LAAS/GBAS Ground Reference Antenna With Enhanced Mitigation of Ground Multipath

Similar documents
Near-field Computation and. Uncertainty Estimation using Basic. Cylindrical-Spherical Formulae

Antenna fundamentals: With answers to questions and problems (See also Chapter 9 in the textbook.)

Optimal Design of Smart Mobile Terminal Antennas for Wireless Communication and Computing Systems

Design of A Circularly Polarized E-shaped Patch Antenna with Enhanced Bandwidth for 2.4 GHz WLAN Applications

A New Method of VHF Antenna Gain Measurement Based on the Two-ray Interference Loss

Figure Geometry for Computing the Antenna Parameters.

Design of Microstrip Antenna for Wireless Local Area Network

ECE 6640 Digital Communications

Parameters of spinning AM reticles

Helical Antenna Performance in Wideband Communications

DESIGN AND PARAMETRIC EVALUATION OF RECTANGULAR MICROSTRIP PATCH ANTENNA FOR GSM APPLICATION

VTU NOTES QUESTION PAPERS NEWS VTU RESULTS FORUM BOOKSPAR ANDROID APP UNIT-4

DESIGN OF PRINTED DIPOLE ANTENNA AND ITS APPLICATIONS IN UMTS MOBILE COMMUNICATION NETWORKS

Optimal Eccentricity of a Low Permittivity Integrated Lens for a High-Gain Beam-Steering Antenna

CORNER TRUNCATED MICROSTRIP PATCH ANTENNA

ECE 6640 Digital Communications

Wireless Communication (Subject Code: 7EC3)

ScienceDirect. Simplified Generation of Electromagnetic Field within EMC Immunity Test Area

1 Performance and Cost

This article presents the

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

ONE-WAY RADAR EQUATION / RF PROPAGATION

where and are polynomials with real coefficients and of degrees m and n, respectively. Assume that and have no zero on axis.

NICKEL RELEASE REGULATIONS, EN 1811:2011 WHAT S NEW?

International Journal of Engineering Research-Online A Peer Reviewed International Journal Articles available online

Study and Design of Dual Frequency High Gain and Conformal Microstrip Patch Antenna

Minimizing Ringing and Crosstalk

UNCERTAINTY ESTIMATION OF SIZE-OF-SOURCE EFFECT MEASUREMENT FOR 650 NM RADIATION THERMOMETERS

Optimised Wireless Network Using Smart Mobile Terminal Antenna (SMTA) System

Available online at ScienceDirect. Procedia Engineering 100 (2015 )

Chamber Influence Estimation for Radiated Emission Testing in the Frequency Range of 1 GHz to 18 GHz

A Coplanar Waveguide Fed Asymmetric Ground Frequency Reconfigurable Antenna

Design and Characterization of Conformal Microstrip Antennas Integrated into 3D Orthogonal Woven Fabrics

Realistic Simulation of a Wireless Signal Propagation in an Urban Environment

Performance Analysis of Z-Source Inverter Considering Inductor Resistance

Sliding Mode Control for Half-Wave Zero Current Switching Quasi-Resonant Buck Converter

DESIGN OF DUAL BAND 1X2 MICROSTRIP PATCH ANTENNA ARRAY FOR GPS RECEIVERS

CHAPTER 2 DESIGN OF PLANAR MICROSTRIP ANTENNA ARRAYS AND MUTUAL COUPLING EFFECTS

Optic Cable Tracking and Positioning Method Based on Distributed Optical Fiber Vibration Sensing

Analysis of a Fractal Microstrip Patch Antenna

AMERICAN NATIONAL STANDARD

Low Profile MIMO Diversity Antenna with Multiple Feed

INVESTIGATION OF CLOSE-TO-WALL WIRELESS SENSOR DEPLOYMENT USING 2D FINITE-DIFFERENCE TIME-DOMAIN MODELLING. Y. Wu and I. J.

Feasibility of a triple mode, low SAR material coated antenna for mobile handsets

Study on Arc Envelope Grinding Process of Revolving Curved Surface Lingye Kong1, a,qiusheng Yan2,b,Yongliang Qiu1,c and Tengxiong Qiu1,d

Absolute calibration of null correctors using twin computer-generated holograms

Published in: International Journal of Material Forming. Document Version: Peer reviewed version

Diagnosis method of radiated emission from battery management system for electric vehicle

An Efficient Control Approach for DC-DC Buck-Boost Converter

Research on the Propagation of Extremely Low Frequency Electromagnetic Wave in Shallow Sea Area

WIRELESS SENSORS EMBEDDED IN CONCRETE

Investigation. Name: a About how long would the threaded rod need to be if the jack is to be stored with

Design of Broad-Beam Microstrip Reflectarray

Statement of Works Data Template Version: 4.0 Date:

Radiation resistance

Near-field emission prediction of CESAME

MIMO OTA Testing in Small Multi-Probe Anechoic Chamber Setups Llorente, Ines Carton; Fan, Wei; Pedersen, Gert F.

The Periodic Ambiguity Function Its Validity and Value

FREQUENCY RECONFIGURABLE MICROSTRIP SLOT ANTENNA LOADED WITH VARACTOR DIODE

ERROR ESTIMATIONS IN CYLINDRICAL NEAR FIELD SYSTEM FOR LARGE RADAR ANTENNAS

Mitigation of GPS Multipath Using Polarization and Spatial Diversities

N2-1. The Voltage Source. V = ε ri. The Current Source

SOIL MOISTURE MONITORIZATION USING GNSS REFLECTED SIGNALS

Week 5. Lecture Quiz 1. Forces of Friction, cont. Forces of Friction. Forces of Friction, final. Static Friction

Electrical characterization of thin film ferroelectric capacitors

Compact CP Feed Broadband Microstrip Patch Antenna for Wireless Applications

Investigate Surface Area of Three-Dimensional Objects

Design of an LLC Resonant Converter Using Genetic Algorithm

Hexagonal Shaped Microstrip Patch Antenna for Satellite and Military Applications

cos s Presentation Layout HIGH ACCURACY REAL-TIME DAM MONITORING USING LOW COST GPS EQUIPMENT

Key Laboratory of Earthquake Engineering and Engineering Vibration, China Earthquake Administration, China

June 2012 Volume 1, Issue 3 Article #07

Figure 1-1 Sample Antenna Pattern

Analysis of the Radiation Resistance and Gain of Full-Wave Dipole Antenna for Different Feeding Design

Synopsis of Technical Report: Designing and Specifying Aspheres for Manufacturability By Jay Kumler

Noise Attenuation Due to Vegetation

Analysis of the optimized low-nonlinearity lateral effect sensing detector

Low-Complexity Time-Domain SNR Estimation for OFDM Systems

Communication Antenas for UAVs

OTA MEASUREMENTS OF SMALL RADIO TERMINALS BY A SPHEROIDAL COUPLER

Design of FIR Filter using Filter Response Masking Technique

For most of us, discoveries in the art are

Instant Active Positioning with One LEO Satellite

Journal of Applied Science and Agriculture

Surface Areas of Cylinders ACTIVITY: Finding Surface Area. ACTIVITY: Finding Area. How can you find the surface area of. a cylinder?

LAAS Reference Antennas - Circular Polarization Mitigates Multipath Effects

OPTIMUM MEDIUM ACCESS TECHNIQUE FOR NEXT GENERATION WIRELESS SYSTEMS

Experiments with the HoloEye LCD spatial light modulator

Introduction to Antenna principles

Controller Design of Discrete Systems by Order Reduction Technique Employing Differential Evolution Optimization Algorithm

ISSN: [Reddy & Rao* et al., 5(12): December, 2016] Impact Factor: 4.116

S11 PHY114 Problem Set 8

On Solving TM 0n Modal Excitation in a Ka-Band Overmoded Circular Waveguide by the Conservation of Complex Power Technique

Spectrum Sharing between Public Safety and Commercial Users in 4G-LTE

Highly Selective Dual-Mode Microstrip Bandpass Filters Using Triangular Patch Resonators

GAMMA SHAPED MONOPOLE PATCH ANTENNA FOR TABLET PC

ECEN326: Electronic Circuits Fall 2017

An Ultra Low Power Segmented Digital-to-Analog Converter

Optimization of the law of variation of shunt regulator impedance for Proximity Contactless Smart Card Applications to reduce the loading effect.

Microwave Finite Element Modeling Applications to Coupled Electromagnetic-Thermal Problems and Characterization of Dielectric Materials

Transcription:

LAAS/BAS ound Refeence Antenna With Enhanced Mitigation of ound Multipath Alfed R Lopez, BAE Systems BIORAPHY Alfed R Lopez is a Life Fellow of the IEEE He is a Hazeltine Fellow and Engineeing Fellow with BAE Systems, eenlawn, NY He stated his caee at Wheele Laboatoies in 958 as an antenna design specialist He has made contibutions to the theoy and pactice of electonic scanned antennas Fom 969 to 99 he was involved with the development of the Micowave Landing System He has published extensively in IEEE publications, has been issued 6 US Patents, and has eceived seveal IEEE and BAE Systems awads He is the invento of the ARL-9 ound Refeence Antenna ABSTRACT The concept fo the ARL-9 LAAS/BAS gound efeence antenna was fist descibed at the ION 2 National Technical Meeting This antenna has the following featues: One-pot cicula-polaization L-L2-L5 coveage of the uppe hemisphee Shap antenna patten cutoff on the hoizon fo mitigation of gound multipath at low elevation 3 db sidelobes in the lowe hemisphee fo mitigation of gound multipath at highe elevation Vey high quality caie delay (antenna phase cente) and code (goup) delay chaacteistics Cicula polaization at low elevation fo mitigation of lateal multipath This antenna has been unde development since 999, and is now enteing the initial phase of field deployment The pototype ARL-9 antenna was built unde contact to the FAA Afte successful testing by the FAA, in Decembe of 25, 7 additional antennas wee built and tested Ten additional antennas ae cuently being built This pape eviews the gound multipath issue and descibes a means fo enhanced mitigation of the gound multipath poblem The vaiability of the gound eflectivity is quantified and its impact on the possible vaiation of the gound multipath eo is descibed Siting ecommendations ae made which enhance the multipath pefomance INTRODUCTION The ARL-9 gound efeence antenna is shown in Figue installed at the William J Hughes FAA Technical Cente, Atlantic City, NJ It is a 9-element collinea aay antenna designed specifically fo the LAAS/BAS application Figue 2 shows the aay antenna with the adome emoved ARL-9 Diffeential PS ound Refeence Antenna 8 5 2 2 2 Figue COMPUTER SIMULATION 9 35 3 25 2 5 5 MEASUREMENT 27 6 3 3 33

ARL-9 Antenna Radome Removed 9 Element Aay 9 Excited Elements Paasitic Elements High-Accuacy Aay Excitation (±25 db, ±2º) Figue 2 The aay antenna compises 9 adiating elements and a 9-way-powe-divide and cabling assembly as shown in Figue 2 The cabling assembly has 9 equal-length coaxial cables that connect to (counting fom the bottom) elements numbes 3, 5, 7, 9,,, 3, 5, and 7 These elements ae excited diectly; the emaining elements ae excited paasitically (indiectly via mutual coupling)the ARL-9 is a vey simple but a vey high pecision antenna The key featues of the ARL-9 antenna ae: One-pot, cicula polaization, L-L2-L5 coveage of the uppe hemisphee o One pot one eceive, no satellite handove poblem o Full NSS band, 5-6 MHz Shap antenna patten cutoff on the hoizon fo mitigation of gound multipath at low elevation o 25 db/º slope on hoizon o 3 db antenna Up/Down gain atio down to 6º elevation 3 db sidelobes in the lowe hemisphee fo mitigation of gound multipath at highe elevation o 3 db antenna Up/Down gain atio Vey high quality caie delay (antenna phase cente) and code (goup) delay chaacteistics o Caie delay vaiation ±cm (unit-to-unit ±mm) o Code delay vaiation ±25cm (unit-to-unit ±3mm) Cicula polaization at low elevation fo mitigation of lateal multipath [5-6] o Taxing aicaft, hanges, etc Unit-to-unit de-coelated sidelobes in the lowe hemisphee o Enhances gound multipath de-coelation amongst gound efeence eceives Integal ai teminal fo lightning potection o Non-scatteing ai teminal configuation, no pefomance degadation The initial concept fo the ARL-9 was developed in 993 and the fist patent was issued in 996 [] The initial concept was vey naow band and thee wee poblems with the implementation An impoved wideband vesion was developed in 999 with an associated patent issued in 2 [2] This second vesion had the same basic achitectue as the ARL-9 [3] but it had one significant poblem, excessive code delay vaiation with azimuth angle at high elevation [] The solution to the poblem associated with the second vesion became appaent in 23 The ARL-9 antenna is the embodiment of this solution Measuements in Decembe of 25, at the William J Hughes FAA Technical Cente [7] (see Figue 3) demonstated excellent pefomance fo the ARL-9 antenna FAA Measuement Atlantic City Decembe 7, 25 ARL-9 Antenna Seial No Figue 3 RANDOM SIDELOBES ENHANCE MULTIPATH DE-CORRELATION AMONST REFERENCE RECIEVER STATIONS The equiement fo coveage of the uppe hemisphee esults in an inheently low-gain antenna Ideally, with no antenna dissipative loss, the highest gain possible is 3 dbi It is vey difficult to design a low-gain antenna with low sidelobes (3 db) The design stategy fo achieving low sidelobes fo a low gain antenna was pesented in [3] The basic concept is to set the systematic (zeo aayexcitation eo) peak sidelobe level substantially below the desied peak sidelobe level (3 db), and then to specify the eo toleance on the aay excitation such that the combined 2-sigma value fo the peak systematic and eo sidelobes is less than 3 db Figue pesents the basic appoach fo the design of the ARL-9 antenna The aay excitation toleances of ± 2 db and ± 2º equie high pecision components fo the collinea aay antenna The elevation pattens fo 2 andom-eo tials pesented in Figue show the pedominant andom natue of the unit-to-unit sidelobe levels

Random sidelobe levels with 2 db amplitude and 2 phase eos 2-sigma up/down gain atio equals 296 db Figue ARL-9 Random Sidelobe level Elevation Angle (Degees) Zeo Eo Peak Sidelobe Level One significant benefit fo the ARL-9 antenna is povided by the andom natue of the unit-to-unit sidelobe level Fou efeence eceive stations ae typically utilized to suppess multipath The fou stations ae located with espect to each othe to povide decoelation of the multipath signals The andom natue of the ARL-9 antenna unit-to-unit sidelobe level enhances the de-coelation of the gound multipath signals ROUND MULTIPATH CHARACTERISTICS The basic geomety fo gound multipath is shown in Figue 5 At the antenna phase cente the diect signal and a gound eflected (multipath) signal ae combined The polaization of the gound eflected signal expeiences a tansfomation upon eflection The Fesnel fomulas quantify this tansfomation and ae pesented below Antenna Phase Cente H Figue 5 ound Multipath eomety Delay 2 H sin( θ ) Diect ound Reflected (Fesnel Fomulas) The Fesnel fomulas fo the eflection facto fo vetical polaization,, and fo hoizontal polaization,, ae given by: θ sin sin + Fee space dielectic constant Relative dielectic constant Conductivity ω Radian fequency θ Elevation angle Smooth Sea Vey Dy ound Figue 6 Reflection Facto (Voltage Ratio) ound Type Fesh Wate Wet ound ω ω sin sin + ω ω ound Paametes Relative Dielectic Constant, 8 8 6 ω ω cos cos cos cos Conductivity, (S/m) 2 ound Reflection Facto Linea Polaization 9 8 7 6 5 3 2 Figue 7 2 3 5 6 7 8 9 Smooth Sea Vetical Polaization Smooth Sea Hoizontal Polaization Vey Wet ound Vetical Polaization Vey Wet ound Hoizontal Polaization Vey Dy ound Vetical Polaization Vey Dy ound Hoizontal Polaization Fequency 575 MHz Bewste Angle: Elevation angle whee the vetical polaization component is a minimum value The gound eflection chaacteistics ae quantified by two paametes in the Fesnel fomulas, the elative dielectic constant, and the conductivity, Figue 6 pesents a table that lists these paametes fo fou diffeent types of gounds anging fom a smooth sea to a vey dy gound

Cicula Pol Reflected Powe (db) ound Reflection Facto Cicula Polaization 2 3 5 6 7 8 Figue 8 H 3m, Antenna Up/Down ain Ratio 3 db 9 δ 6 cm 2 3 5 6 7 8 9 Elevation Angle (Degees) Smooth Sea Cicula Polaization Vey Wet ound Cicula Polaization Vey Dy ound Cicula Polaization δ 5 cm Multipath Eo δ cm 8 db The eflection facto magnitude vesus elevation angle fo vetical and hoizontal linea polaization components of an incident signal ae pesented in Figue 7 The Bewste angle is defined as the elevation angle whee the magnitude of the vetically polaized component is a minimum The eflection phase fo the vetically polaized component vaies 8º acoss the Bewste angle The handedness fo a eflected ciculaly polaized incident signal eveses acoss the Bewste angle On the zenith side of the Bewste angle an incident ight-hand ciculaly polaized incident signal is eflected with lefthand polaization Figue 8 pesents the magnitude of the eflection facto fo an incident ciculaly polaized signal At nea the hoizon ight hand cicula polaization is eflected as ight-hand cicula polaization At the Bewste angle the eflected signal is essentially hoizontally polaized At nea zenith, an incident signal with ight-hand cicula polaization is eflected with left-hand cicula polaization (Thee have been cases whee the antenna gain patten has been measued with espect to ight hand cicula polaization, and the atio of the gain in the zenith diection to the gain in the nadi diection has been epoted as the desied-to-undesied atio fo the zenith diection This, of couse, was in eo since the antenna has, inheently, left-hand cicula polaization in the nadi diection) Figue 8 shows that fo elevation below º the magnitude of the eflection facto is essentially independent of the type of gound Fo elevation above 3º thee is substantial vaiation of the eflection facto magnitude In the zenith diection thee can be an 8 db diffeence in the eflection magnitude fo smooth sea and a vey dy gound The coesponding vaiation in the multipath eo could ange fom 5 cm fo the case of a smooth sea to 6 cm fo the case of vey dy gound DEFINITION OF DESIRED-TO-UNDESIRED (D/U) SINAL RATIO Fo a given satellite elevation angle and assuming a flat hoizontal gound: The D/U atio is defined as the atio of the eceived diect signal to the eceived multipath (indiect) signal An appoximate fomula fo D/U is given by: D Up / Down ain Ratio ( θ ) () U ( ( ( ( Antenna gain with espect to an isotopic antenna (dbi, total adiated powe) ( Magnitude of gound eflection facto θ Elevation angle Equation () assumes polaization match fo both the diect and indiect signals (The magnitude of the diect signal is popotional to the total powe in the diect signal; the magnitude of the indiect signal is popotional to the total powe in the eflected signal) It is a consevative estimate fo the D/U atio An exact fomula fo D/U is given by: D U Antenna gain with espect to vetical linea polaization Antenna gain with espect to hoizontal linea polaization Fesnel Fesnel ( + j + j ( fomula fo vetical polaization fomula fo hoizontal polaization All the factos in Equation (2) ae complex voltages MULTIPATH ERROR VERSUS ELEVATION ANLE The multipath eo, δ(, vesus elevation angle is given by the appoximate fomula [8]: πh δ( 2H sin sin sin D / U λ ( πh δ( ( 2H sin sin sin λ It is assumed that the gound is flat and hoizontal Equation (3) is valid fo H < 75 m and D/U >> (2) (3)

Code Delay Multiptah Eo (Metes) 2 Multipath Eo Vesus Elevation Angle 2 2 3 5 6 7 8 9 Elevation Angle (Degees) H 3 m D/U( 36 db Antenna Up/DownainRatio/( Antenna Up/DownainRatio 3 db ( - 6 db Figue 9 Multipath eo vesus elevation angle is pesented in Figue 9 The intefeence patten shown in Figue 9 is simply that of a souce located 3 m above the gound suface and its image 3 m below the suface It is noted that if the antenna wee located above a pool of wate, the peak eo would be nea 5 m ENERAL SITIN CONSIDERATIONS As indicated in Equation (3), the peak multipath eo is diectly elated to the antenna height above the local gound One would tend to locate the antenna as close to gound as possible, but it is soon ecognized that this location would be ovely sensitive to local tansient objects that can poduce substantial multipath effects Expeience to date has indicated that an antenna phase cente height of 3 m is suitable fo aipot envionments It is ecommended that the phase cente height should not be less than 2 m The vaiability of the peak multipath eo associated with the wate content of the local gound leads to the following ecommendations: Avoid a site with a local bowl-shaped (concave) teain featue Concave gound can amplify the gound eflection facto Concave gound can also accumulate ain wate at the base of the antenna Location at the apex of a convex suface is the ideal location Stabilization consideations ade the local site ( m adius) to minimize the possibility of a wate satuated local gound o pools of wate nea the antenna base Add a laye of cushed stone (o othe suitable mateials) to povide a stable electically-ough suface with a eflection facto anging between -6 and -9 db SUMMARY This pape: Pesented an oveview of the ARL-9 gound efeence antenna pefomance and histoy This antenna is unique with nea ideal chaacteistics Pesented a detailed desciption of gound multipath chaacteistics, which highlighted the possible vaiability of the local gound eflectivity This impacts the multipath pefomance, especially at high elevation Made ecommendations fo the siting of the antenna and possible teatment of the local gound suface fo contol of the vaiability of the local gound eflectivity ACKNOWLEDEMENTS Many thanks ae given to M John Wabuton (William J Hughes FAA Technical Cente) fo his help ove the many yeas with the development of the ARL-9 antenna The successful development of the ARL-9 antenna is cedited, in geat pat, to the technical leadeship of M ay A Schay (BAE Systems) and the manageial leadeship of M ay T Nolan (BAE Systems) REFERENCES [] AR Lopez, US Patent No 5,53,882, PS Antenna Systems, Jul 9, 996 [2] AR Lopez, RJ Kumpfbeck, EM Newman, US Patent No 6,2,5, Self-Contained Pogessive- Phase PS Elements and Antennas, Ma 3, 2 [3] AR Lopez, PS ound Station Antenna fo Local Aea Augmentation System, LAAS, ION NTM 2, 26-28 Januay 2, Anaheim, CA [] AR Lopez, Calibation of LAAS Refeence Antennas, ION PS 2, - Septembe 2, Salt Lake City, UT [5] AR Lopez, LAAS Refeence Antennas Cicula Polaization Mitigates Multipath Effects, ION 59 th Annual Meeting/CITF 22 nd uidance Test Symposium, 23-25 June 23, Albuqueque, NM [6] AR Lopez, LAAS Refeence Antennas Key Siting Consideations, ION NSS 7 th Intenational Meeting of the Satellite Division, 2-2 Sept 2, Long Beach, CA [7] FAA Navigation/LAAS T&E Team, Local Aea Augmentation System Pefomance Analysis / Activities Repot, Repot #9, Repoting Peiod: Januay to Mach 3, 26, Apil 3, 26, pp 3-5 [8] CC Counselman, Multipath-Rejecting PS Antennas, Poceedings of the IEEE, Vol 87, No, Jan 999