Design and Development of a Near Isotropic Printed Arc Antenna for Direction of Arrival (Doa) Applications
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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. -
Simulation and Measurements of VSWR for Microwave Communication Systems
Int. J. Communications, Network and System Sciences, 2012, 5, 767-773 http://dx.doi.org/10.4236/ijcns.2012.511080 Published Online November 2012 (http://www.SciRP.org/journal/ijcns) Simulation and Measurements of VSWR for Microwave Communication Systems Bexhet Kamo, Shkelzen Cakaj, Vladi Koliçi, Erida Mulla Faculty of Information Technology, Polytechnic University of Tirana, Tirana, Albania Email: [email protected], [email protected], [email protected], [email protected] Received September 5, 2012; revised October 11, 2012; accepted October 18, 2012 ABSTRACT Nowadays, microwave frequency systems, in many applications are used. Regardless of the application, all microwave communication systems are faced with transmission line matching problem, related to the load or impedance connected to them. The mismatching of microwave lines with the load connected to them generates reflected waves. Mismatching is identified by a parameter known as VSWR (Voltage Standing Wave Ratio). VSWR is a crucial parameter on deter- mining the efficiency of microwave systems. In medical application VSWR gets a specific importance. The presence of reflected waves can lead to the wrong measurement information, consequently a wrong diagnostic result interpretation applied to a specific patient. For this reason, specifically in medical applications, it is important to minimize the re- flected waves, or control the VSWR value with the high accuracy level. In this paper, the transmission line under dif- ferent matching conditions is simulated and experimented. Through simulation and experimental measurements, the VSWR for each case of connected line with the respective load is calculated and measured. Further elements either with impact or not on the VSWR value are identified. -
Ant-433-Heth
ANT-433-HETH Data Sheet by Product Description HE Series antennas are designed for direct PCB Outside 8.89 mm mounting. Thanks to the HE’s compact size, they Diameter (0.35") are ideal for internal concealment inside a product’s housing. The HE is also very low in cost, making it well suited to high-volume applications. HE Series Inside 6.4 mm Diameter (0.25") antennas have a very narrow bandwidth; thus, care in placement and layout is required. In addition, they are not as efficient as whip-style antennas, so they are generally better suited for use on the transmitter end where attenuation is often required Wire 15.24 mm Diameter (0.60") anyway for regulatory compliance. Use on both 1.3 mm 6.35 mm transmitter and receiver ends is recommended only (0.05") (0.25") in instances where a short range (less than 30% of whip style) is acceptable. 38.1 mm (1.50") Features • Very low cost • Compact for physical concealment Recommended Mounting • Precision-wound coil No ground plane or traces No electircal • Rugged phosphor-bronze construction under the antenna connection on this • Mounts directly to the PCB pad. For physical 38.10 mm support only. (1.50") Electrical Specifications 1.52 mm Center Frequency: 433MHz 7.62 mm (Ø0.060") Recom. Freq. Range: 418–458MHz (0.30") 3.81 mm Wavelength: ¼-wave 12.70 mm (0.50") (0.15") VSWR: ≤ 2.0 typical at center Peak Gain: 1.9dBi Impedance: 50-ohms Connection: Through-hole Oper. Temp. Range: –40°C to +80°C Electrical specifications and plots measured on a 7.62 x 19.05 Ground plane on cm (3.00" x 7.50") reference ground plane 50-ohm microstrip line bottom layer for counterpoise Ordering Information ANT-433-HETH (helical, through-hole) – 1 – Revised 5/16/16 Counterpoise Quarter-wave or monopole antennas require an associated ground plane counterpoise for proper operation. -
Slotted Line-SWR
Lab 2: Slotted Line and SWR Meter NAME NAME NAME Introduction: In this lab you will learn how to characterize and use a 50-ohm slotted line, crystal detector, and standing wave ratio (SWR) meter to measure an unknown impedance. The apparatus used is shown below. The slotted line is a (rigid) continuation of the coaxial transmission lines. Its characteristic impedance is 50 ohms. It has a thin slot in its outer conductor, cut along z. A probe rides within (but not touching) the slot to sample the transmission line voltage. The probe can be moved along z to sample the standing wave ratio at different locations. It can also be moved into and out of the slot by means of a micrometer in order to adjust the signal strength. The probe is connected to a crystal (diode) detector that converts the time-varying microwave voltage to a DC value with the help of a low speed modulation envelope (1 kHz) on the microwave signal. The DC voltage is measured using the SWR meter (HP 415D). 1 Using Slotted Line to Measure an Unknown Impedance: The magnitude of the line voltage as a function of position is: + −2 jβ l + j(θ −2β l ) jθ V ()z = V0 1− Γe = V0 1+ Γ e with Γ = Γ e and l the distance from the load towards the generator. Notice that the voltage magnitude has maxima and minima at different locations. + Vmax = V0 (1+ Γ ) when θ − 2β l = π + Vmin = V0 (1− Γ ) when θ − 2β l = 0 V 1+ Γ The SWR is defined as: SWR = max = . -
Voltage Standing Wave Ratio Measurement and Prediction
International Journal of Physical Sciences Vol. 4 (11), pp. 651-656, November, 2009 Available online at http://www.academicjournals.org/ijps ISSN 1992 - 1950 © 2009 Academic Journals Full Length Research Paper Voltage standing wave ratio measurement and prediction P. O. Otasowie* and E. A. Ogujor Department of Electrical/Electronic Engineering University of Benin, Benin City, Nigeria. Accepted 8 September, 2009 In this work, Voltage Standing Wave Ratio (VSWR) was measured in a Global System for Mobile communication base station (GSM) located in Evbotubu district of Benin City, Edo State, Nigeria. The measurement was carried out with the aid of the Anritsu site master instrument model S332C. This Anritsu site master instrument is capable of determining the voltage standing wave ratio in a transmission line. It was produced by Anritsu company, microwave measurements division 490 Jarvis drive Morgan hill United States of America. This instrument works in the frequency range of 25MHz to 4GHz. The result obtained from this Anritsu site master instrument model S332C shows that the base station have low voltage standing wave ratio meaning that signals were not reflected from the load to the generator. A model equation was developed to predict the VSWR values in the base station. The result of the comparism of the developed and measured values showed a mean deviation of 0.932 which indicates that the model can be used to accurately predict the voltage standing wave ratio in the base station. Key words: Voltage standing wave ratio, GSM base station, impedance matching, losses, reflection coefficient. INTRODUCTION Justification for the work amplitude in a transmission line is called the Voltage Standing Wave Ratio (VSWR). -
Ec6503 - Transmission Lines and Waveguides Transmission Lines and Waveguides Unit I - Transmission Line Theory 1
EC6503 - TRANSMISSION LINES AND WAVEGUIDES TRANSMISSION LINES AND WAVEGUIDES UNIT I - TRANSMISSION LINE THEORY 1. Define – Characteristic Impedance [M/J–2006, N/D–2006] Characteristic impedance is defined as the impedance of a transmission line measured at the sending end. It is given by 푍 푍0 = √ ⁄푌 where Z = R + jωL is the series impedance Y = G + jωC is the shunt admittance 2. State the line parameters of a transmission line. The line parameters of a transmission line are resistance, inductance, capacitance and conductance. Resistance (R) is defined as the loop resistance per unit length of the transmission line. Its unit is ohms/km. Inductance (L) is defined as the loop inductance per unit length of the transmission line. Its unit is Henries/km. Capacitance (C) is defined as the shunt capacitance per unit length between the two transmission lines. Its unit is Farad/km. Conductance (G) is defined as the shunt conductance per unit length between the two transmission lines. Its unit is mhos/km. 3. What are the secondary constants of a line? The secondary constants of a line are 푍 i. Characteristic impedance, 푍0 = √ ⁄푌 ii. Propagation constant, γ = α + jβ 4. Why the line parameters are called distributed elements? The line parameters R, L, C and G are distributed over the entire length of the transmission line. Hence they are called distributed parameters. They are also called primary constants. The infinite line, wavelength, velocity, propagation & Distortion line, the telephone cable 5. What is an infinite line? [M/J–2012, A/M–2004] An infinite line is a line where length is infinite. -
Antenna Theory and Matching
Antenna Theory and Matching Farrukh Inam Applications Engineer LPRF TI 1 Agenda • Antenna Basics • Antenna Parameters • Radio Range and Communication Link • Antenna Matching Example 2 What is an Antenna • Converts guided EM waves from a transmission line to spherical wave in free space or vice versa. • Matches the transmission line impedance to that of free space for maximum radiated power. • An important design consideration is matching the antenna to the transmission line (TL) and the RF source. The quality of match is specified in terms of VSWR or S11. • Standing waves are produced when RF power is not completely delivered to the antenna. In high power RF systems this might even cause arching or discharge in the transmission lines. • Resistive/dielectric losses are also undesirable as they decrease the efficiency of the antenna. 3 When does radiation occur • EM radiation occurs when charge is accelerated or decelerated (time-varying current element). • Stationary charge means zero current ⇒ no radiation. • If charge is moving with a uniform velocity ⇒ no radiation. • If charge is accelerated due to EMF or due to discontinuities, such as termination, bend, curvature ⇒ radiation occurs. 4 Commonly Used Antennas • PCB antennas – No extra cost – Size can be demanding at sub 433 MHz (but we have a good solution!) – Good performance at > 868 MHz • Whip antennas – Expensive solutions for high volume – Good performance – Hard to fit in many applications • Chip antennas – Medium cost – Good performance at 2.4 GHz – OK performance at 868-955 -
Radiation Hazard Analysis KVH Industries Carlsbad, CA
Radiation Hazard Analysis KVH Industries Carlsbad, CA This analysis predicts the radiation levels around a proposed earth station complex, comprised of one (reflector) type antennas. This report is developed in accordance with the prediction methods contained in OET Bulletin No. 65, Evaluating Compliance with FCC Guidelines for Human Exposure to Radio Frequency Electromagnetic Fields, Edition 97-01, pp 26-30. The maximum level of non-ionizing radiation to which employees may be exposed is limited to a power density level of 5 milliwatts per square centimeter (5 mW/cm2) averaged over any 6 minute period in a controlled environment and the maximum level of non-ionizing radiation to which the general public is exposed is limited to a power density level of 1 milliwatt per square centimeter (1 mW/cm2) averaged over any 30 minute period in a uncontrolled environment. Note that the worse-case radiation hazards exist along the beam axis. Under normal circumstances, it is highly unlikely that the antenna axis will be aligned with any occupied area since that would represent a blockage to the desired signals, thus rendering the link unusable. Earth Station Technical Parameter Table Antenna Actual Diameter 1 meters Antenna Surface Area 0.8 sq. meters Antenna Isotropic Gain 34.5 dBi Number of Identical Adjacent Antennas 1 Nominal Antenna Efficiency (ε) 67.50% Nominal Frequency 6.138 GHz Nominal Wavelength (λ) 0.0489 meters Maximum Transmit Power / Carrier 22.0 Watts Number of Carriers 1 Total Transmit Power 22.0 Watts W/G Loss from Transmitter to Feed 1.0 dB Total Feed Input Power 17.48 Watts Near Field Limit Rnf = D²/4λ =5.12 meters Far Field Limit Rff = 0.6 D²/λ = 12.28 meters Transition Region Rnf to Rff In the following sections, the power density in the above regions, as well as other critically important areas will be calculated and evaluated. -
Unit V Microwave Antennas and Measurements
UNIT V MICROWAVE ANTENNAS AND MEASUREMENTS Horn antenna and its types, micro strip and patch antennas. Network Analyzer, Measurement of VSWR, Frequency and Power, Noise, cavity Q, Impedance, Attenuation, Dielectric Constant and antenna gain. ------------------------------------------------------------------------------------------------------------------------------- DEFINITION: A conductor or group of conductors used either for radiating electromagnetic energy into space or for collecting it from space.or Is a structure which may be described as a metallic object, often a wire or a collection of wires through specific design capable of converting high frequency current into em wave and transmit it into free space at light velocity with high power (kW) besides receiving em wave from free space and convert it into high frequency current at much lower power (mW). Also known as transducer because it acts as coupling devices between microwave circuits and free space and vice versa. Electrical energy from the transmitter is converted into electromagnetic energy by the antenna and radiated into space. On the receiving end, electromagnetic energy is converted into electrical energy by the antenna and fed into the receiver. Basic operation of transmit and receive antennas. Transmission - radiates electromagnetic energy into space Reception - collects electromagnetic energy from space In two-way communication, the same antenna can be used for transmission and reception. Short wavelength produced by high frequency microwave, allows the usage -
Optical Antennas for Harvesting Solar Radiation Energy Waleed Tariq Sethi
Optical antennas for harvesting solar radiation energy Waleed Tariq Sethi To cite this version: Waleed Tariq Sethi. Optical antennas for harvesting solar radiation energy. Electronics. Université Rennes 1, 2018. English. NNT : 2018REN1S129. tel-02295386 HAL Id: tel-02295386 https://tel.archives-ouvertes.fr/tel-02295386 Submitted on 24 Sep 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THÈSE / UNIVERSITÉ DE RENNES 1 sous le sceau de l’Université Bretagne Loire pour le grade de DOCTEUR DE L’UNIVERSITÉ DE RENNES 1 Mention : Traitement de Signal et Télécommunications Ecole doctorale MathSTIC présentée par Waleed Tariq Sethi préparée à l’unité de recherche IETR (UMR 6164) (Institut d’Electronique et de Télécommunications de Rennes UFR Informatique et Electronique Thèse soutenue à Rennes le 16 Février 2018 Optical antennas devant le jury composé de : for harvesting solar Guillaume Ducournau IEMN Université Lille 1 / Polytech'Lille, France / radiation energy rapporteur Paola Russo Università Politecnica delle Marche Ancona, Italy / rapporteur Olivier -
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. -
ISOTROPIC RADIATOR in General, Isotropic Radiator Is a Hypothetical
Lecture 8 Antenna And Wave Propagation Isotropic Antenna ISOTROPIC RADIATOR In general, isotropic radiator is a hypothetical or fictitious radiator. The isotropic radiator is defined as a radiator which radiates energy in all directions uniformly. It is also called isotropic source. As it radiates uniformly in all directions. Basically isotropic radiator is a lossless ideal radiator or antenna. Generally all the practical antennas are compared with the characteristics of the isotropic radiator. The isotropic antenna or radiator is used as reference antenna. Practically all antennas show directional properties i.e. directivity property. That means none of the antennas radiate energy in all directions uniformly. Hence practically isotropic radiator cannot exist. Figure 1: Isotropic radiator Consider that an isotropic radiator is placed at the center of sphere of radius (r). Then all the power radiated by the isotropic radiator passes over the surface area of the sphere given by (4πr) assuming zero absorption of the power. Then at any point on the surface, the Poynting vector W gives the power radiated per unit area in any direction. But radiated power travels in the radial direction. Thus the magnitude of the Poynting vector W will be equal to radial component as the components in θ and ∅ directions are zero i.e. 푊휃=푊∅=0. Type equation here.Hence we can write, Technical College / communication Dept. 1 By: Ghufran M. Hatem Lecture 8 Antenna And Wave Propagation Isotropic Antenna |푊| = 푊푟 The total power radiated is given by, 2 푃푟푎푑 = ∮ 푊 푑푠 = ∮ 푊푟 푑푠 = 푊° ∮ 푑푠 = 4휋푟 푊° Where 푊° = 푃푎푣푔 = Average power density component ∮ 푑푠 = 4휋푟2=surface of sphere 푃 푃 = 푟푎푑 푎푣푔 4휋푟2 Where, P푟푎푑 = Total power radiated in watts r = Radius of sphere in meters 2 푃푎푣푔 =Radial component of average power density in W/m Electric Field of Isotropic Antenna The Point source is located at the origin point O, then the power density at the point Q is given as 푃푟푎푑 2 W 푃 = 4휋푟 … … … … … (1) 푎푣푔 m2 The power density is related to the electric and magnetic field 2 1 ∗ 퐸 1 2 푊 = 푅푒|퐸.