Low-Profile Wideband Antennas Based on Tightly Coupled Dipole
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A Technical Assessment of Aperture-Coupled Antenna Technology
Running head: APERTURE-COUPLED ANTENNA TECHNOLOGY 1 A Technical Assessment of Aperture-coupled Antenna Technology Justin Obenchain A Senior Thesis submitted in partial fulfillment of the requirements for graduation in the Honors Program Liberty University Spring 2014 APERTURE-COUPLED ANTENNA TECHNOLOGY 2 Acceptance of Senior Honors Thesis This Senior Honors Thesis is accepted in partial fulfillment of the requirements for graduation from the Honors Program of Liberty University. ______________________________ Carl Pettiford, Ph.D. Thesis Chair ______________________________ Kyung K. Bae, Ph.D. Committee Member ______________________________ James Cook, Ph.D. Committee Member ______________________________ Brenda Ayres, Ph.D. Honors Director ______________________________ Date APERTURE-COUPLED ANTENNA TECHNOLOGY 3 Abstract Aperture coupling refers to a method of construction for patch antennas, which are specific types of microstrip antennas. These antennas are used in a variety of applications including cellular telephones, military radios, and other communications devices. The purpose of this thesis is to assess the benefits and drawbacks of aperture- coupled antenna technology. To develop a successful analysis of the patch antenna construction technique known as aperture coupling, this assessment begins by examining basic antenna theory and patch antenna design. After uncovering some of the fundamental principles that govern aperture-coupled antenna technology, a hypothesis is created and assessed based on the positive and negative aspects -
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. -
Chapter 5 the Microstrip Antenna
CHAPTER 5 THE MICROSTRIP ANTENNA 5.1 Introduction Applications that require low-profile, light weight, easily manufactured, inexpensive, conformable antennas often use some form of a microstrip radiator. The microstrip antenna (MSA) is a resonant structure that consists of a dielectric substrate sandwiched between a metallic conducting patch and a ground plane. The MSA is commonly excited using a microstrip edge feed or a coaxial probe. The canonical forms of the MSA are the rectangular and circular patch MSAs. The rectangular patch antenna in Figure 5.1 is fed using a microstrip edge feed and the circular patch antenna is fed using a coaxial probe. (a) (b) Coaxial Feed Microstrip Feed Figure 5.1. (a) A rectangular patch microstrip antenna fed with a microstrip edge feed. (b) A circular patch microstrip antenna fed with a coaxial probe feed. The patch shapes in Figure 5.1 are symmetric and their radiation is easy to model. However, application specific patch shapes are often used to optimize certain aspects of MSA performance. 154 The earliest work on the MSA was performed in the 1950s by Gutton and Baissinot in France and Deschamps in the United States. [1] Demand for low-profile antennas increased in the 1970s, and interest in the MSA was renewed. Notably, Munson obtained the original patent on the MSA, and Howell published the first experimental data involving circular and rectangular patch MSA characteristics. [1] Today the MSA is widely used in practice due to its low profile, light weight, cheap manufacturing costs, and potential conformability. [2] A number of methods are used to model the performance of the MSA. -
Path Loss and Shadowing 2017
Path-loss and Shadowing (Large-scale Fading) PROF. MICHAEL TSAI 2017/10/23 Friis Formula TX Antenna RX Antenna �"�"�- × � ⇒ � = � - 0 4��+ EIRP=�"�" % Power spatial density &' 1 × 4��+ 2 � � � � = � � - Antenna Aperture � 4��+ • Antenna Aperture=Effective Area �� • Isotropic Antenna’s effective area � ≐ �,��� �� • Isotropic Antenna’s Gain=1 �� • � = � �� � � � � �� � � � • Friis Formula becomes: � = � � � = � � � � ��� � ���� 3 � � � �� Friis Formula � = � � � � ��� � �� • is often referred as “Free-Space Path Loss” (FSPL) ��� � • Only valid when d is in the “far-field” of the transmitting antenna • Far-field: when � > ��, Fraunhofer distance ��� • � = , and it must satisfies � ≫ � and � ≫ � � � � � • D: Largest physical linear dimension of the antenna • �: Wavelength • We often choose a �� in the far-field region, and smaller than any practical distance used in the system � � • Then we have � � = � � � � � � � 4 Received Signal after Free-Space Path Loss phase difference due to propagation distance ���� � ������� − � � � = �� �N � ��� ���� � ��� � Free-Space Path Loss Carrier (sinusoid) Complex envelope 5 Example: Far-field Distance • Find the far-field distance of an antenna with maximum dimension of 1m and operating freQuency of 900 MHz (GSM 900) • Ans: • Largest dimension of antenna: D=1m • Operating FreQuency: f=900 MHz � �×��� • Wavelength: � = = = �. �� � ���×��� ��� � • � = = = �. �� (m) � � �.�� 6 Example: FSPL • If a transmitter produces 50 watts of power, express the transmit power in units of (a) dBm and (b) dBW. • If 50 watts -
Exp-1: Understand the Pathloss Prediction Formula
Exp-1: Understand the pathloss prediction formula. Aim To understand the pathloss prediction formula Objectives 1. Calculation of received signal strength as a function of distance of separation between transmitter and receiver. 2. To understand the impact of the following parameters on received signal strength. (a) Transmitter Power (b) Path loss exponent, (c) Carrier frequency, (d) Receiver antenna height, (e) Transmitter antenna height. 1 Theory for Experiment 1:-Understand the pathloss prediction formula. The design of a communication system involves selection of values for several parameters. One of the important parameter is the transmit power. Higher transmit power ensures large allowable separation distance between the transmitter (Tx) and receiver(Rx). Of course the loss in signal power per unit distance depends on the properties of the medium. In case of wireless communication on one hand it is desired to have a very large coverage (large allowable separation between Txand Rx) on the other hand it is also desired that co-channel interference be as low as possible.An understanding of the large scale propagation effects is very important for design of suitable communication system. In terrestrial mobile communication system, electro-magnetic wave propagation is affected by reflection, diffraction and scattering. These lead to dynamic variation of signal strength as a function of time, frequency, distance of separation, antenna height, antenna configuration, local scattering environment etc. Propagation models are necessary in order to predict the received signal strength for a given set of parameters as mentioned above. These models can be broadly considered under:- • Large scale Fading Model. • Small Scale Fading Model. -
Design and Analysis of Microstrip Patch Antenna Arrays
Design and Analysis of Microstrip Patch Antenna Arrays Ahmed Fatthi Alsager This thesis comprises 30 ECTS credits and is a compulsory part in the Master of Science with a Major in Electrical Engineering– Communication and Signal processing. Thesis No. 1/2011 Design and Analysis of Microstrip Patch Antenna Arrays Ahmed Fatthi Alsager, [email protected] Master thesis Subject Category: Electrical Engineering– Communication and Signal processing University College of Borås School of Engineering SE‐501 90 BORÅS Telephone +46 033 435 4640 Examiner: Samir Al‐mulla, Samir.al‐[email protected] Supervisor: Samir Al‐mulla Supervisor, address: University College of Borås SE‐501 90 BORÅS Date: 2011 January Keywords: Antenna, Microstrip Antenna, Array 2 To My Parents 3 ACKNOWLEGEMENTS I would like to express my sincere gratitude to the School of Engineering in the University of Borås for the effective contribution in carrying out this thesis. My deepest appreciation is due to my teacher and supervisor Dr. Samir Al-Mulla. I would like also to thank Mr. Tomas Södergren for the assistance and support he offered to me. I would like to mention the significant help I have got from: Holders Technology Cogra Pro AB Technical Research Institute of Sweden SP I am very grateful to them for supplying the materials, manufacturing the antennas, and testing them. My heartiest thanks and deepest appreciation is due to my parents, my wife, and my brothers and sisters for standing beside me, encouraging and supporting me all the time I have been working on this thesis. Thanks to all those who assisted me in all terms and helped me to bring out this work. -
Patch Antenna Array for RF Energy Harvesting Systems in 2.4 Ghz WLAN Frequency Band
Published by : International Journal of Engineering Research & Technology (IJERT) http://www.ijert.org ISSN: 2278-0181 Vol. 9 Issue 05, May-2020 Patch Antenna Array for RF Energy Harvesting Systems in 2.4 GHz WLAN Frequency Band Akash Kumar Gupta V. Praveen, V. Swetha Sri, Department of ECE CH. Nagavinay Kumar, B. Kishore Raghu Institute of Technology UG-Student, Department of ECE Raghu Visakhapatnam, India Institute of Technology Visakhapatnam, India Abstract—In present days, technology have been emerging harvesting topologies that operates low power devices. It has with significant importance mainly in wireless local area network. three stages receiving antenna, energy conversion into DC In this Energy harvesting is playing a key role. The RF Energy output, utilization of output of output in low power applications. harvesting is the collection of small amounts of ambient energy to power wireless devices, Especially, radio frequency (RF) energy II. RADIO FREQUENCY ENERGY HARVESTING has interesting key attributes that make it very attractive for low- power consumer electronics and wireless sensor networks (WSNs). FOR MICROSTRIP ANTENNA Commercial RF transmitting stations like Wi-Fi, or radar signals Microstrip patch antenna is a metallic patch which is may provide ambient RF energy. Throughout this paper, a specific fabricated on a dielectric substrate. The microstrip patch emphasis is on RFEH, as a green technology that is suitable for antenna is layered structure of ground plane as bottom layer solving power supply to WLAN node-related problems throughout and dielectric substrate as medium layer and radiating patch difficult environments or locations that cannot be reached. For RF harvesting RF signals are extracted using antennas.in this work to as top layer. -
RF Exposure Evaluation Declaration
MRT Technology (Taiwan) Co., Ltd Report No.: 2007TW0001-U3 Phone: +886-3-3288388 Report Version: V01 Web: www.mrt-cert.com Issue Date: 07-10-2020 RF Exposure Evaluation Declaration FCC ID: TE7AX3200 APPLICANT: TP-Link Technologies Co., Ltd. Application Type: Certification Product: AX3200 Tri-Band Wi-Fi 6 Router Model No.: Archer AX3200 Trademark: tp-link FCC Classification: Digital Transmission System (DTS) Unlicensed National Information Infrastructure (NII) Test Procedure(s): KDB 447498 D01v06 Test Date: July 04, 2020 Reviewed By: ( Paddy Chen ) Approved By: (Chenz Ker) The test results relate only to the samples tested. The test results shown in the test report are traceable to the national/international standards through the calibration of the equipment and evaluated measurement uncertainty herein. The test report shall not be reproduced except in full without the written approval of MRT Technology (Taiwan) Co., Ltd. Page Number: 1 of 7 Report No.: 2007TW0001-U3 Revision History Report No. Version Description Issue Date Note 2007TW0001-U3 Rev. 01 Initial report 07-10-2020 Valid Page Number: 2 of 7 Report No.: 2007TW0001-U3 1. PRODUCT INFORMATION 1.1. Equipment Description Product Name AX3200 Tri-Band Wi-Fi 6 Router Model No. Archer AX3200 Brand Name: tp-link Wi-Fi Specification: 802.11a/b/g/n/ac/ax 1.2. Description of Available Antennas Antenna Frequency TX Number of Max Beamforming CDD Directional Gain Type Band (MHz) Paths spatial Antenna Directional (dBi) streams Gain Gain For Power For PSD (dBi) (dBi) 2412 ~ 2462 2 1 3.52 6.53 3.52 6.53 Monopole 5150 ~ 5250 2 1 3.54 6.55 3.54 6.55 Antenna 5725 ~ 5850 4 1 3.20 9.22 3.20 9.22 Note: 1. -
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. -
Review of Recent Phased Arrays for Millimeter-Wave Wireless Communication
sensors Review Review of Recent Phased Arrays for Millimeter-Wave Wireless Communication Aqeel Hussain Naqvi and Sungjoon Lim * School of Electrical and Electronics Engineering, College of Engineering, Chung-Ang University, 221, Heukseok-Dong, Dongjak-Gu, Seoul 156-756, Korea; [email protected] * Correspondence: [email protected]; Tel.: +82-2-820-5827; Fax: +82-2-812-7431 Received: 27 July 2018; Accepted: 18 September 2018; Published: 21 September 2018 Abstract: Owing to the rapid growth in wireless data traffic, millimeter-wave (mm-wave) communications have shown tremendous promise and are considered an attractive technique in fifth-generation (5G) wireless communication systems. However, to design robust communication systems, it is important to understand the channel dynamics with respect to space and time at these frequencies. Millimeter-wave signals are highly susceptible to blocking, and they have communication limitations owing to their poor signal attenuation compared with microwave signals. Therefore, by employing highly directional antennas, co-channel interference to or from other systems can be alleviated using line-of-sight (LOS) propagation. Because of the ability to shape, switch, or scan the propagating beam, phased arrays play an important role in advanced wireless communication systems. Beam-switching, beam-scanning, and multibeam arrays can be realized at mm-wave frequencies using analog or digital system architectures. This review article presents state-of-the-art phased arrays for mm-wave mobile terminals (MSs) and base stations (BSs), with an emphasis on beamforming arrays. We also discuss challenges and strategies used to address unfavorable path loss and blockage issues related to mm-wave applications, which sets future directions. -
Design & Fabrication of Rectangular Microstrip Patch Antenna for WLAN
et International Journal on Emerging Technologies (Special Issue NCETST-2017) 8(1): 11-15(2017) (Published by Research Trend, Website: www.researchtrend.net ) ISSN No. (Print) : 0975-8364 ISSN No. (Online) : 2249-3255 Design & Fabrication of Rectangular Microstrip Patch Antenna for WLAN using Symmetrical slots Mudit Gupta, Pramod Kumar Morya and Satyajit Das Department of Electronics & Communication, Amrapali Group of Institute, Shiksha Nagar, Haldwani, (Uttarakhand), India ABSTRACT: This paper presents the symmetrical rectangular slotted microstrip patch antenna. The proposed antenna is simulated with the help of HFSS. The aim of this paper is to design and fabricate the Rectangular Microstrip Antenna and study the effect of antenna dimensions Length (L) , Width (W) and substrate parameters relative dielectric constant (εr), substrate thickness on power, vswr, return loss, impedance, admittance parameters. Low dielectric constant substrates are generally preferred for maximum radiation. Conducting patch can take any of the shape but rectangular and circular configurations are the most commonly used configuration. The other configurations are more complex to analyze and require heavy numerical computations. The length of the antenna is nearly half wavelength in the dielectric; it is a very critical parameter, which governs or control the resonant frequency of patch antenna. In the view of design, selection of patch width and length are the major parameters along with feed line depth. The desired microstrip patch antenna design is initially simulated by using HFSS simulator and patch antenna is realized as per design requirements. Keywords: Compact, Rectangular, WLAN, HFSS, Coaxial feed resonance frequency, gain are changed which may I. INTRODUCTION seriously degrade or upgrade the system performance. -
1.Effective Aperture of Antenna Directivity Bounding and Its
International Journal of Advanced Trends in Engineering, Science and Technology (IJATEST:2456-1126) Vol.3.Issue.5,September.2018 Effective Aperture of Antenna Directivity Bounding and Its Radiation Aperture MD. Javeed Ahammed 1, Dr. R.P. Singh2, Dr. M. Satya Sai Ram3 1.Research Scholar, ECE Department, Sri Satya Sai University of Technology and Medical Science, Sehore, Bhopal, Madhya Pradesh, India. E-mail: [email protected] 2. Vice- Chancellor, Sri Satya Sai University of Technology and Medical Science, Sehore, Bhopal, Madhya Pradesh, India. 3. HOD, ECE, Chalapathi Institute of Engineering and Technology, Chalapathi Nagar, Guntur, Andhra Pradesh, India. Abstract: In this paper, among the earliest type of antennas in production was aperture type. These antennas were rigid and consisted of a parabolic, paraboloidal, cylindrical, or spherical shape. A major limitation of this type of antenna stems from the fact they could only give one particular radiation pattern, and if one wanted to scan the signal from one point to another, then the whole structure had to be moved which meant the satellite had to be realigned. This major shortcoming led to the development of the more costly phased array technology and other technologies where beam scanning was exploited. The aperture is defined as the area, oriented perpendicular to the direction of an incoming radio wave, which would intercept the same amount of power from that wave as is produced by the antenna receiving it. At any point, a beam of radio waves has an irradiance or power flux density which is the amount of radio power passing through a unit area of one square meter.