Antenna System Guide, NIJ Guide 202-00
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RF & Microwave Components & Systems Catalog
There is a new leader and source for your RF & microwave systems and components … Spectrum Microwave. Combining the people, products and technologies from FSY Microwave, Salisbury Engineering, Q-Bit, Magnum Microwave, Radian Technologies and Amplifonix into a single organization poised to provide a wide range of microwave solutions. Spectrum Microwave offers a worldwide network of sales, distribution and manufacturing locations that gives us a responsive local presence in North America, Europe and Asia. We’ve assembled an experienced engineering team that will help you select the right standard product or design a custom solution for your specific application. Our expanded product line now ranges from sophisticated microwave systems and integrated assemblies to advanced control components to ceramic filters and antennas. This diverse array of products includes technologies to satisfy both low cost commercial and high performance military applications. 2 rf microwave& components and systems Index Page Introduction Product Selection Guide . .5-9 Design & Testing . .10-11 RF & Microwave Solutions Development . .12-13 • Lumped element and cavity filters Cascade . .14-15 Specwave.com . .16 • BTS filters and tower mounted amplifiers About Spectrum Control . .17 • Waveguide and tubular filters • Ceramic bandpass filters and duplexers Frequency Control Components • Patch antenna elements and assemblies Amplifiers . .19-20 Mixers . .21-22 Voltage Controlled Oscillators (VCOs) . .23 Dielectric Resonator Oscillators (DROs) . .24 Attenuators, Detectors & Switches . .25-26 Coaxial Ceramic Resonators . .27-28 Custom Microwave Filters Filter Topology Selection . .30-33 Filter Considerations . .34 Frequency Ranges . .35 Lumped Element Filters . .36-38 Cavity Filters . .39-41 Waveguide Filters . .42-43 Tubular Filters . .44-45 Suspended Substrate Filters . -
Frequency Finder
FREQUENCY FINDER USER MANUAL Version 22 November 2013 ManualFF.docx 1(175) 19 November 2013 Table of contents Chapter 1 Introduction Chapter 2 Installing 2.1 Operating systems 2.2 Installing with FileMaker Pro Advanced 2.3 Installing runtime version 2.4 Installing Google Earth 2.5 Downloading 2.6 Pop-up dialog boxes 2.7 Updating the database Chapter 3 Starting 3.1 Open 3.2 FileMaker Folders 3.3 FileMaker Toolbar 3.4 Start Page 3.4.1 Access to websites and documentation 3.4.2 Installing relevant programs 3.4.3 Regional Offices web sites 3.4.4 Navigation to data bases 3.4.5 Applications 3.4.6 Preset Region 3.4.7 Back-up and recovery 3.5 Closing Frequency Finder Chapter 4 Frequency assignment planning for VHF air/ground communication systems 4.1 VHF COM Home Page 4.2 VHF COM data base 4.2.1 Data fields in VHF Com list 4.2.2 Content of the data fields 4.2.3 Buttons on the toolbar 4.3 Finding frequency assignments 4.3.1 Find temporary (D) records 4.3.2 Query 4.3.3 Select Frequencies (Manually) 4.4 Export COM list 4.4.1 Initiate Export COM list 4.4.2 Toolbar for export COM list 4.4.3 File format for export COM list 4.4.4 Printing the COM list (exported) 4.5 Mapping ManualFF.docx 2(175) 19 November 2013 4.5.1 Initiate mapping 4.5.2 Mapping single station 4.5.3 Mapping found stations 4.6 Testing of frequency assignments and viewing the calculation results 4.6.1 Initiating the testing of frequency assignments 4.6.2 Start testing 4.6.3 Test results 4.6.4 Visualizing test results on the map 4.6.5 Summary calculations 4.6.6 Details co-frequency compatibility 4.6.7 Details adjacent frequency compatibility 4.7 Introducing of a new or modified frequency assignment 4.7.1 Initializing a new or modified frequency assignment 4.7.2 New/Mod frequency window toolbar 4.7.3 New frequency or modifying existing frequency 4.7.3.1 Station characteristics 4.7.3.2 Sector name 4.7.4. -
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. -
Improving Wireless LAN Antenna Gain and Coverage
APPLICATION NOTE Improving Wireless LAN Antenna Gain and Coverage antenna, which can help mitigate interference between floors. The only drawback is that the longer antenna may be somewhat less aesthetic. Mounting a dipole antenna on a conductive ground plane has a similar effect as using a longer antenna. The elevation pattern is flattened, creating higher gain around the perimeter of the doughnut. Additionally, the ground plane mounted antennas pattern is maximized downward slightly (if the antenna is mounted beneath a ceiling ground plane). This is an ideal elevation pattern for a ceiling mounted antenna in a multi-story building. The ground plane has the effect of minimizing gain below and especially above Most of the antennas provided with Wi-Fi the antenna. access points, or purchased separately, are simple dipole antennas with an omni- Wi-Fi antennas may be classified as ground directional pattern. Omni-directional means plane dependent and ground plane that the gain is the same in a 360º circle independent. The ground plane dependent around the axis of the antenna. antenna must be mounted on a conductive, flat ground plane which is several However, the elevation gain pattern is wavelengths long and wide in order to different. In cross section, the elevation provide the rated gain and impedance pattern is that of a doughnut, with the match. The ground plane independent antenna axis running through the center of antenna does not need to be mounted on a the doughnut. In the absence of a ground ground plane to provide the rated gain and plane, the gain of the dipole is a maximum impedance match. -
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. -
Radio Frequency Interference Analysis of Spectra from the Big Blade Antenna at the LWDA Site
Radio Frequency Interference Analysis of Spectra from the Big Blade Antenna at the LWDA Site Robert Duffin (GMU/NRL) and Paul S. Ray (NRL) March 23, 2007 Introduction The LWA analog receiver will be required to amplify and digitize RF signals over the full bandwidth of at least 20–80 MHz. This frequency range is populated with a number of strong sources of radio frequency interference (RFI), including several TV stations, HF broadcast transmissions, ham radio, and is adjacent to the FM band. Although filtering can be used to attenuate signals outside the band, the receiver must be designed with sufficient linearity and dynamic range to observe cosmic sources in the unoccupied regions between the, typically narrowband, RFI signals. A receiver of insufficient linearity will generate inter-modulation products at frequencies in the observing bands that will make it difficult or impossible to accomplish the science objectives. On the other hand, over-designing the receiver is undesirable because any excess cost or power usage will be multiplied by the 26,000 channels in the full design and may make the project unfeasible. Since the sky background is low level and broadband, the linearity requirements primarily depend on the RFI signals presented to the receiver. Consequently, a detailed study of the RFI environment at candidate LWA sites is essential. Often RFI surveys are done using antennas optimized for RFI detection such as discone antennas. However, such data are of limited usefulness for setting the receiver requirements because what is relevant is what signals are passed to the receiver when it is connected to the actual LWA antenna. -
Open Bradley Sherman Spring 2014.Pdf
THE PENNSYLVANIA STATE UNIVERSITY SCHREYER HONORS COLLEGE DEPARTMENT OF ELECTRICAL ENGINEERING HIGH FREQUENCY ANTENNA COUPLING STUDY BRADLEY SHERMAN SPRING 2014 A thesis submitted in partial fulfillment of the requirements for a baccalaureate degree in Electrical Engineering with honors in Electrical Engineering Reviewed and approved* by the following: James K. Breakall Professor of Electrical Engineering Thesis Supervisor John D. Mitchell Professor of Electrical Engineering Honors Adviser Keith A. Lysiak Senior Research Associate Thesis Reader * Signatures are on file in the Schreyer Honors College. i ABSTRACT The objective of this project was to develop a methodology to accurately predict antenna coupling through the use of numerical electromagnetic modeling. A high-frequency (HF) ionospheric sounder is being developed for HF propagation studies. This sounder requires high power transmissions on one antenna while receiving on another antenna. In order to minimize the coupling of high power energy back into the receiver, the transmit and receive antenna coupling must be minimized. The results of this research effort have shown that the current antenna setup can be improved by choosing a co-polarization setup and changing the frequency to 6.78 MHz. Rotating the receive antenna so that it runs parallel to the receive antenna decreases the antenna coupling by 8 dB. Typically the cross-polarization created by putting two antennas perpendicular to each other would decrease the antenna coupling dramatically, but that does not work if the feeds are along the perpendicular access. Attaining the ideal perpendicular setup is not possible in this case due to space restrictions. ii TABLE OF CONTENTS List of Figures ......................................................................................................................... -
Mfj-1046 Passive Preselector
MFJ-1046 Instruction Manual Passive Preselector MFJ-1046 PASSIVE PRESELECTOR Introduction The MFJ-1046 Passive Preselector is designed to reduce receive overload from strong out of band signals. It contains selective circuits that cover 1.6 to 33 MHz in six steps, providing the greatest selectivity on the lowest frequencies where overload is most common. The MFJ-1046 has two rear panel SO-239 connectors for RF connections and a bypass switch to take the unit in and out of the circuit. Installation Connect the MFJ-1046 Passive Preselector between your antenna and receiver as shown in Figure 1. The Radio connector goes directly to the receiver with a short well shielded lead; the Antenna connector goes to the antenna. Figure 1 WARNING: NEVER connect an amplifier or transmitter to the MFJ-1046 Passive Preselector. Failure to follow this warning may cause MFJ-1046 Passive Preselector or other equipment to be damaged. 1 MFJ-1046 Instruction Manual Passive Preselector Operation With the MFJ-1046 Passive Preselector properly connected, simply turn the Band switch to the desired band and adjust the Tune control for maximum signal level. With the Bypass switch depressed, the MFJ-1046 Passive Preselector becomes active. Adjust the Tune control for maximum signal level. The maximum loss on the desired amateur band is less than 5dB if the correct frequency range is selected. Note: Always use the highest frequency band range that covers the desired band for minimum loss. Typical frequency response is shown in Figure 2. A: Transmission Loss Figure 2 2 MFJ-1046 Instruction Manual Passive Preselector Technical Assistance If you have any problem with this unit first check the appropriate section of this manual. -
A Century of WWV
Volume 124, Article No. 124025 (2019) https://doi.org/10.6028/jres.124.025 Journal of Research of the National Institute of Standards and Technology A Century of WWV Glenn K. Nelson National Institute of Standards and Technology, Radio Station WWV, Fort Collins, CO 80524, USA [email protected] WWV was established as a radio station on October 1, 1919, with the issuance of the call letters by the U.S. Department of Commerce. This paper will observe the upcoming 100th anniversary of that event by exploring the events leading to the founding of WWV, the various early experiments and broadcasts, its official debut as a service of the National Bureau of Standards, and its role in frequency and time dissemination over the past century. Key words: broadcasting; frequency; radio; standards; time. Accepted: September 6, 2019 Published: September 24, 2019 https://doi.org/10.6028/jres.124.025 1. Introduction WWV is the high-frequency radio broadcast service that disseminates time and frequency information from the National Institute of Standards and Technology (NIST), part of the U.S. Department of Commerce. WWV has been performing this service since the early 1920s, and, in 2019, it is celebrating the 100th anniversary of the issuance of its call sign. 2. Radio Pioneers Other radio transmissions predate WWV by decades. Guglielmo Marconi and others were conducting radio research in the late 1890s, and in 1901, Marconi claimed to have received a message sent across the Atlantic Ocean, the letter “S” in telegraphic code [1]. Radio was called “wireless telegraphy” in those days and was, if not commonplace, viewed as an emerging technology. -
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.