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ECE 5011: Antennas
ECE 5011: Antennas Course Description Electromagnetic radiation; fundamental antenna parameters; dipole, loops, patches, broadband and other antennas; array theory; ground plane effects; horn and reflector antennas; pattern synthesis; antenna measurements. Prior Course Number: ECE 711 Transcript Abbreviation: Antennas Grading Plan: Letter Grade Course Deliveries: Classroom Course Levels: Undergrad, Graduate Student Ranks: Junior, Senior, Masters, Doctoral Course Offerings: Spring Flex Scheduled Course: Never Course Frequency: Every Year Course Length: 14 Week Credits: 3.0 Repeatable: No Time Distribution: 3.0 hr Lec Expected out-of-class hours per week: 6.0 Graded Component: Lecture Credit by Examination: No Admission Condition: No Off Campus: Never Campus Locations: Columbus Prerequisites and Co-requisites: Prereq: 3010 (312), or Grad standing in Engineering, Biological Sciences, or Math and Physical Sciences. Exclusions: Not open to students with credit for 711. Cross-Listings: Course Rationale: Existing course. The course is required for this unit's degrees, majors, and/or minors: No The course is a GEC: No The course is an elective (for this or other units) or is a service course for other units: Yes Subject/CIP Code: 14.1001 Subsidy Level: Doctoral Course Programs Abbreviation Description CpE Computer Engineering EE Electrical Engineering Course Goals Teach students basic antenna parameters, including radiation resistance, input impedance, gain and directivity Expose students to antenna radiation properties, propagation (Friis transmission -
Antenna Gain Measurement Using Image Theory
i ANTENNA GAIN MEASUREMENT USING IMAGE THEORY SANDRAWARMAN A/L BALASUNDRAM A project report submitted in partial fulfillment of the requirement for the award of the degree Master of Electrical Engineering Faculty of Electrical and Electronic Engineering Universiti Tun Hussein Onn Malaysia JANUARY 2014 v ABSTRACT This report presents the measurement result of a passive horn antenna gain by only using metallic reflector and vector network analyzer, according to image theory. This method is an alternative way to conventional methods such as the three antennas method and the two antennas method. The gain values are calculated using a simple formula using the distance between the antenna and reflector, operating frequency, S- parameter and speed of light. The antenna is directed towards an absorber and then directed towards the reflector to obtain the S11 parameter using the vector network analyzer. The experiments are performed in three locations which are in the shielding room, anechoic chamber and open space with distances of 0.5m, 1m, 2m, 3m and 4m. The results calculated are compared and analyzed with the manufacture’s data. The calculated data have the best similarities with the manufacturer data at distance of 0.5m for the anechoic chamber with correlation coefficient of 0.93 and at a distance of 1m for the shield room and open space with correlation coefficient of 0.79 and 0.77 but distort at distances of 2m, 3m and 4m at all of the three places. This proves that the single antenna method using image theory needs less space, time and cost to perform it. -
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. -
Price List/Order Terms
PRICE LIST/ORDER TERMS 575 SE ASHLEY PLACE • GRANTS PASS, OR 97526 PHONE: (800) 736-6677 • FAX: (541) 471-6251 WIRELESS MADE SIMPLE www.linxtechnologies.com RF MODULES Prices Effective 02/04/04 Linx RF modules make it easy and cost-effective to add wireless capabilities to any product. That’s because Linx modules contain all the components necessary for the transmission of RF. Since no external components (except an antenna) are needed, the modules are easily applied, even by persons lacking previous RF design experience. This conserves valuable engineering resources and greatly reduces the product's time to market. Once in production, Linx RF modules improve yields, reduce placement costs, and eliminate the need for testing or adjustment. LC Series - Low-Cost Ultra-Compact RF Data Module The LC Series is ideally suited for volume use in OEM applications, such as remote control, security, identification, and periodic data transfer. Packaged in a compact SMD package, the LC modules utilize a highly optimized SAW architecture to achieve an unmatched blend of performance, size, efficiency and cost. Quantity TX RX-P* RX-S • Complete RF TX/RX solution <200 $5.60 $11.80 $10.90 • Ultra-compact size • Low cost in volume 200-999 $4.90 $10.65 $9.85 • High-performance SAW 1,000-4,999 $4.38 $9.50 $8.90 architecture >5000 Call Call Call • Direct serial interface • Low power consumption Part #’s Description • 5kbps maximum data rate TXM-***-LC LC Series Transmitter • >300ft. range RXM-***-LC-P LC Series Receiver Pinned SMD • No production tuning RXM-***-LC-S LC Series Receiver Compact SMD • No external components =315, 418, 433MHz 418MHz Standard RX-S *** required (except antenna) * = -P version not recommended for new designs • Wide temperature range RX-P LR Series - Long Range, Low Cost RF Data Module NEW The LR Series provides a 5-10 times range improvement over previous discrete and modular solutions and establishes a new benchmark for range performance and cost effectiveness within our product line. -
3794 Series Granger Wideband Conical Monopole Antennas
3794 Series Granger Wideband Conical Monopole Antennas ● 2-30 MHz Bandwidth permits Frequency change without antenna tuning ● Up to 25 KW average power rating ● 50 Ohm input provides 2.0:1 nominal VSWR without impedance transformers ● Single tower ● Short, medium, long-range communications General Description The Model 3794 series antenna is a vertically polarized, omnidirectional broadband antenna for transmitting or receiving applications. It is designed for high power area coverage. The 3794 Wideband Conical Monopole Antenna is an inverted cone- like structure with it’s apex pointing downwards. The array is supported by a 17 inch (431 mm) face steel guyed tower and consists of a number of evenly spaced radiator wires. The radiators spread out from the tower top to an outer guyed catenary then converge back down at the tower base. The antenna is fed at the apex of the cone through a 50 ohm coaxial connector. A ground screen is laid over the area below the antenna and consists of a radial pattern of wire laid on the ground with it’s centre at the apex of the antenna. The radiating elements of the array are prefabricated to facilitate installation. All radiators are manufactured from aluminum clad steel wire for maximum conductivity and corrosion resistance. The mechanical arrangement provides high strength while keeping both manufacturing and installation costs to a minimum. Application The 3794 Wideband Conical Monopole Antenna Series provides a cost effective solution for the vertical omnidirectional antenna if the reduced ground area offered by the 1794 Monocone is not required. The broad frequency range permits use of the optimum frequency for any distance. -
Directional Or Omnidirectional Antenna?
TECHNOTE No. 1 Joe Carr's Radio Tech-Notes Directional or Omnidirectional Antenna? Joseph J. Carr Universal Radio Research 6830 Americana Parkway Reynoldsburg, Ohio 43068 1 Directional or Omnidirectional Antenna? Joseph J. Carr Do you need a directional antenna or an omnidirectional antenna? That question is basic for amateur radio operators, shortwave listeners and scanner operators. The answer is simple: It depends. I would like to give you a simple rule for all situations, but that is not possible. With radio antennas, the "global solution" is rarely the correct solution for all users. In this paper you will find a discussion of the issues involved so that you can make an informed decision on the antenna type that meets most of your needs. But first, let's take a look at what we mean by "directional" and "omnidirectional." Antenna Patterns Radio antennas produce a three dimensional radiation pattern, but for purposes of this discussion we will consider only the azimuthal pattern. This pattern is as seen from a "bird's eye" view above the antenna. In the discussions below we will assume four different signals (A, B, C, D) arriving from different directions. In actual situations, of course, the signals will arrive from any direction, but we need to keep our discussion simplified. Omnidirectional Antennas. The omnidirectional antenna radiates or receives equally well in all directions. It is also called the "non-directional" antenna because it does not favor any particular direction. Figure 1 shows the pattern for an omnidirectional antenna, with the four cardinal signals. This type of pattern is commonly associated with verticals, ground planes and other antenna types in which the radiator element is vertical with respect to the Earth's surface. -
Antenna Characteristics
Antenna Characteristics Team Cygnus Shivam Garg Sheena Agarwal Prince Tiwari Gunjan Bansal Adikeshav C. Outline • Introduction • Characteristics • Methodology • Observations • Inferences Antenna • An antenna is a device designed to radiate and/or receive electromagnetic waves in a prescribed manner. A Yagi Uda antenna meant for home use Schematic diagram of a antenna The current distributions on the antennas produce the radiation. Usually, these current distributions are excited by transmission lines or waveguides. Types Of Antennas Wire Antennas Aperture antennas Micro strip Antennas Reflector antennas Antenna Basics Radiation Pattern • The distribution of radiated energy from an antenna over a surface of constant radius centered upon the antenna as a function of directional angles from antenna . Reciprocity Theorem • The reception pattern of an antenna is identical to its radiation (transmission) pattern. This is a general rule, known as the reciprocity theorem. • A complete radiation pattern is three dimensional function. • a pair of two-dimensional patterns are usually sufficient to characterize the directional properties of an antenna. • In most cases, the two radiation patterns are measured in planes which are perpendicular to each other. • A plane parallel to the electric field is chosen as one plane and the plane parallel to the magnetic field as the other. The two planes are called the E-plane and the H-plane, respectively. 15 E-plane (y-z or θ) and H-plane (x-y or φ) of a Dipole Antenna Gain • Some antennas are highly directional • Directional antenna is an antenna, which radiates (or receives) much more power in (or from) some directions than in (or from) others. -
Antennacraft Hookup
The Antennacraft Mini-State Directional, Rotating Antenna provides excellent reception of VHF/UHF TV channels in most viewing locations. The UV protective housing is made of impact-resistant filled co-polymer, making the exterior resistant to weathering. It features both AC and DC operation and is excellent for use on recreational vehicles 5/5(1). AntennaCraft 5MS RV Home Marine Amplified Antenna OMNIDIRECTIONAL UHF VHF. $ +$ shipping. Make Offer - AntennaCraft 5MS RV Home Marine Amplified Antenna OMNIDIRECTIONAL UHF VHF. Antennacraft HDTV Indoor Ultrathin Amplified Omniidirectional Antenna $ Product Reviews for AntennaCraft High Gain VHF/UHF TV Antenna Pre-Amp (10G) Product reviews help other customers decide which product to purchase, where the best deals are, and your get a sense of what to expect with the product.5/5(4). Manufacturers of TV antennas, amplifiers, and related electronic accessories. Includes product listing, support and contact information. Nov 16, · How to Hook Up a TV Antenna. This wikiHow teaches you how to select and set up an antenna for your TV. Determine your television's antenna connector type. Virtually every TV has an antenna input on the back or side; this is where you'll Views: M. Jun 01, · THE HAPPY SATELLITE NERD EPISODE The Antenna I use! It had 16 position settings it is amplified and works well. I can receive channels from . Related Manuals for Antennacraft Antenna AntennaCraft Mini State 5MS Manual. Amplified uhf/vhf indoor/outdoor tv antenna (8 pages) Antenna AntennaCraft HDX Quick Start Manual. Indoor/outdoor hdtv directional antenna (4 pages) Antenna AntennaCraft . Antennacraft Specification Sheet Model Number:5MS General Channels/Frequency:2 - 69 75 pHYPhysical Maximum Width (in) V ( w/ mast bracket) Turning Radius (in) 22 x 21 x 3 Antenna Performance Average Gain Over Reference Dipole (dB): Low Band: Half-Power Beamwidth. -
Coordinate Transformations-Based Antenna Elements Embedded in a Metamaterial Shell with Scanning Capabilities
electronics Article Coordinate Transformations-Based Antenna Elements Embedded in a Metamaterial Shell with Scanning Capabilities Dipankar Mitra 1,*, Sukrith Dev 2, Monica S. Allen 2, Jeffery W. Allen 2 and Benjamin D. Braaten 1,* 1 Department of Electrical and Computer Engineering, North Dakota State University, Fargo, ND 58105, USA 2 Air Force Research Laboratory, Munitions Directorate, Eglin Air Force Base, FL 32542, USA; [email protected] (S.D.); [email protected] (M.S.A.); [email protected] (J.W.A.) * Correspondence: [email protected] (D.M.); [email protected] (B.D.B.) Abstract: In this work transformation electromagnetics/optics (TE/TO) were employed to realize a non-homogeneous, anisotropic material-embedded beam-steerer using both a single antenna element and an antenna array without phase control circuitry. Initially, through theory and validation with numerical simulations it is shown that beam-steering can be achieved in an arbitrary direction by enclosing a single antenna element within the transformation media. Then, this was followed by an array with fixed voltages and equal phases enclosed by transformation media. This enclosed array was scanned, and the proposed theory was validated through numerical simulations. Further- more, through full-wave simulations it was shown that a horizontal dipole antenna embedded in a metamaterial can be designed such that the horizontal dipole performs identically to a vertical Citation: Mitra, D.; Dev, S.; Allen, dipole in free-space. Similarly, it was also shown that a material-embedded horizontal dipole array M.S.; Allen, J.W.; Braaten, B.D. -
2019 IEEE International Symposium on Antennas and Propagation and USNC-URSI National Radio Science Meeting
2019 IEEE International Symposium on Antennas and Propagation and USNC-URSI National Radio Science Meeting Final Program 7–12 July 2019 Hilton Atlanta Atlanta, Georgia, U.S.A. Conference at a Glance Saturday, July 6 14:00-16:00 Strategic Planning Committee 16:15-17:15 AP-S Meetings Committee 17:15-18:15 JMC Meeting (Closed Session) 18:15-21:30 JMC Meeting, Dinner and Presentations 19:15-21:15 IEEE AP-S Constitution and Bylaws Committee Meeting & Dinner Sunday, July 7 08:00-10:00 Past Presidents’ Breakfast 10:00-18:00 AdCom Meeting 19:30-22:00 Welcome Dessert Reception at the Georgia Aquarium Monday, July 8 07:00-08:00 Amateur Radio Operators Breakfast 08:00-11:40 Technical Sessions 09:00-18:00 Technical Tour - “An Engineer’s Eye View” of the Mercedes Benz Stadium 12:00-13:20 Transactions on Antennas and Propagation Editorial Board Lunch Meeting 13:20-17:00 Technical Sessions 17:00-18:00 URSI Commission A Business Meeting 17:00-18:00 URSI Commission B Business Meeting 17:00-18:00 URSI Commissions C/E (combined) Business Meeting Tuesday, July 9 07:00-08:00 AP Magazine Staff Meeting 07:00-08:00 APS 2020 Committee Meeting 07:00-08:00 Industrial Initiatives 07:00-08:00 Membership Committee Meeting 07:00-08:00 Student Design Contest (Set-Up - Closed to Others) 07:00-08:00 Technical Committee on Antenna Measurement 08:00-11:40 Student Paper Competition 08:00-11:40 Technical Sessions 08:00-09:30 Student Design Contest (Demo for Judges - Closed to Others) 08:30-14:00 Standards Committee Meeting 09:30-12:00 Student Design Contest (Demo for Public) -
An Improved Method to Determine the Antenna Factor Wout Joseph and Luc Martens, Member, IEEE
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Ghent University Academic Bibliography 252 IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 54, NO. 1, FEBRUARY 2005 An Improved Method to Determine the Antenna Factor Wout Joseph and Luc Martens, Member, IEEE Abstract—In this paper, we present an improved method to de- [5] and [6]. These methods make use of tabulated values of termine the antenna factor of three antennas. Instead of using a the maximum field strength for frequencies below 1000 MHz. reflecting ground plane we use absorbers. Destructive interference An advantage of our method is that it is applicable for both E- between the direct beam and the residual reflected beam from the absorbers is avoided by splitting the measured frequency range and H-field probes. For the calibration of loop antennas, two in bands and changing the distance between the two antennas de- methods are described in [7]. The first method is based on cal- pending on the frequency band. Furthermore, this method is ap- culation of the loop impedances. The second method is by gen- plicable for both E- and H-field probes. Our method has also the erating a well-defined standard magnetic field. The first method advantage of being low-cost: The method does not need to be per- cannot be used because the geometric shape of the split-shield formed in an anechoic chamber to obtain high accuracy. To take the residual reflections of the environment into account, we perform a loop probes is not simple. -
High-Performance Indoor VHF-UHF Antennas
High‐Performance Indoor VHF‐UHF Antennas: Technology Update Report 15 May 2010 (Revised 16 August, 2010) M. W. Cross, P.E. (Principal Investigator) Emanuel Merulla, M.S.E.E. Richard Formato, Ph.D. Prepared for: National Association of Broadcasters Science and Technology Department 1771 N Street NW Washington, DC 20036 Mr. Kelly Williams, Senior Director Prepared by: MegaWave Corporation 100 Jackson Road Devens, MA 01434 Contents: Section Title Page 1. Introduction and Summary of Findings……………………………………………..3 2. Specific Design Methods and Technologies Investigated…………………..7 2.1 Advanced Computational Methods…………………………………………………..7 2.2 Fragmented Antennas……………………………………………………………………..22 2.3 Non‐Foster Impedance Matching…………………………………………………….26 2.4 Active RF Noise Cancelling……………………………………………………………….35 2.5 Automatic Antenna Matching Systems……………………………………………37 2.6 Physically Reconfigurable Antenna Elements………………………………….58 2.7 Use of Metamaterials in Antenna Systems……………………………………..75 2.8 Electronic Band‐Gap and High Impedance Surfaces………………………..98 2.9 Fractal and Self‐Similar Antennas………………………………………………….104 2.10 Retrodirective Arrays…………………………………………………………………….112 3. Conclusions and Design Recommendations………………………………….128 2 1.0 Introduction and Summary of Findings In 1995 MegaWave Corporation, under an NAB sponsored project, developed a broadband VHF/UHF set‐top antenna using the continuously resistively loaded printed thin‐film bow‐tie shown in Figure 1‐1. It featured a low VSWR (< 3:1) and a constant dipole‐like azimuthal pattern across both the VHF and UHF television bands. Figure 1‐1: MegaWave 54‐806 MHz Set Top TV Antenna, 1995 In the 15 years since then much technical progress has been made in the area of broadband and low‐profile antenna design methods and actual designs.