Radar Cross Section Analysis of Aircraft using CONCEPT-II
|
|
- Branden Gardner
- 5 years ago
- Views:
Transcription
1 Radar Cross Section Analysis of Aircraft using CONCEPT-II Arne Schröder University of Bern - Institute of Applied Physics Microwave Physics WS2, Modeling of EMC Problems Using CONCEPT-II
2 Radar - Radio Detection and Ranging
3 Radar - Radio Detection and Ranging, Conventional Radar
4 Radar - Radio Detection and Ranging, Passive Radar
5 Key Quantity: Radar Cross Section (RCS) RCS = lim r 4πr 2 E sca 2 E inc 2
6 Key Quantity: Radar Cross Section (RCS) RCS = lim r 4πr 2 E sca 2 E inc 2 Bistatic RCS Monostatic RCS Multistatic RCS - transmitter and receiver at diff. positions - transmitter and receiver at same position - multiple excitations - time consuming computation - multiple transmitters/receivers - arbritrary angles of incidence
7 1 A Typical CONCEPT-II Simulation Procedure 2 Bi- and Monostatic RCS Computations 3 Multistatic RCS Computations 4 Conclusion
8 1 A Typical CONCEPT-II Simulation Procedure 2 Bi- and Monostatic RCS Computations 3 Multistatic RCS Computations 4 Conclusion
9 Typical CONCEPT-II Simulation Procedure Starting point: CAD model, often mechanical model
10 Typical CONCEPT-II Simulation Procedure Starting point: CAD model, often mechanical model CAD cleaning, creating a surface model with CAD tools Closing gaps and overlaps between surfaces Removing detailed geometries like screws, springs etc. Simplification of internal structure
11 Typical CONCEPT-II Simulation Procedure
12 Typical CONCEPT-II Simulation Procedure Starting point: CAD model, often mechanical model CAD cleaning, creating a surface model with CAD tools Closing gaps and overlaps between surfaces Removing detailed geometries like screws, springs etc. Simplification of internal structure Surface mesh generation, i.e. using gmsh
13 Typical CONCEPT-II Simulation Procedure
14 Typical CONCEPT-II Simulation Procedure Starting point: CAD model, often mechanical model CAD cleaning, creating a surface model with CAD tools Closing gaps and overlaps between surfaces Removing detailed geometries like screws, springs etc. Simplification of internal structure Surface mesh generation, i.e. using gmsh CONCEPT-II simulation
15 Typical CONCEPT-II Simulation Procedure
16 Typical CONCEPT-II Simulation Procedure
17 Typical CONCEPT-II Simulation Procedure Starting point: CAD model, often mechanical model CAD cleaning, creating a surface model with CAD tools Closing gaps and overlaps between surfaces Removing detailed geometries like screws, springs etc. Simplification of internal structure Surface mesh generation, i.e. using gmsh CONCEPT-II simulation CONCEPT-II post-processing, external post-processing, i.e. in MATLAB
18 1 A Typical CONCEPT-II Simulation Procedure 2 Bi- and Monostatic RCS Computations 3 Multistatic RCS Computations 4 Conclusion
19 Bistatic Example Airbus A320 Incidence: θ = 90, φ = 0, vertical polarization RCS for: φ = , φ = 0.5 Frequency: 120 MHz
20 Airbus A320 Simulation Setup
21 Airbus A320 Post-Processing
22 Airbus A320 Results CONCEPT HFSS RCS [db(m 2 )] Angle [ ]
23 Monostatic Example NASA Almond Monostatic RCS for: φ = , θ = excitation vectors θ-polarization
24 NASA-Almond Monostatic Setup MLFMA solver RHS compression using ACA, accuracy: 10 5
25 NASA Almond Results θ [ ] φ [ ] RCS [db λ 2 ] 0.9 h and 0.7 GB with CONCEPT-II Not possible in HFSS, memory >120 GB
26 NASA Almond Results RCS [db(m 2 )] CONCEPT HFSS Angle [ ] 0.9 h and 0.7 GB with CONCEPT-II Not possible in HFSS, memory >120 GB
27 1 A Typical CONCEPT-II Simulation Procedure 2 Bi- and Monostatic RCS Computations 3 Multistatic RCS Computations 4 Conclusion
28 Multistatic Example Trajectory Observer Transmitter 1 Airport Bern-Belp Transmitter 2 Aim: Computation of RCS depending on position on trajectory
29 Transmitter 1 Trajectory Transmitter 2 Airport Observer Setup 200 MHz, typical T-DAB frequency Evektor EV-55 aircraft Pre-processing in MATLAB Coordinates of observer, transmitter, trajectory in WGS 84 Computation of incident angles, observation angles
30 CONCEPT-II setup Excitation: Bistatic RCS, angles from file RHS compression: ACA, accuracy: RHSs 31 RHSs
31 Multistatic Example Results Radar Cross Section [db(m 2 )] Transmitter 1 Transmitter Relative Position CONCEPT-II: 12 h, 7 GB - MLFMA 3.3 h, 5 GB - Fast Direct Solver HFSS: computation time h = 41 d
32 1 A Typical CONCEPT-II Simulation Procedure 2 Bi- and Monostatic RCS Computations 3 Multistatic RCS Computations 4 Conclusion
33 Conclusion CONCEPT-II... provides import option for real aircraft models solves large RCS problems efficiently due to ACA-compression of excitation matrix provides fast direct solver, perfectly suited for monostatic RCS problems can treat arbritray angles of incidence and observation angles is well-suited for RCS computation of aircraft
34 Thank you for your attention!
35 P r = P tg t A r σf 4 (4π) 2 R 2 t R2 r
Lecture 7: Introduction to HFSS-IE
Lecture 7: Introduction to HFSS-IE 2015.0 Release ANSYS HFSS for Antenna Design 1 2015 ANSYS, Inc. HFSS-IE: Integral Equation Solver Introduction HFSS-IE: Technology An Integral Equation solver technology
More informationEnhanced Characteristic Basis Function Method for Solving the Monostatic Radar Cross Section of Conducting Targets
Progress In Electromagnetics Research M, Vol. 68, 173 180, 2018 Enhanced Characteristic Basis Function Method for Solving the Monostatic Radar Cross Section of Conducting Targets Jinyu Zhu, Yufa Sun *,
More informationSimulation Advances for RF, Microwave and Antenna Applications
Simulation Advances for RF, Microwave and Antenna Applications Bill McGinn Application Engineer 1 Overview Advanced Integrated Solver Technologies Finite Arrays with Domain Decomposition Hybrid solving:
More informationA MATLAB PHYSICAL OPTICS RCS PREDICTION CODE
A MATLAB PHYSICAL OPTICS RCS PREDICTION CODE Elmo E. Garrido, Jr. and David C. Jenn Naval Postgraduate School Monterey, CA 93943 SUMMARY POFACETS is an implementation of the physical optics approximation
More informationSimulation Advances. Antenna Applications
Simulation Advances for RF, Microwave and Antenna Applications Presented by Martin Vogel, PhD Application Engineer 1 Overview Advanced Integrated Solver Technologies Finite Arrays with Domain Decomposition
More informationCan Xia 1, 2,WanqingYou 2, and Yufa Sun 2, *
Progress In Electromagnetics Research Letters, Vol. 81, 133 139, 2019 Fast Calculation of Monostatic Radar Cross Section of Conducting Targets Using Hierarchical Characteristic Basis Function Method and
More informationHFSS Ansys ANSYS, Inc. All rights reserved. 1 ANSYS, Inc. Proprietary
HFSS 12.0 Ansys 2009 ANSYS, Inc. All rights reserved. 1 ANSYS, Inc. Proprietary Comparison of HFSS 11 and HFSS 12 for JSF Antenna Model UHF blade antenna on Joint Strike Fighter Inherent improvements in
More informationHFSS 14 Update for SI and RF Applications Markus Kopp Product Manager, Electronics ANSYS, Inc.
HFSS 14 Update for SI and RF Applications Markus Kopp Product Manager, Electronics ANSYS, Inc. 1 ANSYS, Inc. September 21, Advanced Solvers: Finite Arrays with DDM 2 ANSYS, Inc. September 21, Finite Arrays
More informationMultistatic SAR Algorithm with Image Combination
Multistatic SAR Algorithm with Image Combination Tommy Teer and Nathan A. Goodman Department of Electrical and Computer Engineering, The University of Arizona 13 E. Speedway Blvd., Tucson, AZ 8571-14 Phone:
More informationWorkshop 10-1: HPC for Finite Arrays
Workshop 10-1: HPC for Finite Arrays 2015.0 Release ANSYS HFSS for Antenna Design 1 2015 ANSYS, Inc. Getting Started Launching ANSYS Electronics Desktop 2015 Select Programs > ANSYS Electromagnetics >
More informationMission Status and Data Availability: TanDEM-X
Mission Status and Data Availability: TanDEM-X Irena Hajnsek, Thomas Busche, Alberto Moreira & TanDEM-X Team Microwaves and Radar Institute, German Aerospace Center irena.hajnsek@dlr.de 26-Jan-2009 Outline
More informationImperfections and Errors (Chapter 6)
Imperfections and Errors (Chapter 6) EC4630 Radar and Laser Cross Section Fall 011 Prof. D. Jenn jenn@nps.navy.mil www.nps.navy.mil/jenn AY011 1 Imperfections and Errors Imperfections and errors are deviations
More informationRCS CALCUATIONS USING THE PHYSICAL OPTICS CODES
RCS CALCATIONS SING THE PHYSICAL OPTICS CODES Introduction Physical optics based RCS calculations are performed by the two Matlab computer codes:. pofacets.m. pobistatic.m The first code (pofacets.m )
More informationHFSS Hybrid Finite Element and Integral Equation Solver for Large Scale Electromagnetic Design and Simulation
HFSS Hybrid Finite Element and Integral Equation Solver for Large Scale Electromagnetic Design and Simulation Laila Salman, PhD Technical Services Specialist laila.salman@ansys.com 1 Agenda Overview of
More informationLocal Multilevel Fast Multipole Algorithm for 3D Electromagnetic Scattering
Progress In Electromagnetics Research Symposium 2005, Hangzhou, China, August 22-26 745 Local Multilevel Fast Multipole Algorithm for 3D Electromagnetic Scattering Jun Hu, Zaiping Nie, Lin Lei, and Jun
More informationUnknown calibrators characterization by means of COSMO-SkyMed data
Unknown calibrators characterization by means of COSMO-SkyMed data CEOS SAR 2015 Valerio Grimani, Pasquale Salemme 83230918-DOC-TAS-EN-003 Needs for Radiometric performances assesment Need of different
More informationModeling the Effects of Wind Turbines on Radar Returns
Modeling the Effects of Wind Turbines on Radar Returns R. Ryan Ohs, Gregory J. Skidmore, Dr. Gary Bedrosian Remcom, Inc. State College, PA USA Abstract Wind turbines located near radar installations can
More informationNew Technologies in CST STUDIO SUITE CST COMPUTER SIMULATION TECHNOLOGY
New Technologies in CST STUDIO SUITE 2016 Outline Design Tools & Modeling Antenna Magus Filter Designer 2D/3D Modeling 3D EM Solver Technology Cable / Circuit / PCB Systems Multiphysics CST Design Tools
More informationUser s Manual for FEM-BEM Method
NASA/CR-22-211966 User s Manual for FEM-BEM Method Version 1. Theresa Butler Lockheed Martin Corporation, Hampton, Virginia December 22 The NASA STI Program Office... in Profile Since its founding, NASA
More informationHFSS - Antennas, Arrays and FSS's. David Perry Applications Engineer Ansoft Corporation
HFSS - Antennas, Arrays and FSS's David Perry Applications Engineer Ansoft Corporation Synopsis Some Excerpts from What s New Enhancements to HFSS Wave Guide Simulator (WGS) What is it? Why you would use
More informationPATTERN SYNTHESIS FOR PLANAR ARRAY BASED ON ELEMENTS ROTATION
Progress In Electromagnetics Research Letters, Vol. 11, 55 64, 2009 PATTERN SYNTHESIS FOR PLANAR ARRAY BASED ON ELEMENTS ROTATION F. Zhang, F.-S. Zhang, C. Lin, G. Zhao, and Y.-C. Jiao National Key Laboratory
More informationMotion Compensation in Bistatic Airborne SAR Based on a Geometrical Approach
SAR Based on a Geometrical Approach Amaya Medrano Ortiz, Holger Nies, Otmar Loffeld Center for Sensorsystems (ZESS) University of Siegen Paul-Bonatz-Str. 9-11 D-57068 Siegen Germany medrano-ortiz@ipp.zess.uni-siegen.de
More informationResearch Article A New Shooting Bouncing Ray Method for Composite Scattering from a Target above the Electrically Large Scope Sea Surface
Hindawi Mathematical Problems in Engineering Volume 17, Article ID 61745, 7 pages https://doi.org/1.1155/17/61745 Research Article A New Shooting Bouncing Ray Method for Composite Scattering from a Target
More informationLecture 2: Introduction
Lecture 2: Introduction v2015.0 Release ANSYS HFSS for Antenna Design 1 2015 ANSYS, Inc. Multiple Advanced Techniques Allow HFSS to Excel at a Wide Variety of Applications Platform Integration and RCS
More informationSolution of Electrically Large Scattering problems using the Characteristic Basis Function Method
Forum for Electromagnetic Research Methods and Application Technologies (FERMAT) Solution of Electrically Large Scattering problems using the Characteristic Basis Function Method Chao Li 1,2, Raj Mittra
More informationPowerful features (1)
HFSS Overview Powerful features (1) Tangential Vector Finite Elements Provides only correct physical solutions with no spurious modes Transfinite Element Method Adaptive Meshing r E = t E γ i i ( x, y,
More informationA Graphical User Interface (GUI) for Two-Dimensional Electromagnetic Scattering Problems
A Graphical User Interface (GUI) for Two-Dimensional Electromagnetic Scattering Problems Veysel Demir vdemir@olemiss.edu Mohamed Al Sharkawy malshark@olemiss.edu Atef Z. Elsherbeni atef@olemiss.edu Abstract
More information2
1 2 3 4 5 Summary A bistatic k-space image concept for frequency domain (FD) electromagnetic (EM) computer codes is presented. The concept enables images to be computed without the frequency sweep required
More informationHFSS PO Hybrid Region
HFSS PO Hybrid Region Introduction The design of electrically large systems poses many challenges. Electromagnetic simulations can relatively quickly assess options and trade-offs before any physical testing.
More informationHFSS: Optimal Phased Array Modeling Using Domain Decomposition
HFSS: Optimal Phased Array Modeling Using Domain Decomposition 15. 0 Release Authors: Dane Thompson Nick Hirth Irina Gordion Sara Louie Presenter: Dane Thompson Motivation Electronically scannable antenna
More informationEVALUATION OF BISTATIC FAR-FIELD QUANTITIES FROM NEAR-FIELD MEASUREMENTS
Progress In Electromagnetics Research, PIER 25, 167 188, 2000 EVALUATION OF BISTATIC FAR-FIELD QUANTITIES FROM NEAR-FIELD MEASUREMENTS J. L. Leou and H. J. Li Department of Electrical Engineering & Graduate
More informationIMPLEMENTATION OF ANALYTICAL (MATLAB) AND NUMERICAL (HFSS) SOLUTIONS ADVANCED ELECTROMAGNETIC THEORY SOHAIB SAADAT AFRIDI HAMMAD BUTT ZUNNURAIN AHMAD
STUDY OF SCATTERING & RESULTANT RADIATION PATTERN: INFINITE LINE CURRENT SOURCE POSITIONED HORIZONTALLY OVER A PERFECTLY CONDUCTING INFINITE GROUND PLANE IMPLEMENTATION OF ANALYTICAL (MATLAB) AND NUMERICAL
More informationA Magnetic Field Integral Equation Based Iterative Solver for Scattered Field Prediction
Progress In Electromagnetics Research M, Vol. 40, 27 35, 2014 A Magnetic Field Integral Equation Based Iterative Solver for Scattered Field Prediction Robert Brem * and Thomas F. Eibert Abstract An iterative
More informationDevelopment of Code for a Physical Optics Radar Cross Section prediction and analysis application
Calhoun: The NPS Institutional Archive DSpace Repository Department of Systems Engineering Thesis and Dissertation Collection 2004-09 Development of Code for a Physical Optics Radar Cross Section prediction
More informationFor functionality and CAD/EDA import filter, see technical specifications of the CST STUDIO SUITE
CST MICROWAVE STUDIO Technical Specification 1 May 2015 Frontend Module For functionality and CAD/EDA import filter, see technical specifications of the CST STUDIO SUITE Transient Solver Module Fast and
More informationOptimization of metallic biperiodic photonic crystals. Application to compact directive antennas
Optimization of metallic biperiodic photonic crystals Application to compact directive antennas Nicolas Guérin Computational Optic Groups (COG) IFH, ETHZ, http://alphard.ethz.ch Keywords: 3D modeling,
More informationRCS Measurement and Analysis of Rectangular and Circular Cross-section Cavities
RCS Measurement and Analysis of Rectangular and Circular Cross-section Cavities Abhinav Bharat, M L Meena, S. Sunil Kumar, Neha Sangwa, Shyam Rankawat Defence Laboratory, DRDO Jodhpur, India-342011 Abstract
More informationKeywords: Quasi-static principle; Moving target group; Multilevel fast multipole; Electromagnetic scattering; RCS
4th International Conference on Machinery, Materials and Information Technology Applications (ICMMITA 2016) Analysis of Electromagnetic Scattering Characteristics of Moving Target Group Based on Quasi-static
More informationPHYS 202 Notes, Week 8
PHYS 202 Notes, Week 8 Greg Christian March 8 & 10, 2016 Last updated: 03/10/2016 at 12:30:44 This week we learn about electromagnetic waves and optics. Electromagnetic Waves So far, we ve learned about
More informationX-ray Diffraction from Materials
X-ray Diffraction from Materials 2008 Spring Semester Lecturer; Yang Mo Koo Monday and Wednesday 14:45~16:00 8. Experimental X-ray Diffraction Procedures 8.1 Diffraction Experiments using Films 8.1.1 Laue
More informationWorkshop 3-1: Antenna Post-Processing
Workshop 3-1: Antenna Post-Processing 2015.0 Release ANSYS HFSS for Antenna Design 1 2015 ANSYS, Inc. Example Antenna Post-Processing Analysis of a Dual Polarized Probe Fed Patch Antenna This example is
More informationNumerical Simulation of RCS for A Spherical Convergent Flap Nozzle with A Non-rectangular Divergent Duct
Numerical Simulation of RCS for A Spherical Convergent Flap Nozzle with A Non-rectangular Divergent Duct CUI Jinhui a, SHANG Shoutang a, YANG Qingzhen b, CHEN Lihai b a AVIC Shenyang Engine Design and
More informationVirtual Engineering: Model based Off-line Programming Method for Industrial Robot
Virtual Engineering: Model based Off-line Programming Method for Industrial Robot Xingguo Yin, Li Tao ABB Corporate Research China No. 31 Fu Te Dong Dan Rd., Waigaoqiao Free Trade Zone, 200131 Shanghai,
More informationLAB # 3 Wave Port Excitation Radiation Setup & Analysis
COMSATS Institute of Information Technology Electrical Engineering Department (Islamabad Campus) LAB # 3 Wave Port Excitation Radiation Setup & Analysis Designed by Syed Muzahir Abbas 1 WAVE PORT 1. New
More informationITERATIVE HYBRID METHOD FOR ELECTROMAG- NETIC SCATTERING FROM A 3-D OBJECT ABOVE A 2-D RANDOM DIELECTRIC ROUGH SURFACE
Progress In Electromagnetics Research, Vol. 117, 435 448, 2011 ITERATIVE HYBRID METHOD FOR ELECTROMAG- NETIC SCATTERING FROM A 3-D OBJECT ABOVE A 2-D RANDOM DIELECTRIC ROUGH SURFACE W. Yang, Z. Q. Zhao
More informationComparison of iteration convergences of SIE and VSIE for solving electromagnetic scattering problems for coated objects
RADIO SCIENCE, VOL. 38, NO. 2, 1028, doi:10.1029/2002rs002610, 2003 Comparison of iteration convergences of SIE and VSIE for solving electromagnetic scattering problems for coated objects Cai-Cheng Lu
More informationHFSS 14 Update for SI and RF Applications. Presenter: Senior Application Engineer Jeff Tharp, Ph.D.
HFSS 14 Update for SI and RF Applications Presenter: Senior Application Engineer Jeff Tharp, Ph.D. 1 Overview Advanced Integrated Solver Technologies Finite Arrays with Domain Decomposition Hybrid solving
More informationEfficacy of Numerically Approximating Pi with an N-sided Polygon
Peter Vu Brewer MAT66 Honors Topic Efficacy of umerically Approximating Pi with an -sided Polygon The quest for precisely finding the irrational number pi has been an endeavor since early human history.
More informationParameterization of Meshes
2-Manifold Parameterization of Meshes What makes for a smooth manifold? locally looks like Euclidian space collection of charts mutually compatible on their overlaps form an atlas Parameterizations are
More informationDual Polarized Phased Array Antenna Simulation Using Optimized FDTD Method With PBC.
Dual Polarized Phased Array Antenna Simulation Using Optimized FDTD Method With PBC. Sudantha Perera Advanced Radar Research Center School of Electrical and Computer Engineering The University of Oklahoma,
More informationNanostructures with HFSS
. May 9 leidenberger@ifh.ee.ethz.ch / 9 Nanostructures with HFSS Patrick Leidenberger. May 9 . May 9 leidenberger@ifh.ee.ethz.ch / 9 Table of contents HFSS Features Mie Benchmark Possible Simulation Mistakes
More informationNew Approach to finding Active-element Patterns for Large Arrays
New Approach to finding Active-element Patterns for Large Arrays Alan Larkin O Donnell Thesis submitted to the faculty of the Virginia Polytechnic Institute and State University in partial fulfillment
More informationM-SPURT Compressing the target characterization for a fast monostatic RCS simulation
M-SPURT Compressing the target characterization for a fast monostatic RCS simulation Henna Perälä, Minna Väilä, and Juha Jylhä Laboratory of Signal Processing Tampere University of Technology Tampere,
More informationPerformance Evaluation of the Radon Transformation in Limited Angle Radar Tomography
Performance Evaluation of the Radon Transformation in Limited Angle Radar Tomography Joshua Alton Noble Pennsylvania State University Faculty Research Advisor: Ram Narayanan, Ph.D. Professor of Electrical
More informationNEW BENCHMARK RADAR TARGETS FOR SCATTERING ANALYSIS AND ELECTROMAGNETIC SOFTWARE VALIDATION
Progress In Electromagnetics Research, PIER 88, 39 52, 2008 NEW BENCHMARK RADAR TARGETS FOR SCATTERING ANALYSIS AND ELECTROMAGNETIC SOFTWARE VALIDATION D. Escot-Bocanegra, D. Poyatos-Martinez R. Fernández-Recio,
More informationVirtual Acoustic Prototyping for Loudspeaker Horn Development
Presented at the COMSOL Conference 2010 Boston Virtual Acoustic Prototyping for Loudspeaker Horn Development Alex Salvatti Senior R&D Engineer JBL Professional, Northridge CA alex.salvatti@harman.com Outline
More informationBistatic SAR coherence improvement through spatially variant polarimetry
1 Bistatic SAR coherence improvement through spatially variant polarimetry By Daniel Andre Centre for Electronic Warfare, Cranfield University, Defence Academy of the United Kingdom, Shrivenham, UK. Abstract
More informationAccurate Radar Cross Section Modelling of Jet Inlets & Engines
Kwok Kee Chan Chan Technologies Inc. 15 Links Lane Brampton, Ontario L6Y 5H1 Canada Silvester Wong and Edwin Riseborough DRDC-Ottawa 371 Carling Avenue Ottawa, Ontario K1A Z4 Canada kwok-kee.chan@rogers.com
More informationThe sources must be coherent. This means they emit waves with a constant phase with respect to each other.
CH. 24 Wave Optics The sources must be coherent. This means they emit waves with a constant phase with respect to each other. The waves need to have identical wavelengths. Can t be coherent without this.
More informationGlobal Illumination and the Rendering Equation
CS294-13: Special Topics Lecture #3 Advanced Computer Graphics University of California, Berkeley Handout Date??? Global Illumination and the Rendering Equation Lecture #3: Wednesday, 9 September 2009
More informationAIR FORCE INSTITUTE OF TECHNOLOGY
AFIT/GE/ENG/04-24 UTILIZING NEAR-FIELD MEASUREMENTS TO CHARACTERIZE FAR-FIELD RADAR SIGNATURES THESIS John R. Watkins Captain, USAF AFIT/GE/ENG/04-24 DEPARTMENT OF THE AIR FORCE AIR UNIVERSITY AIR FORCE
More informationA RCS model of complex targets for radar performance prediction
Tampere University of Technology A RCS model of complex targets for radar performance prediction Citation Väilä, M., Jylhä, J., Väisänen, V., Perälä, H., Visa, A., Harju, M., & Virtanen, K. (217). A RCS
More informationEXTENDED EXACT TRANSFER FUNCTION ALGO- RITHM FOR BISTATIC SAR OF TRANSLATIONAL IN- VARIANT CASE
Progress In Electromagnetics Research, PIER 99, 89 108, 2009 EXTENDED EXACT TRANSFER FUNCTION ALGO- RITHM FOR BISTATIC SAR OF TRANSLATIONAL IN- VARIANT CASE J. P. Sun and S. Y. Mao School of Electronic
More informationixcube 4-10 Brief introduction for membrane and cable systems.
ixcube 4-10 Brief introduction for membrane and cable systems. ixcube is the evolution of 20 years of R&D in the field of membrane structures so it takes a while to understand the basic features. You must
More informationMRI Induced Heating of a Pacemaker. Peter Krenz, Application Engineer
MRI Induced Heating of a Pacemaker Peter Krenz, Application Engineer 1 Problem Statement Electric fields generated during MRI exposure are dissipated in tissue of the human body resulting in a temperature
More informationProcessing techniques for a GNSS-R scatterometric remote sensing instrument
Processing techniques for a GNSS-R scatterometric remote sensing instrument Philip J. Jales (1) Martin Unwin (2) Craig Underwood (1) (1) Surrey Space Centre, University Of Surrey, UK (2) Satellite Technology
More informationLocal Reflection Models
Local Reflection Models Illumination Thus Far Simple Illumination Models Ambient + Diffuse + Attenuation + Specular Additions Texture, Shadows, Used in global algs! (Ray tracing) Problem: Different materials
More informationEfficient Meshing Scheme for Bodies of Revolution Application to Physical Optics Prediction of Electromagnetic Scattering
Progress In Electromagnetics Research M, Vol. 48, 163 172, 216 Efficient Meshing Scheme for Bodies of Revolution Application to Physical Optics Prediction of Electromagnetic Scattering Zohreh Asadi and
More informationSupplementary Material: The Rotation Matrix
Supplementary Material: The Rotation Matrix Computer Science 4766/6778 Department of Computer Science Memorial University of Newfoundland January 16, 2014 COMP 4766/6778 (MUN) The Rotation Matrix January
More informationTHE concept of using a lossy material to absorb an
40 IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, VOL. 45, NO. 1, JANUARY 1997 A Comparison of Anisotropic PML to Berenger s PML and Its Application to the Finite-Element Method for EM Scattering Jo-Yu
More informationEfficient Higher-Order Analysis of Electromagnetic Scattering of Objects in Half-Space by Domain Decomposition Method with a Hybrid Solver
Progress In Electromagnetics Research C, Vol. 68, 201 209, 2016 Efficient Higher-Order Analysis of Electromagnetic Scattering of Objects in Half-Space by Domain Decomposition Method with a Hybrid Solver
More informationHFSS 3D Components. Steve Rousselle, ANSYS. Build, Share, Conquer Release. Release ANSYS, Inc.
HFSS 3D Components Build, Share, Conquer 2015.0 Release Steve Rousselle, ANSYS 1 2015 ANSYS, Inc. What is a 3D Component? Exploded View Assembly of 3D Components Device 2 2015 ANSYS, Inc. Introduction
More informationLecture 04. Fundamentals of Lidar Remote Sensing (2)
Lecture 04. Fundamentals of Lidar Remote Sensing (2) Lidar Equation Introduction Physical Picture of Lidar Equation Fundamental Lidar Equation Different Forms of Lidar Equation Illustration of Lidar Equation
More informationREDESIGN AND OPTIMIZATION OF THE PAVING AL- GORITHM APPLIED TO ELECTROMAGNETIC TOOLS (INVITED PAPER)
Progress In Electromagnetics Research B, Vol. 29, 409 429, 2011 REDESIGN AND OPTIMIZATION OF THE PAVING AL- GORITHM APPLIED TO ELECTROMAGNETIC TOOLS (INVITED PAPER) J. Moreno, M. J. Algar, I. González,
More informationAnalysis of Urban Areas Scattering with Simulated SAR Imagery
Analysis of Urban Areas Scattering with Simulated SAR Imagery G. Margarit, J. J. Mallorquí, I. Corney, L. Pipia, C. López-Martínez, X. Fàbregas, A. Aguasca mallorqui@tsc.upc.edu Remote Sensing Laboratory
More informationHigh-Frequency Method for Terahertz Radar Cross Section of Conductive Targets in Free Space
Progress In Electromagnetics Research B, Vol. 59, 193 04, 014 High-Frequency Method for Terahertz Radar Cross Section of Conductive Targets in Free Space Houqiang Hua, Yuesong Jiang *, and Yuntao He Abstract
More informationReflection and Shading
Reflection and Shading R. J. Renka Department of Computer Science & Engineering University of North Texas 10/19/2015 Light Sources Realistic rendering requires that we model the interaction between light
More informationMRFD Method for Scattering from Three Dimensional Dielectric Bodies
RADIONGINRING, VOL., NO., SPTMBR 58 MRFD Method for Scattering from Three Dimensional Dielectric Bodies Ahmet Fazil YAGLI Turksat A.S. Ar-Ge Uydu Tasarim Dir. Gazi Universitesi Teknopark, Golbasi Ankara,
More informationHomogeneous coordinates, lines, screws and twists
Homogeneous coordinates, lines, screws and twists In lecture 1 of module 2, a brief mention was made of homogeneous coordinates, lines in R 3, screws and twists to describe the general motion of a rigid
More informationIdentifiability of 3D Attributed Scattering Features from Sparse Nonlinear Apertures
Identifiability of 3D Attributed Scattering Features from Sparse Nonlinear Apertures Julie Ann Jackson and Randolph L. Moses Ohio State University, Dept. of Electrical and Computer Engineering, Columbus,
More information2.710 Optics Spring 09 Solutions to Problem Set #1 Posted Wednesday, Feb. 18, 2009
MASSACHUSETTS INSTITUTE OF TECHNOLOGY.70 Optics Spring 09 Solutions to Problem Set # Posted Wednesday, Feb. 8, 009 Problem : Spherical waves and energy conservation In class we mentioned that the radiation
More informationPSI Precision, accuracy and validation aspects
PSI Precision, accuracy and validation aspects Urs Wegmüller Charles Werner Gamma Remote Sensing AG, Gümligen, Switzerland, wegmuller@gamma-rs.ch Contents Aim is to obtain a deeper understanding of what
More informationMathematical simulation of riveting process
Mathematical simulation of riveting process Author: Margarita Kovtun E-mail: margarita_kovtun@inbox.ru Introduction he theme of this report arose in the context of the project which results from the cooperation
More informationPedestrian Detection with Radar and Computer Vision
Pedestrian Detection with Radar and Computer Vision camera radar sensor Stefan Milch, Marc Behrens, Darmstadt, September 25 25 / 26, 2001 Pedestrian accidents and protection systems Impact zone: 10% opposite
More informationIntroduction to Radiosity
Introduction to Radiosity Produce photorealistic pictures using global illumination Mathematical basis from the theory of heat transfer Enables color bleeding Provides view independent representation Unfortunately,
More informationANALYSIS OF ELECTROMAGNETIC SCATTERING WITH HIGHER-ORDER MOMENT METHOD AND NURBS MODEL
Progress In Electromagnetics Research, PIER 96, 83 100, 2009 ANALYSIS OF ELECTROMAGNETIC SCATTERING WITH HIGHER-ORDER MOMENT METHOD AND NURBS MODEL Z.-L. Liu Temasek Laboratories National University of
More informationSurfaces: notes on Geometry & Topology
Surfaces: notes on Geometry & Topology 1 Surfaces A 2-dimensional region of 3D space A portion of space having length and breadth but no thickness 2 Defining Surfaces Analytically... Parametric surfaces
More informationUse of Simulation Software in Pre-Qualification Tests
Use of Simulation Software in Pre-Qualification Tests RF & Hyper Europe 2009 Villepinte Yannis Braux: Senior EM Engineer CST FRANCE 1 www.cst.com Use of Simulation Software in Pre-Qualification Tests 1.
More informationA Diagonal Split-cell Model for the High-order Symplectic FDTD Scheme
PIERS ONLINE, VOL. 2, NO. 6, 2006 715 A Diagonal Split-cell Model for the High-order Symplectic FDTD Scheme Wei Sha, Xianliang Wu, and Mingsheng Chen Key Laboratory of Intelligent Computing & Signal Processing
More informationUniversity Physics (Prof. David Flory) Chapt_37 Monday, August 06, 2007
Name: Date: 1. If we increase the wavelength of the light used to form a double-slit diffraction pattern: A) the width of the central diffraction peak increases and the number of bright fringes within
More informationElectromagnetics. R14 Update. Greg Pitner ANSYS, Inc. February 24, 2012
Electromagnetics R14 Update Greg Pitner 1 HFSS Version 14 2 HFSS Overview Advanced Integrated Solver Technologies Finite Arrays with Domain Decomposition Hybrid solving: FEBI, IE Regions Physical Optics
More informationValidation of an Unstructured Overset Mesh Method for CFD Analysis of Store Separation D. Snyder presented by R. Fitzsimmons
Validation of an Unstructured Overset Mesh Method for CFD Analysis of Store Separation D. Snyder presented by R. Fitzsimmons Stores Separation Introduction Flight Test Expensive, high-risk, sometimes catastrophic
More informationAnalytic Spherical Geometry:
Analytic Spherical Geometry: Begin with a sphere of radius R, with center at the origin O. Measuring the length of a segment (arc) on a sphere. Let A and B be any two points on the sphere. We know that
More informationOpenVSP: Parametric Geometry for Conceptual Aircraft Design. Rob McDonald, Ph.D. Associate Professor, Cal Poly
OpenVSP: Parametric Geometry for Conceptual Aircraft Design Rob McDonald, Ph.D. Associate Professor, Cal Poly 1 Vehicle Sketch Pad (VSP) Rapid parametric geometry for design NASA developed & trusted tool
More informationdq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ =
Radiometry (From Intro to Optics, Pedrotti -4) Radiometry is measurement of Emag radiation (light) Consider a small spherical source Total energy radiating from the body over some time is Q total Radiant
More informationLecture 39: Mueller Calculus and Optical Activity Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:29 PM) W.J.
C:\Dallas\1_Courses\1_OpSci_33\1 Lecture Notes\39 MuellerCalculus.doc: Page 1 of 5 Lecture 39: Mueller Calculus and Optical Activity Physical Optics II (Optical Sciences 33) (Updated: Friday, April 29,
More informationThis offering is not approved or endorsed by OpenCFD Limited, the producer of the OpenFOAM software and owner of the OPENFOAM and OpenCFD trade marks.
Disclaimer This offering is not approved or endorsed by OpenCFD Limited, the producer of the OpenFOAM software and owner of the OPENFOAM and OpenCFD trade marks. Introductory OpenFOAM Course From 8 th
More informationBEARING CAPACITY OF CIRCULAR FOOTING
This document describes an example that has been used to verify the ultimate limit state capabilities of PLAXIS. The problem involves the bearing capacity of a smooth circular footing on frictional soil.
More information3D Feature Estimation for Sparse, Nonlinear Bistatic SAR Apertures
3D Feature Estimation for Sparse, Nonlinear Bistatic SAR Apertures Julie Ann Jackson Dept. of Electrical and Computer Engineering Air Force Institute of Technology Dayton, Ohio, 45433 Email: julie.jackson@afit.edu
More informationDeterministic Approach to Achieve Broadband Polarization-Independent Diffusive Scatterings Based on Metasurfaces
Supporting Information for Deterministic Approach to Achieve Broadband Polarization-Independent Diffusive Scatterings Based on Metasurfaces He-Xiu Xu 1,,6 *, Shaojie Ma 1, Xiaohui Ling 1,6, Xiao-Kuan Zhang,
More information