A Guide to UHF Television Reception by Dr
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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. -
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. -
Automatic Measurement of Rf Signal Spatial Properties and Antenna Patterns
AUTOMATIC MEASUREMENT OF RF SIGNAL SPATIAL PROPERTIES AND ANTENNA PATTERNS Ing. Michal VAVRDA, Doctoral Degree Programme (2) Dept. of Radio Electronics, FEEC, BUT E-mail: [email protected] Ing. Ivo HERTL, Doctoral Degree Programme (2) Dept. of Radio Electronics, FEEC, BUT E-mail: [email protected] Supervised by: Dr. Zdeněk Nováček ABSTRACT Radio frequency signal measurement site is described in the presented paper. It enables direction setting by antenna rotator and signal frequency scanning and consequently measuring the parameters using a receiver. The site has two basic uses: measuring of antenna pattern; scanning and locating of RF signal. The site and its operation are made universally, the accuracy depends of rotator quality and parameter amount depends of receiver type. 1 INTRODUCTION The current development in wireless communication requires powerful technologies for antenna testing and signal measuring. Sophisticated devices measure plenty signal parameters, but there is not simply site, which combines the use of these devices with antenna rotator system for measuring the spatial properties of signal also. In this work the site for scanning, locating and measuring of radio frequency signal and measuring and testing the spatial properties of antennas is designed. It consists of antenna system, antenna rotor, receiver and control unit (rotator controller, PC and operating software). The antenna system and receiver type both has to be chosen depending on the measuring conditions (service, frequency band, bandwidth, polarisation, etc.). The locating accuracy is increased with antenna directivity but the necessary number of measuring directions is also increased. The antenna rotor quality determines the accuracy of location. -
Measurement Techniques and New Technologies for Satellite Monitoring
Report ITU-R SM.2424-0 (06/2018) Measurement techniques and new technologies for satellite monitoring SM Series Spectrum management ii Rep. ITU-R SM.2424-0 Foreword The role of the Radiocommunication Sector is to ensure the rational, equitable, efficient and economical use of the radio- frequency spectrum by all radiocommunication services, including satellite services, and carry out studies without limit of frequency range on the basis of which Recommendations are adopted. The regulatory and policy functions of the Radiocommunication Sector are performed by World and Regional Radiocommunication Conferences and Radiocommunication Assemblies supported by Study Groups. Policy on Intellectual Property Right (IPR) ITU-R policy on IPR is described in the Common Patent Policy for ITU-T/ITU-R/ISO/IEC referenced in Annex 1 of Resolution ITU-R 1. Forms to be used for the submission of patent statements and licensing declarations by patent holders are available from http://www.itu.int/ITU-R/go/patents/en where the Guidelines for Implementation of the Common Patent Policy for ITU-T/ITU-R/ISO/IEC and the ITU-R patent information database can also be found. Series of ITU-R Reports (Also available online at http://www.itu.int/publ/R-REP/en) Series Title BO Satellite delivery BR Recording for production, archival and play-out; film for television BS Broadcasting service (sound) BT Broadcasting service (television) F Fixed service M Mobile, radiodetermination, amateur and related satellite services P Radiowave propagation RA Radio astronomy RS Remote sensing systems S Fixed-satellite service SA Space applications and meteorology SF Frequency sharing and coordination between fixed-satellite and fixed service systems SM Spectrum management Note: This ITU-R Report was approved in English by the Study Group under the procedure detailed in Resolution ITU-R 1. -
ANTENNA ROTATOR DESIGN and CONTROL by MUHAMMAD RUSYDI BIN BUCHEK 14302 Dissertation Submitted in Partial Fulfilment of the Requ
ANTENNA ROTATOR DESIGN AND CONTROL by MUHAMMAD RUSYDI BIN BUCHEK 14302 Dissertation submitted in partial fulfilment of the requirement for the Bachelor of Engineering (Hons) (Electrical & Electronics Engineering) SEPTEMBER 2014 Universiti Teknologi PETRONAS Bandar Seri Iskandar 31750 Tronoh, Perak Darul Ridzuan CERTIFICATION OF APPROVAL Antenna Rotator Design and Control by Muhammad Rusydi bin Buchek 14302 A project dissertation submitted to the Electrical & Electronics Engineering Programme Universiti Teknologi PETRONAS in partial fulfilment of the requirement for the BACHELOR OF ENGINEERING (Hons) (ELECTRICAL & ELECTRONICS) Approved by, _____________________ (AP Dr Mohd Noh Karsiti) UNIVERSITI TEKNOLOGI PETRONAS TRONOH, PERAK September 2014 i CERTIFICATION OF ORIGINALITY This is to certify that I am responsible for the work submitted in this project, that the original work is my own except as specified in the references and acknowledgements, and that the original work contained herein have not been undertaken or done by unspecified sources or persons. ___________________________________________ MUHAMMAD RUSYDI BIN BUCHEK ii ABSTRACT This paper consists of design and development of rotator for antenna positioning according to the desired azimuth and elevation. The rotator is to have the capability to be manually controlled (press button switch) or software driven. It should incorporate safety stop switches as well as position and speed sensors in order to achieve smooth movement and correct stopping position. The basic principle needs to be studies are speed control using the microcontroller, exact angle of position movement, and stoppable motor can be done in time due to emergency cases. As larger load is applied to the device, the large inertia will need to be compensated to achieve a good dynamic. -
Performance Evaluation of Array Antennas
International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.1, Issue.2, pp-510-515 ISSN: 2249-6645 PERFORMANCE EVALUATION OF ARRAY ANTENNAS K.Ch.sri Kavya1 , Y.N.Sandhya Devi2 ,G.Sudheer Kumar2 , Narendra Neupane2 1(Associate Professor, Dept. of Electronics and Communication Engineering, KL University.) 2 PERFORMANCE(B.Tech Scholars, Dept. of EVALUATION Electronics and Communication OF Engineering, ARRAY KL University.) ANTENNAS ABSTRACT The purpose of the paper is to present a proper This paper will presents an optimization technique to reduce the side lobe level in the case normalization technique to obtain a low side lobe of linear array antennas. There several methods level and to avoid loss in main lobe directivity. are introduced for the side lobe reduction .But always the basic trade-off occur when II.METHODOLOGIES implementing amplitude weighting functions is that a trade between low side lobe levels and a loss A. Uniform Illumination method in main beam directivity always results . Here we Equal illumination at every element in an array made a comparison of three methods namely referred to as uniform illumination, results in uniform illumination method , Taylor line source directivity patterns with three distinct features. attenuation method and Taylor line source using Firstly, uniform illumination gives the highest redistribution method .The paper also presents aperture efficiency possible of 100% or 0 dB, for any different source distributions and their respective given aperture area. Secondly, the first side lobes for directivity patterns. a linear/rectangular aperture have peaks of approximately –13.1 dB relative to the main beam Keywords: Amplitude weighing, uniform peak; and the first side lobes for a circular aperture illumination, array antennas, normalization. -
Blockage and Directivity in 60 Ghz Wireless Personal Area Networks
1 Blockage and Directivity in 60 GHz Wireless Personal Area Networks: From Cross-Layer Model to Multihop MAC Design Sumit Singh, Student Member, IEEE, Federico Ziliotto, Upamanyu Madhow, Fellow, IEEE, Elizabeth M. Belding, Senior Member, IEEE, and Mark Rodwell, Fellow, IEEE Abstract—We present a cross-layer modeling and design ap- of multimedia content) between devices such as cameras, proach for multiGigabit indoor wireless personal area networks camcorders, personal computers and televisions, as well as (WPANs) utilizing the unlicensed millimeter (mm) wave spectrum real-time streaming of both compressed and uncompressed in the 60 GHz band. Our approach accounts for the following two characteristics that sharply distinguish mm wave networking high definition television (HDTV). This convergence of these from that at lower carrier frequencies. First, mm wave links are hardware and application trends has fueled intense efforts in inherently directional: directivity is required to overcome the both research and standardization for mm wave communica- higher path loss at smaller wavelengths, and it is feasible with tion [1]–[9]. However, the eventual success of these efforts compact, low-cost circuit board antenna arrays. Second, indoor depends on system designs that account for the fundamental mm wave links are highly susceptible to blockage because of the limited ability to diffract around obstacles such as the human differences between mm wave communication and existing body and furniture. We develop a diffraction-based model to wireless networks at lower carrier frequencies (e.g., from determine network link connectivity as a function of the locations 900 MHz to 5 GHz). In particular, the goal of this paper of stationary and moving obstacles. -
Of the Radiation Properties of the Antenna As a Function of Space Coordinates
LECTURE 4: Fundamental Antenna Parameters (Radiation pattern. Pattern beamwidths. Radiation intensity. Directivity. Gain. Antenna efficiency and radiation efficiency. Frequency bandwidth. Input impedance and radiation resistance. Antenna equivalent area. Relationship between directivity and area.) The antenna parameters describe the antenna performance with respect to space distribution of the radiated energy, power efficiency, matching to the feed circuitry, etc. Many of these parameters are interrelated. There are several parameters not described here, such as antenna temperature and noise characteristics. They will be discussed later in conjunction with radiowave propagation and system performance. 1. Radiation pattern The radiation pattern (RP) (or antenna pattern) is the representation of the radiation properties of the antenna as a function of space coordinates. The RP is measured in the far-field region, where the spatial (angular) distribution of the radiated power does not depend on the distance. One can measure and plot the field intensity, e.g. ∼ E ()θ ,ϕ , or the received power 2 E ()θϕ, 2 ∼ =η H ()θ ,ϕ η The trace of the spatial variation of the received/radiated power at a constant radius from the antenna is called the power pattern. The trace of the spatial variation of the electric (magnetic) field at a constant radius from the antenna is called the amplitude field pattern. Usually, the pattern describes the normalized field (power) values with respect to the maximum value. Note: The power pattern and the amplitude field pattern are the same when computed and plotted in dB. 1 The pattern can be a 3-D plot (both θ and ϕ vary), or a 2-D plot. -
LECTURE 4: Fundamental Antenna Parameters (Radiation Pattern
LECTURE 4: Fundamental Antenna Parameters (Radiation pattern. Pattern beamwidths. Radiation intensity. Directivity. Gain. Antenna efficiency and radiation efficiency. Frequency bandwidth. Input impedance and radiation resistance. Antenna effective area. Relationship between directivity and antenna effective area. Other antenna equivalent areas.) The antenna parameters describe the antenna performance with respect to space distribution of the radiated energy, power efficiency, matching to the feed circuitry, etc. Many of these parameters are interrelated. There are several parameters not described here, in particular, antenna temperature and noise characteristics. They are discussed later in conjunction with radio-wave propagation and system performance. 1. Radiation Pattern Definitions: The radiation pattern (RP) (or antenna pattern) is the representation of a radiation property of the antenna as a function of the angular coordinates. The trace of the angular variation of the received/radiated power at a constant radius from the antenna is called the power pattern. The trace of the angular variation of the magnitude of the electric (or magnetic) field at a constant radius from the antenna is called the amplitude field pattern. RPs are measured in the far-field region, where the angular distribution of the radiated power does not depend on the distance. We measure and plot either the field intensity, |E ( , ) |, or the power |E ( , ) |2 / = |H ( , ) |2 . Usually, the pattern describes the normalized field (or power) values with respect to the maximum value. Note: The power pattern and the amplitude field pattern are the same when computed and plotted in dB. The pattern can be a 3-D plot (both and vary), or a 2-D plot. -
ANTENNA INTRODUCTION / BASICS Rules of Thumb
ANTENNA INTRODUCTION / BASICS Rules of Thumb: 1. The Gain of an antenna with losses is given by: Where BW are the elev & az another is: 2 and N 4B0A 0 ' Efficiency beamwidths in degrees. G • Where For approximating an antenna pattern with: 2 A ' Physical aperture area ' X 0 8 G (1) A rectangle; X'41253,0 '0.7 ' BW BW typical 8 wavelength N 2 ' ' (2) An ellipsoid; X 52525,0typical 0.55 2. Gain of rectangular X-Band Aperture G = 1.4 LW Where: Length (L) and Width (W) are in cm 3. Gain of Circular X-Band Aperture 3 dB Beamwidth G = d20 Where: d = antenna diameter in cm 0 = aperture efficiency .5 power 4. Gain of an isotropic antenna radiating in a uniform spherical pattern is one (0 dB). .707 voltage 5. Antenna with a 20 degree beamwidth has a 20 dB gain. 6. 3 dB beamwidth is approximately equal to the angle from the peak of the power to Peak power Antenna the first null (see figure at right). to first null Radiation Pattern 708 7. Parabolic Antenna Beamwidth: BW ' d Where: BW = antenna beamwidth; 8 = wavelength; d = antenna diameter. The antenna equations which follow relate to Figure 1 as a typical antenna. In Figure 1, BWN is the azimuth beamwidth and BW2 is the elevation beamwidth. Beamwidth is normally measured at the half-power or -3 dB point of the main lobe unless otherwise specified. See Glossary. The gain or directivity of an antenna is the ratio of the radiation BWN BW2 intensity in a given direction to the radiation intensity averaged over Azimuth and Elevation Beamwidths all directions. -
Antenna Characteristics Page 1
Antenna Characteristics Page 1 Antenna Characteristics 1 Radiation Pattern The radiation pattern of an antenna is a graphical representation of the radiation properties of the antenna. Graphically, we surround the antenna by a sphere and evaluate the electric / magnetic fields (far field radiation fields) at a distance equal to the radius of the sphere. Figure 1: Radiated fields evaluated on an imaginary sphere surrounding a dipole [1] Usually we will focus on one field component (Eff or Hff ) radiated by the antenna. Usually we plot the dominant component of the E-field (e.g. Eθ for a dipole). This can be done by plotting the field component over all angles (θ; φ), yielding a 3D plot. For a dipole, this leads to the doughnut pattern in 3D because of the dependence of Eθ on sin θ. Figure 2: 3D radiation pattern of an ideal dipole [1] Usually, it is easier and more meaningful to plot a field in a number of principal planes in 2D in a polar plot. A plane containing the electric field vector is called the E-plane of the antenna. For a dipole, φ = constant is the E-plane; the constant can be any angle since there is no field variation with φ. The corresponding plot is a cross section of the doughnut: Similarly, a plane containing the H vector is called the H-plane. For the dipole, θ = 90◦ is appropriate: Prof. Sean Victor Hum Radio and Microwave Wireless Systems Antenna Characteristics Page 2 Figure 3: Radiation pattern of a dipole in the E-plane (polar form) [1] Figure 4: Radiation pattern of a dipole in the H-plane (polar form) [1] Since there is no variation of the radiated E/H fields with azimuth angle (φ), we call this type of antenna pattern omnidirectional 1.