Wi-Fi, Wi-max and Bluetooth for better radiation efficiency Hina D.Pal, J.Jenifer, Kavitha Balamurugan, M.E,Suntheravel, PG student, PG student, Associate Prof. Assistant Prof. KCG College of technology, KCG College of technology, KCG College of technology, KCG College of technology, Karapakkam, Karapakkam, Karapakkam, Karapakkam, Chennai-600097 Chennai-600097 Chennai-600097 Chennai-600097 ABSTRACT: Microstrip antenna is a printed type antenna This paper presents the radiation performance of rectangular consisting of a dielectric substrate sandwiched in patch antenna having a two slots. The design is used for between a ground plane and a patch. In this project three different frequencies 2.4, 5 and 7GHz . As a substrate Micro strip patch antenna technology is used for material Cu_clad is used. The simulated results for this different application for different frequencies antenna are obtained by varying the length and width of different materials are used for better efficiency. three dipoles.The results indicate that rectangular patch antenna with two slots offers a good antenna efficiency 41.576 at 2.45 GHz,51.958 at 5 GHz,46.810 at 7 GHz with the input feed 50 Ohm. Desired patch antenna design was simulated by ADS simulator program. ADS supports every step of the design process—schematic capture, layout, frequency-domain and time-domain circuit simulation, and electromagnetic field simulation, allowing the engineer to fully characterize and optimize an RF design without changing tools. -
Study of Radiation Patterns Using Modified Design of Yagi-Uda Antenna G
Adv. Eng. Tec. Appl. 5, No. 1, 7-9 (2016) 7 Advanced Engineering Technology and Application An International Journal http://dx.doi.org/10.18576/aeta/050102 Study of Radiation Patterns Using Modified Design of Yagi-Uda Antenna G. M. Thakur1, V. B. Sanap2,* and B. H. Pawar1. PI, Wireless section, DPW &Adl DG office, Pune (M.S.), India. Yeshwantrao Chavan College, Sillod Dist Aurangabad (M.S.), India. Received: 8 Aug. 2015, Revised: 20 Oct. 2015, Accepted: 28 Oct. 2015. Published online: 1 Jan. 2016. Abstract: Antenna is very important in wireless communication system. Among the most prevalent antennas, Yagi-Uda antenna is widely used. To improve the antenna gain and directivity, design of antenna is always important. In this paper, the Yagi Uda antenna is modified by adding two more reflectors instead of single and the gain, directivity & radiation pattern were studied. This antenna is designed to give better gain in one particular direction as well as somewhat reduced gain in other directions. The direction of "reduced gain" and gain at particular direction are not controllable in Yagi Uda. This paper provides a design which modifies radiation pattern of Yagi as per user requirement. The experiment is carried out at 157 MHz and all readings are taken for vertical polarization, with the help of Radio Communication Monitor. Keywords: Wireless communication, Yagi-Uda, Communication Service Monitor, Vertical polarization. 1 Introduction three) are used. The said antenna is designed with following set of parameters, Antennas have numerous advantages such as they can be Type:- Yagi-Uda antenna with additional two suitably used for wide range of applications such as reflectors wireless communications, satellite communications, pattern Input :- FM modulated signal of 157 MHz, with stability combining and antenna arrays. -
Chapter 22 Fundamentalfundamental Propertiesproperties Ofof Antennasantennas
ChapterChapter 22 FundamentalFundamental PropertiesProperties ofof AntennasAntennas ECE 5318/6352 Antenna Engineering Dr. Stuart Long 1 .. IEEEIEEE StandardsStandards . Definition of Terms for Antennas . IEEE Standard 145-1983 . IEEE Transactions on Antennas and Propagation Vol. AP-31, No. 6, Part II, Nov. 1983 2 ..RadiationRadiation PatternPattern (or(or AntennaAntenna Pattern)Pattern) “The spatial distribution of a quantity which characterizes the electromagnetic field generated by an antenna.” 3 ..DistributionDistribution cancan bebe aa . Mathematical function . Graphical representation . Collection of experimental data points 4 ..QuantityQuantity plottedplotted cancan bebe aa . Power flux density W [W/m²] . Radiation intensity U [W/sr] . Field strength E [V/m] . Directivity D 5 . GraphGraph cancan bebe . Polar or rectangular 6 . GraphGraph cancan bebe . Amplitude field |E| or power |E|² patterns (in linear scale) (in dB) 7 ..GraphGraph cancan bebe . 2-dimensional or 3-D most usually several 2-D “cuts” in principle planes 8 .. RadiationRadiation patternpattern cancan bebe . Isotropic Equal radiation in all directions (not physically realizable, but valuable for comparison purposes) . Directional Radiates (or receives) more effectively in some directions than in others . Omni-directional nondirectional in azimuth, directional in elevation 9 ..PrinciplePrinciple patternspatterns . E-plane . H-plane Plane defined by H-field and Plane defined by E-field and direction of maximum direction of maximum radiation radiation (usually coincide with principle planes of the coordinate system) 10 Coordinate System Fig. 2.1 Coordinate system for antenna analysis. 11 ..RadiationRadiation patternpattern lobeslobes . Major lobe (main beam) in direction of maximum radiation (may be more than one) . Minor lobe - any lobe but a major one . Side lobe - lobe adjacent to major one . -
Radiometry and the Friis Transmission Equation Joseph A
Radiometry and the Friis transmission equation Joseph A. Shaw Citation: Am. J. Phys. 81, 33 (2013); doi: 10.1119/1.4755780 View online: http://dx.doi.org/10.1119/1.4755780 View Table of Contents: http://ajp.aapt.org/resource/1/AJPIAS/v81/i1 Published by the American Association of Physics Teachers Related Articles The reciprocal relation of mutual inductance in a coupled circuit system Am. J. Phys. 80, 840 (2012) Teaching solar cell I-V characteristics using SPICE Am. J. Phys. 79, 1232 (2011) A digital oscilloscope setup for the measurement of a transistor’s characteristic curves Am. J. Phys. 78, 1425 (2010) A low cost, modular, and physiologically inspired electronic neuron Am. J. Phys. 78, 1297 (2010) Spreadsheet lock-in amplifier Am. J. Phys. 78, 1227 (2010) Additional information on Am. J. Phys. Journal Homepage: http://ajp.aapt.org/ Journal Information: http://ajp.aapt.org/about/about_the_journal Top downloads: http://ajp.aapt.org/most_downloaded Information for Authors: http://ajp.dickinson.edu/Contributors/contGenInfo.html Downloaded 07 Jan 2013 to 153.90.120.11. Redistribution subject to AAPT license or copyright; see http://ajp.aapt.org/authors/copyright_permission Radiometry and the Friis transmission equation Joseph A. Shaw Department of Electrical & Computer Engineering, Montana State University, Bozeman, Montana 59717 (Received 1 July 2011; accepted 13 September 2012) To more effectively tailor courses involving antennas, wireless communications, optics, and applied electromagnetics to a mixed audience of engineering and physics students, the Friis transmission equation—which quantifies the power received in a free-space communication link—is developed from principles of optical radiometry and scalar diffraction. -
Fig. 1 System Block Diagram
SSC13-II-2 300 Mbps Downlink Communications from 50kg Class Small Satellites Hirobumi Saito Japan Aerospace Exploration Agency (JAXA), Institute of Space and Astronautical Science (ISAS) Naohiko Iwakiri , Atsushi Tomiki, Takahide Mizuno, Hiromi Watanabe, Tomoya Fukami, Osamu Shigeta, Hitoshi Nunomura, Yasuaki Kanda , Kaname Kojima, Takahiro Shinke, and Toshiki Kumazawa Contents 1. Purpose : 320Mbps down link for small sat 2. Onboard segment: high effiency transmitter. small antenna 3. Ground segment : 3.8m S/X band antenna powerful receiver 4. Total simulation : SPW software + link calculation 5. EM test finished. FM maunfacturing now. 6. On-orbit demonstration : 2014 with 50kg sat. Limits of Small Satellites for Earth Observations • Mass Limit(<100kg), Power Limit (<100W) ー Telescope Resolution (5m vs. 0.5m) ー Down link Speed (10Mbps vs. 800Mbps) ・ What is the Bottleneck of Down Link Speed ? - Power ! Down link bit rate VS. satellite mass for low earth orbit. 1.0E+12 ) 1T bps TerraSAR-X Hodoyoshi #4 ( (2014) WorldView1 1.0E+09 EROS-B Formosat2 GeoEye-1 1G Orbview3Kompsat2 ALOS Orbview4 JERS1 EOS-PM1 Ikonos2 Radarsat1 TopSat QuickBird2 ERSEnvisat1 Lewis Landsat ADEOS Spot RazakSat-1 UK-DMC2 MOS 1B MOS 1A Terra IRS-1A,1B,1C UK-DMC1 EROS-A AS1000 AlSat Orbview2 TRMM 1.0E+06 データ伝送速度 1M EarlyBird MicroLabSat Cute-1.7 PRISM TOMS-EP Cute-I Down Link Bit Rate(bps) Link Down Bit 観測衛星の 1.0E+031K 1 10 100 1000 10000 Satellite衛星質量 Mass(kg) (kg) High Speed Down Link for Small Sat • Purpose of This Research: High-speed Down Link System with Low Power Consumption ―Goal 50kg Sat @600km orbit DC power <20W, 320Mbps Small Ground Antenna < 4m System block diagram of high-data-rate downlink. -
25. Antennas II
25. Antennas II Radiation patterns Beyond the Hertzian dipole - superposition Directivity and antenna gain More complicated antennas Impedance matching Reminder: Hertzian dipole The Hertzian dipole is a linear d << antenna which is much shorter than the free-space wavelength: V(t) Far field: jk0 r j t 00Id e ˆ Er,, t j sin 4 r Radiation resistance: 2 d 2 RZ rad 3 0 2 where Z 000 377 is the impedance of free space. R Radiation efficiency: rad (typically is small because d << ) RRrad Ohmic Radiation patterns Antennas do not radiate power equally in all directions. For a linear dipole, no power is radiated along the antenna’s axis ( = 0). 222 2 I 00Idsin 0 ˆ 330 30 Sr, 22 32 cr 0 300 60 We’ve seen this picture before… 270 90 Such polar plots of far-field power vs. angle 240 120 210 150 are known as ‘radiation patterns’. 180 Note that this picture is only a 2D slice of a 3D pattern. E-plane pattern: the 2D slice displaying the plane which contains the electric field vectors. H-plane pattern: the 2D slice displaying the plane which contains the magnetic field vectors. Radiation patterns – Hertzian dipole z y E-plane radiation pattern y x 3D cutaway view H-plane radiation pattern Beyond the Hertzian dipole: longer antennas All of the results we’ve derived so far apply only in the situation where the antenna is short, i.e., d << . That assumption allowed us to say that the current in the antenna was independent of position along the antenna, depending only on time: I(t) = I0 cos(t) no z dependence! For longer antennas, this is no longer true. -
WDP.2458.25.4.B.02 Linear Polarization Wifi Dual Bands Patch
SPECIFICATION PATENT PENDING Part No. : WDP.2458.25.4.B.02 Product Name : Wi-Fi Dual-band 2.4/5 GHz Embedded Ceramic Patch Antenna 6dBi+ at 2.4GHz 6dBi+ on 5 to 6 GHz Features : 25mm*25mm*4mm 2400MHz to 2500MHz/5150MHz to 5850MHz Pin Type Supports IEEE 802.11 Dual-band Wi-Fi systems Dual linear polarization Tuned for 70x70mm ground plane RoHS & REACH Compliant SPE-14-8-039/B/WY Page 1 of 14 1. Introduction This unique patent pending high gain, high efficiency embedded ceramic patch antenna is designed for professional Wi-Fi dual-band IEEE 802.11 applications. It is mounted via pin and double-sided adhesive. The passive patch offers stable high gain response from 4 dBi to 6dBi on the 2.4GHz band and from 5dBi to 8dBi on the 5 ~6 GHz band. Efficiency values are impressive also across the bands with on average 60%+. The WDP.25’s high gain, high efficiency performance is the perfect solution for directional dual-band WiFi application which need long range but which want to use small compact embedded antennas. The much higher gain and efficiency of the WDP.25 over smaller less efficient more omni-directional chip antennas (these typically have no more than 2dBi gain, 30% efficiencies) means it can deliver much longer range over a wide sector. Typical applications are • Access Points • Tablets • High definition high throughput video streaming routers • High data MIMO bandwidth routers • Automotive • Home and industrial in-wall WiFi automation • Drones/Quad-copters • UAV • Long range WiFi remote control applications The WDP patch antenna has two distinct linear polarizations, on the 2.4 and 5GHz bands, increasing isolation between bands. -
Design and Implementation of T-Shaped Planar Antenna for MIMO Applications
Computers, Materials & Continua Tech Science Press DOI:10.32604/cmc.2021.018793 Article Design and Implementation of T-Shaped Planar Antenna for MIMO Applications T. Prabhu1,* and S. Chenthur Pandian2 1Department of ECE, SNS College of Technology, Coimbatore, 641035, Tamil Nadu, India 2Department of EEE, SNS College of Technology, Coimbatore, 641035, Tamil Nadu, India *Corresponding Author: T. Prabhu. Email: [email protected] Received: 21 March 2021; Accepted: 26 April 2021 Abstract: This paper proposes, demonstrates, and describes a basic T-shaped Multi-Input and Multi-Output (MIMO) antenna with a resonant frequency of 3.1 to 10.6 GHz. Compared with the U-shaped antenna, the mutual coupling is minimized by using a T-shaped patch antenna. The T-shaped patch antenna shapes filter properties are tested to achieve separation over the 3.1 to 10.6 GHz frequency range. The parametric analysis, including width, duration, and spacing, is designed in the MIMO applications for good isolation. On the FR4 substratum, the configuration of MIMO is simulated. The appropriate dielec- tric material εr = 4.4 is introduced using this contribution and application array feature of the MIMO systems. In this paper, FR4 is used due to its high dielectric strength and low cost. For 3.1 to 10.6 GHz and 3SRR, T-shaped patch antennas are used in the field to increase bandwidth. The suggested T- shaped MIMO antenna is calculated according to the HFSS 13.0 program simulation performances. The antenna suggested is, therefore, a successful WLAN candidate. Keywords: Multi-input and multi-output; FR4 substratum; t-shaped patch antennas; ISM band; HFSS 13.0; WLAN 1 Introduction Multiple Input and Multiple Output (MIMO) devices can send and receive simultaneous signaling at the same power level and maximize high data rate demands in modern communication systems. -
Methods for Measuring Rf Radiation Properties of Small Antennas
Helsinki University of Technology Radio Laboratory Publications Teknillisen korkeakoulun Radiolaboratorion julkaisuja Espoo, October, 2001 REPORT S 250 METHODS FOR MEASURING RF RADIATION PROPERTIES OF SMALL ANTENNAS Clemens Icheln Dissertation for the degree of Doctor of Science in Technology to be presented with due permission for public examination and debate in Auditorium S4 at Helsinki University of Technology (Espoo, Finland) on the 16th of November 2001 at 12 o'clock noon. Helsinki University of Technology Department of Electrical and Communications Engineering Radio Laboratory Teknillinen korkeakoulu Sähkö- ja tietoliikennetekniikan osasto Radiolaboratorio Distribution: Helsinki University of Technology Radio Laboratory P.O. Box 3000 FIN-02015 HUT Tel. +358-9-451 2252 Fax. +358-9-451 2152 © Clemens Icheln and Helsinki University of Technology Radio Laboratory ISBN 951-22- 5666-5 ISSN 1456-3835 Otamedia Oy Espoo 2001 2 Preface The work on which this thesis is based was carried out at the Institute of Digital Communications / Radio Laboratory of Helsinki University of Technology. It has been mainly funded by TEKES and the Academy of Finland. I also received financial support from the Wihuri foundation, from HPY:n Tutkimussäätiö, from Tekniikan Edistämissäätiö, and from Nordisk Forskerutdanningsakademi. I would like to thank all these institutions, and the Radio Laboratory, for making this work possible for me. I am especially thankful for the many ideas and helpful guidance that I got from my supervisor professor Pertti Vainikainen during all my work. Of course I would also like to thank the staff of the Radio Laboratory, who provided a pleasant and inspiring working atmosphere, in which I got lots of help from my colleagues - let me mention especially Stina, Tommi, Jani, Lorenz, Eino and Lauri - without whom this work would not have been possible. -
A Review Paper on Microwave Transmission Using Reflector Antennas
International Journal of Scientific & Engineering Research Volume 8, Issue 10, October-2017 ISSN 2229-5518 251 A Review Paper on Microwave Transmission using Reflector Antennas Sandeep Kumar Singh [1],Sumi Kumari[2] Sr. Lecturer, Dept. of ECE, JBIT, Dehradun [1], Asst. Professor, Dept. of ECE, VGIET, Jaipur[2] [email protected][1] [email protected][2] Abstract: The conventional optimization problem of the beamed microwave energy transmission system is considered. The criterion of maximum efficiency of power intercept is parabolic function of distribution on the transmitting antenna. It is shown that under such a condition of amplitude distribution becomes more uniform than as the unconditional optimization. In this case, we can substantially increase the power radiated by the transmitting antenna losing the power intercept no more than 2%. Keywords: Parabolic Reflector Antenna, Radio Relay, Antenna Gain, Cassegrain Feed. I.INTRODUCTION limited to line of sight propagation; they cannot pass around hills or mountains as lower frequency radio waves can. Microwave radiation is generally defined as that electromagnetic radiation having wavelengths between radio waves and infrared III.ANTENNA radiation. Microwave radiation can be forced to travel in specially designed waveguides. Microwave radiation can be transmitted An antenna (or aerial) is an electrical device which converts through space or through the atmosphere in a microwave beam electric currents into radio waves, and vice versa. It is usually used from a microwave antenna and the microwave energy can be with a radio transmitter or radio receiver. In transmission, a radio collected with a microwave antenna. Microwave antennas are used transmitter applies an oscillating radio frequency electric current to for transmitting and receiving microwave radiation. -
Log Periodic Antenna
TE0321 - ANTENNA & PROPAGATION LABORATORY Laboratory Manual DEPARTMENT OF TELECOMMUNICATION ENGINEERING SRM UNIVERSITY S.R.M. NAGAR, KATTANKULATHUR – 603 203. FOR PRIVATE CIRCULATION ONLY ALL RIGHTS RESERVED SRM UNIVERSITY Faculty of Engineering & Technology Department of Telecommunication Engineering S. No CONTENTS Page no. Introduction – antenna & Propagation 1 6 Arranging the trainer & Performing functional Checks List of Experiments 1 12 Performance analysis of Half wave dipole antenna 2 15 Performance analysis of Folded dipole antenna 3 19 Performance analysis of Loop antenna 4 23 Performance analysis of Yagi ‐Uda antenna 5 38 Performance analysis of Helix antenna 6 41 Performance analysis of Slot antenna 7 44 Performance analysis of Log periodic antenna 8 47 Performance analysis of Parabolic antenna 9 51 Radio wave propagation path loss calculations ANTENNA & PROPAGATION LAB INTRODUCTION: Antennas are a fundamental component of modern communications systems. By Definition, an antenna acts as a transducer between a guided wave in a transmission line and an electromagnetic wave in free space. Antennas demonstrate a property known as reciprocity, that is an antenna will maintain the same characteristics regardless if it is transmitting or receiving. When a signal is fed into an antenna, the antenna will emit radiation distributed in space a certain way. A graphical representation of the relative distribution of the radiated power in space is called a radiation pattern. The following is a glossary of basic antenna concepts. Antenna An antenna is a device that transmits and/or receives electromagnetic waves. Electromagnetic waves are often referred to as radio waves. Most antennas are resonant devices, which operate efficiently over a relatively narrow frequency band.