An 8-channel RF Transceive Coil For Parallel Imaging at 7T/298MHz

Size: px
Start display at page:

Download "An 8-channel RF Transceive Coil For Parallel Imaging at 7T/298MHz"

Transcription

1 CST European User Group Meeting May 2011, Munich, Germany An 8-channel RF Transceive Coil For Parallel Imaging at 7T/298MHz X. Hanus CEA DSM Irfu SACM An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 1

2 Contents NeuroSpin: a high-field MRI facility at CEA Saclay Iseult: a franco/german R&D program for high field MRI RF coils design with numerical codes MWS-TD comparison for an 8-channel RF prototype coil with two anatomical models, Ella (Virtual Family) and Hum (Homemade Unstructured Model based on Ella tissues): mesh & transient simulation parameters tune/match circuit in Design Studio illustration with a reference birdcage mode (rotating B 1+ field) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 2

3 NeuroSpin: a neuro-imaging MR facility at CEA Saclay Project initiated in 2003 from the CEA Life Sciences Division (DSV) to achieve a unique platform for high field MR imaging Internal collaboration with CEA Physical Sciences Division (DSM) Franco/german 'Iseult' collaboration (CEA/Siemens/partners) Building delivered in 2006 (Vasconi). Actually: 3T & 7T scanners for human (Siemens), 17T scanners for small animals (Bruker), 11.7T/90 cm human MRI scanner (Iseult, 2013) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 3

4 NeuroSpin: a neuro-imaging MR facility at CEA Saclay Building delivered in 2006 (Vasconi). An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 4

5 Iseult/Inumac partnership goals Iseult/Inumac: a franco-german CEA-Siemens R&D program for human MR imaging at Ultra High Field (11.7T/500 MHz MRI scanner, contrast agents, pulse sequence designs, etc.) Contract Iseult / CEA-DSM-Irfu to design and build a large bore 11.7T/90 cm magnet, cryogenic system and RF coils (SACM) A challenging transmit RF coil for parallel imaging at 500 MHz Maintain B 1+ homogeneity over the brain despite wavelength effects (as frequency increases, RF wavelength is shortened (λ 0 =60 cm at f=500 MHz) and even more in the brain (ε=50) λ brain =8.5 cm Limit RF dissipations and heating in the inhomogeneous and dissipative dielectric human tissues (SAR, hot spots) A test bed with a validated design at 300 MHz (7T) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 5

6 Iseult/Inumac partnership organization Oséo Franco-German Co-Operation Agreement BMBF Conv. d Aide Consortium français Consortium allemand Guerbet mandat Univ de Fribourg Acc Collab Acc Collab CEA 25 M Acc Collab Siemens MS Luvata Acc Collab Alstom MSA Bruker Biospin MRI Acc Collab An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 6

7 RF coils design with 3D full-wave solvers Various coil designs simulated with MWS-TD since 2004: a 500 MHz TEM/birdcage volume coil with 32 rods, 300MHz array coils based on striplines superposition Curent designs: 8 channels, superposed striplines with Balun feed, and pre-matching system FEM solver with conformal (tetrahedron) meshing to design and optimize the strips assembling MWS-TD validation with accurate anatomical voxel models (HUGO, Virtual family) or home-made models CAD model imported in MWS (.sat/.hfss) Setup for transient calculations (Boolean operations, coaxial connectors (50 Ω) to apply waveguide excitations, additional inactive volumes for local meshing) tune/match circuit in Design Studio maps (E,H,J) x 8 channels basic birdcage mode (combine) B1, SAR An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 7

8 The FEM model and results B1 + (a= 6.8) S_I,I S_I,1 S_I,2 SAR_CP (a= 6.8) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 8

9 The FIT model (import + coaxial WG ports) (1) Different views of FIT model An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 9

10 The FIT model: Coil without shielding (2) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 10

11 The FIT model: Balun and coaxial WG port (3) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 11

12 The FIT model: radiating dipole and capacitor (4) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 12

13 The FIT model: WG port to stripline transition (5) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 13

14 Design model and Cartesian grid 2D mesh view of dipole-1 and dipole-2 in midaxial plane (left), and at port plane (right) Mesh grid details for dipole-1 in axial planes (20 Mcells, local Dx,y = 0.7mm) Align all fixpoints to mesh grid is not possible (< 0.3mm) Meshing is not identical for dipoles (diff. angle positions in the grid) Some mesh cells may contain more than 2 materials (PBA) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 14

15 Inactive volumes to improve local meshing An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 15

16 The anatomical models 'Ella' and 'Hum' (1) 'Ella' from Virtual Family (1mm resolution ) 'Hum' a 9-tissue Home-made Unstructured Model based on Ella dataset An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 16

17 The anatomical models 'Ella' and 'Hum' (2) RF coil loaded with 'Ella_VF' (top) and 'Hum' (bottom) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 17

18 Meshing parameters Same global & local meshing parameters but Hum has finally more meshcells (fixpoints) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 18

19 Mesh grid for Ella_VF-1mm An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 19

20 Mesh grid for Hum An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 20

21 Simulation characteristics Dell 690 XP 64 bit (4x Xeon 5140) + 2xGPU (FX Quadro 5600) Mesh parameters: Global: l/λ= 30/10/30 + FPBA + Equilibrate mesh=1.2 Local: Dx=Dy=0.7 mm, Dz= 1mm (inactive volumes) Local: prority=1 (coaxial connectors, critical elements) cells (Ella_VF) and cells (Hum) Transient parameters: WG excitations [ MHz] on coaxial connectors accuracy limit = -50 db Background=PEC and BC='electric' all except zmin ('open') Time duration 15H to 30H / port Tuning/matching of the dipoles with a DS optimized circuit An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 21

22 Which accuracy limit to use? (1) ProtoV3b_(A) coil loaded with a sphere Inactive volumes for local meshing Global meshing Local meshing Coil elements all lossy materials except coaxial connectors, Background = PEC ; BC = all boundaries, Channel-2 single excitation (τ P = ns, τ=1.02 ps [ MHz]), Stop accuracy limit= -40/-50/-60/-80 db An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 22

23 Which accuracy limit to use? (2) Energy: -40/-50/-60/-80 db 1D-probe [0;0;20] 1D-probe [0;0;20] zoom Reflected S 2,2 parameter (db) 1D-probe [0;0;20] 1D-probe [0;0;20] zoom S 2,2 & 1D-probes at sphere center vs accuracy limits An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 23

24 Which accuracy limit (3) P 0 = 0.5 W (rms) -40db -50 db -60db -80db SAR Calculation Results Pacc. (W-rms) Pabs. (W-rms) Ptissue (W-rms) SAR_10g (W/kg) Max SAR (W/kg) Q_Loss Calculation Results W (J) x x x x 10-8 Pmet. (W-rms) Pdiel. (W-rms) Ptot. (W-rms) Table 1: CHANNEL-2 single f= 298 MHz for E=-40db/-50db/-60db/-80db Table: Losses calculations results vs accuracy limits Accuracy limit = -50 db Power balance consistency (effective input power at ports (S-matrix) Vs total losses in the structure over-estimation of metallic losses?) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 24

25 Boundary condition at z-limits: 'electric' vs 'open' (1) BC: all boundaries BC: xmin,xmax,ymin,ymax,zmax and zmin Scattering S I,2 parameters for 'electric condition Scattering S I,2 parameters for 'open' condition S-parameters for port-2 for BC= 'electric' (left) and 'open' (right), background= PEC An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 25

26 Boundary condition at z-limits: 'electric' vs 'open' (2) Energy decay at port-2 Scattering S i,2 (db) 1D-H probe at sphere center 1D-E probe at sphere center Energy decay, S-parameters at port-2, 1D-H & E probes at center of coil/sphere An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 26

27 Effect of background material: PEC vs vacuum Background= PEC BC = electric S-parameters at port-1 Background= vacuum BC = open S-parameters at port-3 S-parameters at port-1 & port-3 for background=pec & BC= electric (solid lines) and background= vacuum & BC = open (dashed lines) with Ella_VF) RF coil has lateral shielding zmin only An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 27

28 Improve the frequencies consistency Some improvement in the design handling: Larger coaxial (0.9/3 1.5/5), inactive cylinders better adjusted, lines/λ Gives better consistency but there is no unique parameter tuning of the dipoles frequencies can be made in Design Studio An 8-ch RF transmit coil for MRI at 7T/298MHz (X.H.,M.L.) CEA-DSM-Irfu-SACM 28

29 Tuning/matching circuit optimized in Design Studio A parameterized (Z,C) circuit in Design Studio (ELT & Capa) to tune/match the individual channels The tune/match Transmission Line circuit (Z,C) Ella_VF Hum Parameters are optimized in minimizing the reflected S- parameters magnitudes for each channel (single excitation) 3D-field quantities in MWS are extracted with the optimized tuned/matched circuits in DS An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 29

30 Tuning/matching: reflected S-parameters (1) Effect of the tuning/matching on the reflected S-parameters for Ella_VF (top) and Hum (bottom) An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 30

31 Tuning/matching: reflected S-parameters (2) Tuned/matched S-parameters phase and impedances (Smith) for Ella_VF An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 31

32 Tuning/matching : transmission to neighbours (Ella_VF) original After tuning/matching CHANNEL-1 (db, phase) CHANNEL-2 (db, phase) Transmitted S_parameters before (top) and after tuning/matching (bottom) for CH-1 and CH-2 An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 32

33 Tuned/matched CP: birdcage rotating field B 1 + (1) Basic birdcage rotating mode (a=1, phi= angle position) in D.S. Normalization to produce a left handed 2D mean value H 1+ = 4.68 A/m in a target square [±20,±20,20]) (90 1ms square pulse) Combine a birdcage mode with amplitude a in a S-parameters task in DS, calculate left handed polarization H 1+ in [x,y] and evaluate the 2D mean-value in target square CP1_neg (a=8.8) CP1_neg (a=6.8) Normalized left handed H1+ in axial plane [z=20] for 'Ella_VF' (left) and 'Hum' (right) An 8-ch RF transmit coil for MRI at 7T/298MHz (X.H.,M.L.) CEA-DSM-Irfu-SACM 33

34 Tuned/matched CP: birdcage rotating field B 1 + (2) Normalized 90 1ms H 1 + in mid-axial and sagittal planes with 'Ella_VF' (top) and 'Hum' (bottom) An 8-ch RF transmit coil for MRI at 7T/298MHz (X.H.,M.L.) CEA-DSM-Irfu-SACM 34

35 Tuned/matched CP: PLD and SAR_10g (3) PLD (left) and SAR_10g (right) for 'Ella_VF' (top) and 'Hum' (bottom) in axial plane [z=0] An 8-ch RF transmit coil for MRI at 7T/298MHz (X.H.,M.L.) CEA-DSM-Irfu-SACM 35

36 Tuned/matched CP: PLD and SAR_10g (4) PLD (left) and SAR_10g (right) for 'Ella_VF' (top) and 'Hum' (bottom) in sagittal plane An 8-ch RF transmit coil for MRI at 7T/298MHz (X.H.,M.L.) CEA-DSM-Irfu-SACM 36

37 Conclusion Full CAD model simulation for RF coil Dissipative elements Superposition of thin strips elements Integrated physical pre-matching system Above all, no element aligned with Cartesian grids (PBA) dispersion of the dipoles resonant frequencies tuning/matching circuit is essential Small mesh steps, small time steps, low decay, multi-channel prohibitive calculation time GPU option is required Two kind of solver are necessary (FEM, FIT) Convergence of the simulations results FEM/FIT (sphere, Hum) High res. anatomical model only needed for local investigation An 8-ch RF transceive coil for MRI at 7T/298MHz X. Hanus CEA-DSM-Irfu-SACM 37

Introduction to antenna and near-field simulation in CST Microwave Studio software

Introduction to antenna and near-field simulation in CST Microwave Studio software Lisbon, IT, 22 March 2010 Introduction to antenna and near-field simulation in CST Microwave Studio software Jorge R. Costa Jerzy Guterman 2005, it - instituto de telecomunicações. Todos os direitos reservados.

More information

Simulation of Mobile Phone Antenna Performance

Simulation of Mobile Phone Antenna Performance Tough technical requirements are being put on handsets. Mobile phones have to deal with an ever increasing number of services, while at the same time the cost of the systems is being reduced. RD in the

More information

SAR Distribution in Test Animals Exposed to RF Radiation

SAR Distribution in Test Animals Exposed to RF Radiation German Mobile Telecommunication Research Programme, July 25th, 2006 SAR Distribution in Test Animals Exposed to RF Radiation Verónica Berdiñas Torres, Andreas Christ, Niels Kuster IT IS Foundation, ETH

More information

Today s handsets have to meet tough ELECTROMAGNETIC SIMULATION OF MOBILE PHONE ANTENNA PERFORMANCE

Today s handsets have to meet tough ELECTROMAGNETIC SIMULATION OF MOBILE PHONE ANTENNA PERFORMANCE ELECTROMAGNETIC SIMULATION OF MOBILE PHONE ANTENNA PERFORMANCE The telecommunications sector is making great advances aimed at delivering an even stream of high-tech devices, covering the significant consumer

More information

EH-20 20m antenna. By VE3RGW

EH-20 20m antenna. By VE3RGW EH-20 20m antenna By VE3RGW Equivalent circuit of EH-20 (prototype 2A) antenna system. Upper cylinder Lower cylinder Ground Counter pose Phasing coil Impedance transformer and tune circuit Tune coil Feed

More information

Complete Technology and RFID

Complete Technology and RFID UGM 2007 Complete Technology and RFID Overview Operating Principles Inductive Coupling Microwave Coupling Coupling to Circuit Simmulation Summary T. Wittig 1 twi, apr / v2.0 / 12. Jun 2007 Overview Radio

More information

Co-simulation of Microwave Networks. Sanghoon Shin, Ph.D. RS Microwave

Co-simulation of Microwave Networks. Sanghoon Shin, Ph.D. RS Microwave Co-simulation of Microwave Networks Sanghoon Shin, Ph.D. RS Microwave Outline Brief review of EM solvers 2D and 3D EM simulators Technical Tips for EM solvers Co-simulated Examples of RF filters and Diplexer

More information

ANALYSIS AND VERIFICATION OF A PROPOSED ANTENNA DESIGN FOR AN IMPLANTABLE. RFID TAG AT 915 MHz RAHUL BAKORE

ANALYSIS AND VERIFICATION OF A PROPOSED ANTENNA DESIGN FOR AN IMPLANTABLE. RFID TAG AT 915 MHz RAHUL BAKORE ANALYSIS AND VERIFICATION OF A PROPOSED ANTENNA DESIGN FOR AN IMPLANTABLE RFID TAG AT 915 MHz By RAHUL BAKORE Bachelor of Engineering in Electronics and Communication University Of Rajasthan Jaipur, Rajasthan,

More information

Vector Network Analyzer Techniques to Measure WR340 Waveguide Windows

Vector Network Analyzer Techniques to Measure WR340 Waveguide Windows LS-296 Vector Network Analyzer Techniques to Measure WR340 Waveguide Windows T. L. Smith ASD / RF Group Advanced Photon Source Argonne National Laboratory June 26, 2002 Table of Contents 1) Introduction

More information

RICHARD T ELL ASSOCIATES,INC.

RICHARD T ELL ASSOCIATES,INC. RICHARD T ELL ASSOCIATES,INC. An Evaluation of Test Measurement Data Obtained on the KW-Gard RF Protective Suit March 30, 1998 Prepared for Euclid Garment Manufacturing Company 333 Martinel Drive Kent,

More information

Hardware Acceleration for CST MICROWAVE STUDIO

Hardware Acceleration for CST MICROWAVE STUDIO Hardware Acceleration for CST MICROWAVE STUDIO Chris Mason Product Manager Amy Dewis Channel Manager Agenda 1. Introduction 2. Why use Hardware Acceleration? 3. Hardware Acceleration Technologies 4. Current

More information

VBA Macro for construction of an EM 3D model of a tyre and part of the vehicle

VBA Macro for construction of an EM 3D model of a tyre and part of the vehicle VBA Macro for construction of an EM 3D model of a tyre and part of the vehicle Guillermo Vietti, Gianluca Dassano, Mario Orefice LACE, Politecnico di Torino, Turin, Italy. [email protected] Work

More information

A FULL-WAVE ANALYSIS OF HIGH GAIN RADIAL LINE SLOT ANTENNAS USING CST STUDIO SUITE

A FULL-WAVE ANALYSIS OF HIGH GAIN RADIAL LINE SLOT ANTENNAS USING CST STUDIO SUITE Munich Airport Marriott Hotel, 17-19 May 2011 6th EUROPEAN USER GROUP MEETING A FULL-WAVE ANALYSIS OF HIGH GAIN RADIAL LINE SLOT ANTENNAS USING CST STUDIO SUITE Simone Ledda, Matteo Cerretelli, Guido Biffi

More information

Power Rating Simulation of the new QNS connector generation

Power Rating Simulation of the new QNS connector generation Power Rating Simulation of the new QNS connector generation IMS Connector Systems is an international, technology driven company specialized in development and production of high frequency connections.

More information

Solutions Components Products Services IMST THE MORE EFFECTIVE 3D-EM SIMULATION TOOL. EMPIRE XCcel

Solutions Components Products Services IMST THE MORE EFFECTIVE 3D-EM SIMULATION TOOL. EMPIRE XCcel THE MORE EFFECTIVE 3D-EM SIMULATION TOOL EMPIRE XCcel 2 3 EMPIRE XCcel s applicability ranges from analyzing planar, multi-layered and conformal circuits, components and antennas to multi-pin packages,

More information

RF measurements, tools and equipment E. B. Boskamp, A. Nabetani, J. Tropp ([email protected])

RF measurements, tools and equipment E. B. Boskamp, A. Nabetani, J. Tropp (eddy.boskamp@med.ge.com) RF measurements, tools and equipment E. B. Boskamp, A. Nabetani, J. Tropp ([email protected]) INTRODUCTION I am often asked by researchers what kind of equipment is needed to set up an RF lab. The

More information

Simulation électromagnétique 3D et câblage, exemples dans l'automobile et aéronautique :

Simulation électromagnétique 3D et câblage, exemples dans l'automobile et aéronautique : Simulation électromagnétique 3D et câblage, exemples dans l'automobile et aéronautique : CST, Christophe Morin 1 www.cst.com Agenda - Présentation CST - Simulation câblage dans modèle 3D - Exemples automobile

More information

Numerical Calculation of Beam Coupling Impedances in the Frequency Domain using the Finite Integration Technique

Numerical Calculation of Beam Coupling Impedances in the Frequency Domain using the Finite Integration Technique Numerical Calculation of Beam Coupling Impedances in the Frequency Domain using the Finite Integration Technique Uwe Niedermayer and Oliver Boine-Frankenheim 24 August 2012 TU Darmstadt Fachbereich 18

More information

Magnetic Field Generation for MRI:

Magnetic Field Generation for MRI: Magnetic Field Generation for MRI: State of the art and future challenges. Pierre Védrine, CEA Saclay, Irfu 1 Medical Imaging Superconducting Magnet for MRI Objectives and challenges for high field MRI

More information

Operating Frequency Selection for Loosely Coupled Wireless Power Transfer Systems with Respect to RF Emissions and RF Exposure Requirements

Operating Frequency Selection for Loosely Coupled Wireless Power Transfer Systems with Respect to RF Emissions and RF Exposure Requirements Operating Frequency Selection for Loosely Coupled Wireless Power Transfer Systems with Respect to RF Emissions and RF Exposure Requirements Jagadish Nadakuduti, Lin Lu, Paul Guckian Qualcomm Technologies,

More information

Numerical Methods and Software Tools for Simulation, Design, and Resonant Mode Analysis of Radio Frequency Birdcage Coils Used in MRI

Numerical Methods and Software Tools for Simulation, Design, and Resonant Mode Analysis of Radio Frequency Birdcage Coils Used in MRI Numerical Methods and Software Tools for Simulation, Design, and Resonant Mode Analysis of Radio Frequency Birdcage Coils Used in MRI NECIP GURLER, YUSUF ZIYA IDER Department of Electrical and Electronics

More information

Minimizing crosstalk in a high-speed cable-connector assembly.

Minimizing crosstalk in a high-speed cable-connector assembly. Minimizing crosstalk in a high-speed cable-connector assembly. Evans, B.J. Calvo Giraldo, E. Motos Lopez, T. CERN, 1211 Geneva 23, Switzerland [email protected] [email protected] [email protected]

More information

Calculation of Eigenmodes in Superconducting Cavities

Calculation of Eigenmodes in Superconducting Cavities Calculation of Eigenmodes in Superconducting Cavities W. Ackermann, C. Liu, W.F.O. Müller, T. Weiland Institut für Theorie Elektromagnetischer Felder, Technische Universität Darmstadt Status Meeting December

More information

Software for Design NMR Probes Using the Shielded Split Ring and the Shielded Symmetrical Band Resonators

Software for Design NMR Probes Using the Shielded Split Ring and the Shielded Symmetrical Band Resonators Software for Design NMR Probes Using the Shielded Split Ring and the Shielded Symmetrical Band Resonators Nasreddine Benahmed University of Tlemcen, Algeria ABSTRACT This article presents a software (NMR

More information

Embedded FM/TV Antenna System

Embedded FM/TV Antenna System 1 Embedded FM/TV Antenna System Final Report Prepared for By January 21, 2011 2 Table of Contents 1 Introduction... 5 2 Technical Specification... 6 3 Prototype Antenna... 7 4 FASTROAD Active module fabrication...

More information

Design of 2D waveguide networks for the study of fundamental properties of Quantum Graphs

Design of 2D waveguide networks for the study of fundamental properties of Quantum Graphs Design of 2D waveguide networks for the study of fundamental properties of Quantum Graphs Introduction: what is a quantum graph? Areas of application of quantum graphs Motivation of our experiment Experimental

More information

5 Factors Affecting the Signal-to-Noise Ratio

5 Factors Affecting the Signal-to-Noise Ratio 5 Factors Affecting the Signal-to-Noise Ratio 29 5 Factors Affecting the Signal-to-Noise Ratio In the preceding chapters we have learned how an MR signal is generated and how the collected signal is processed

More information

Tuning a Monopole Antenna Using a Network Analyzer

Tuning a Monopole Antenna Using a Network Analyzer 11/21/11 Tuning a Monopole Antenna Using a Network Analyzer Chris Leonard Executive Summary: When designing a monopole antenna it is important to know at which frequency the antenna will be operating at.

More information

Simulation Techniques for Tablet and Mobile Phone Design Bill McGinn; Ansys Senior Application Engineer

Simulation Techniques for Tablet and Mobile Phone Design Bill McGinn; Ansys Senior Application Engineer Simulation Techniques for Tablet and Mobile Phone Design Bill McGinn; Ansys Senior Application Engineer 1 Tablets in our daily lives Tablets are very entertaining, stylish and powerful Shopping, reading,

More information

Preface Acknowledgments Acronyms

Preface Acknowledgments Acronyms Contents Preface Acknowledgments Acronyms xi xiii xv 1 Introduction 1 1.1 The history of Antennas and Antenna Analysis 1 1.2 Antenna Synthesis 5 1.3 Approximate Antenna Modeling 7 1.4 Organization of the

More information

MINIMUM USAGE OF FERRITE TILES IN ANECHOIC CHAMBERS

MINIMUM USAGE OF FERRITE TILES IN ANECHOIC CHAMBERS Progress In Electromagnetics Research B, Vol. 19, 367 383, 2010 MINIMUM USAGE OF FERRITE TILES IN ANECHOIC CHAMBERS S. M. J. Razavi, M. Khalaj-Amirhosseini, and A. Cheldavi College of Electrical Engineering

More information

Forum R.F.& Wireless, Roma il 21 Ottobre 2008 Dr. Emmanuel Leroux Country Manager for Italy [email protected] 340 3768950

Forum R.F.& Wireless, Roma il 21 Ottobre 2008 Dr. Emmanuel Leroux Country Manager for Italy emmanuel.leroux@cst.com 340 3768950 Simulazione 3D elettromagnetica Time e Frequency domain Forum R.F.& Wireless, Roma il 21 Ottobre 2008 Dr. Emmanuel Leroux Country Manager for Italy [email protected] 340 3768950 1 Agenda CST company

More information

SIW 2D PLANAR ARRAY WITH FOUR CROSS SLOTS RADIATOR AND TUNING VIAS

SIW 2D PLANAR ARRAY WITH FOUR CROSS SLOTS RADIATOR AND TUNING VIAS Progress In Electromagnetics Research C, Vol. 40, 83 92, 2013 SIW 2D PLANAR ARRAY WITH FOUR CROSS SLOTS RADIATOR AND TUNING VIAS P. Sanchez-Olivares, J. L. Masa-Campos *, J. A. Ruiz-Cruz, and B. Taha-Ahmed

More information

An octave bandwidth dipole antenna

An octave bandwidth dipole antenna An octave bandwidth dipole antenna Abstract: Achieving wideband performance from resonant structures is challenging because their radiation properties and impedance characteristics are usually sensitive

More information

Evaluating Cell Phone and Personal Communications Equipment and their EMC Effects on Automotive Audio and In-Cabin Modules

Evaluating Cell Phone and Personal Communications Equipment and their EMC Effects on Automotive Audio and In-Cabin Modules Evaluating Cell Phone and Personal Communications Equipment and their EMC Effects on Automotive Audio and In-Cabin Modules Craig W. Fanning Elite Electronic Engineering, Inc. 1516 Centre Circle Downers

More information

RADIATION PATTERNS. The half-power (-3 db) beamwidth is a measure of the directivity of the antenna.

RADIATION PATTERNS. The half-power (-3 db) beamwidth is a measure of the directivity of the antenna. RADIATION PATTERNS The radiation pattern is a graphical depiction of the relative field strength transmitted from or received by the antenna. Antenna radiation patterns are taken at one frequency, one

More information

Trace Layer Import for Printed Circuit Boards Under Icepak

Trace Layer Import for Printed Circuit Boards Under Icepak Tutorial 13. Trace Layer Import for Printed Circuit Boards Under Icepak Introduction: A printed circuit board (PCB) is generally a multi-layered board made of dielectric material and several layers of

More information

Engineering Sciences 151. Electromagnetic Communication Laboratory Assignment 3 Fall Term 1998-99

Engineering Sciences 151. Electromagnetic Communication Laboratory Assignment 3 Fall Term 1998-99 Engineering Sciences 151 Electromagnetic Communication Laboratory Assignment 3 Fall Term 1998-99 WAVE PROPAGATION II: HIGH FREQUENCY SLOTTED LINE AND REFLECTOMETER MEASUREMENTS OBJECTIVES: To build greater

More information

How To Design An Ism Band Antenna For 915Mhz/2.4Ghz Ism Bands On A Pbbb (Bcm) Board

How To Design An Ism Band Antenna For 915Mhz/2.4Ghz Ism Bands On A Pbbb (Bcm) Board APPLICATION NOTE Features AT09567: ISM Band PCB Antenna Reference Design Atmel Wireless Compact PCB antennas for 915MHz and 2.4GHz ISM bands Easy to integrate Altium design files and gerber files Return

More information

Cable Analysis and Fault Detection using the Bode 100

Cable Analysis and Fault Detection using the Bode 100 Cable Analysis and Fault Detection using the Bode 100 By Stephan Synkule 2014 by OMICRON Lab V1.3 Visit www.omicron-lab.com for more information. Contact [email protected] for technical support.

More information

Effects of Mobile Phone Radiation onto Human Head with Variation of Holding Cheek and Tilt Positions

Effects of Mobile Phone Radiation onto Human Head with Variation of Holding Cheek and Tilt Positions Effects of Mobile Phone Radiation onto Human Head with Variation of Holding Cheek and Tilt Positions M. R. Iqbal-Faruque* 1, N. Aisyah-Husni 2, Md. Ikbal-Hossain 1, M. Tariqul-Islam 2 and N. Misran 2 1

More information

R3765/67 CG Network Analyzer

R3765/67 CG Network Analyzer R3765/67 CG Network Analyzer RSE 05.03.02 1 R376XG Series Overview R3765 300kHz ~ 3.8 GHz R3767 300kHz ~ 8 GHz AG BG Basic model Built-in Bridge A/R & B/R Transmission Reflection CG Built-in S-parameter

More information

A wave lab inside a coaxial cable

A wave lab inside a coaxial cable INSTITUTE OF PHYSICS PUBLISHING Eur. J. Phys. 25 (2004) 581 591 EUROPEAN JOURNAL OF PHYSICS PII: S0143-0807(04)76273-X A wave lab inside a coaxial cable JoãoMSerra,MiguelCBrito,JMaiaAlves and A M Vallera

More information

EVALUATION OF SAR AND TEMPERATURE ELEVATION IN A MULTI-LAYERED HUMAN HEAD MODEL EXPOSED TO RF RADIATION. By Ayman Ibrahim Sabbah

EVALUATION OF SAR AND TEMPERATURE ELEVATION IN A MULTI-LAYERED HUMAN HEAD MODEL EXPOSED TO RF RADIATION. By Ayman Ibrahim Sabbah EVALUATION OF SAR AND TEMPERATURE ELEVATION IN A MULTI-LAYERED HUMAN HEAD MODEL EXPOSED TO RF RADIATION By Ayman Ibrahim Sabbah Advisor Prof. Nihad Ibrahim Dib Co-Advisor Prof. Moh d Ahmed Al-Nimr Thesis

More information

Antenna Trainer EAN. www.edibon.com. Technical Teaching Equipment INTRODUCTION

Antenna Trainer EAN. www.edibon.com. Technical Teaching Equipment INTRODUCTION Antenna Trainer EAN Technical Teaching Equipment Products Products range Units 3.-Communications INTRODUCTION Antennas are the main element of aerial communications. They are the transition between a transmission

More information

CREOL, College of Optics & Photonics, University of Central Florida

CREOL, College of Optics & Photonics, University of Central Florida OSE6650 - Optical Properties of Nanostructured Materials Optical Properties of Nanostructured Materials Fall 2013 Class 3 slide 1 Challenge: excite and detect the near field Thus far: Nanostructured materials

More information

Selecting Receiving Antennas for Radio Tracking

Selecting Receiving Antennas for Radio Tracking Selecting Receiving Antennas for Radio Tracking Larry B Kuechle, Advanced Telemetry Systems, Inc. Isanti, Minnesota 55040 [email protected] The receiving antenna is an integral part of any radio location

More information

Antenna Properties and their impact on Wireless System Performance. Dr. Steven R. Best. Cushcraft Corporation 48 Perimeter Road Manchester, NH 03013

Antenna Properties and their impact on Wireless System Performance. Dr. Steven R. Best. Cushcraft Corporation 48 Perimeter Road Manchester, NH 03013 Antenna Properties and their impact on Wireless System Performance Dr. Steven R. Best Cushcraft Corporation 48 Perimeter Road Manchester, NH 03013 Phone (603) 627-7877 FAX: (603) 627-1764 Email: [email protected]

More information

An equivalent circuit of a loop antenna.

An equivalent circuit of a loop antenna. 3.2.1. Circuit Modeling: Loop Impedance A loop antenna can be represented by a lumped circuit when its dimension is small with respect to a wavelength. In this representation, the circuit parameters (generally

More information

CHAPTER4 GENERAL ASPECTS OF MUTUAL

CHAPTER4 GENERAL ASPECTS OF MUTUAL CHAPTER4 GENERAL ASPECTS OF MUTUAL ADMITTANCE OF CPW-FED TWIN SLOTS ON CONDUCTOR-BACKED TWO-LAYER SUBSTRATES 4.1 INTRODUCTORY REMARKS The present chapter is concerned with an exploratory investigation

More information

Investigations on Critical Higher Order Modes in CEBAF Upgrade Cavities

Investigations on Critical Higher Order Modes in CEBAF Upgrade Cavities Investigations on Critical Higher Order Modes in CEBAF Upgrade Cavities F. Marhauser Thanks also to H. Wang and K. Tian 27. August 2009 How HOMs are excited and why they are important - Wakefields- some

More information

How To Simulate An Antenna On A Computer Or Cell Phone

How To Simulate An Antenna On A Computer Or Cell Phone 1 Antennas Complete Technology for Antenna Simulation Edoardo Genovese, CST AG [email protected] www.cst.com CST workshop series 2010 February 10 1 About CST founded in 1992 160 employees world-wide

More information

Applications in EMC testing. Outline. Antennas for EMC Testing. Terminology

Applications in EMC testing. Outline. Antennas for EMC Testing. Terminology Antennas for EMC Testing Zhong Chen ETS-Lindgren 1301 Arrow Point Drive Cedar Park, TX 78613 [email protected] Outline EMC Terms and Definitions Typical EMC Antennas Calibration of EMC Antennas

More information

Wireless Power Transfer System Design. Julius Saitz ANSYS

Wireless Power Transfer System Design. Julius Saitz ANSYS Wireless Power Transfer System Design Julius Saitz ANSYS 1 WPT System 2 Wireless Power Transfer (WPT) Near-Field (Inductive coupling, resonant) Do not rely on propagating EM waves Operate at distances

More information

Quad-Band U-Slot Antenna for Mobile Applications

Quad-Band U-Slot Antenna for Mobile Applications 22 E. HERAS, Z. RAIDA, R. LAMADRID, QUAD-BAND U-SLOT ANTENNA FOR MOBILE APPLICATIONS Quad-Band U-Slot Antenna for Mobile Applications Eduardo de las HERAS PALMERO, Zbyněk RAIDA, Roberto LAMADRID RUIZ Dept.

More information

CONCEPT-II. Overview of demo examples

CONCEPT-II. Overview of demo examples CONCEPT-II CONCEPT-II is a frequency domain method of moment (MoM) code, under development at the Institute of Electromagnetic Theory at the Technische Universität Hamburg-Harburg (www.tet.tuhh.de). Overview

More information

Module 13 : Measurements on Fiber Optic Systems

Module 13 : Measurements on Fiber Optic Systems Module 13 : Measurements on Fiber Optic Systems Lecture : Measurements on Fiber Optic Systems Objectives In this lecture you will learn the following Measurements on Fiber Optic Systems Attenuation (Loss)

More information

Numerical Computation of the Combined Specific Absorption Rates Induced in Human Head due to Multiple Independent Sources

Numerical Computation of the Combined Specific Absorption Rates Induced in Human Head due to Multiple Independent Sources International Journal of Electromagnetics and Applications 2015, 5(2): 73-79 DOI: 10.5923/j.ijea.20150502.01 Numerical Computation of the Combined Specific Absorption Rates Induced in Human Head due to

More information

Forum R.F.& Wireless, Milano il 14 Febbraio 2008 Dr. Emmanuel Leroux Technical Sales Manager for Italy [email protected] 0039 340 3768950

Forum R.F.& Wireless, Milano il 14 Febbraio 2008 Dr. Emmanuel Leroux Technical Sales Manager for Italy emmanuel.leroux@cst.com 0039 340 3768950 Simulazione 3D elettromagnetica Time e Frequency domain Forum R.F.& Wireless, Milano il 14 Febbraio 2008 Dr. Emmanuel Leroux Technical Sales Manager for Italy [email protected] 0039 340 3768950 1

More information

For many years the general public

For many years the general public David Seabury, ETS-Lindgren An Update On SAR Standards And The Basic Requirements For SAR Assessment For many years the general public has been concerned about the possible health effects of exposure to

More information

Compact Integrated Antennas

Compact Integrated Antennas Freescale Semiconductor, Inc. Application Note Document Number: AN2731 Rev. 3, 09/2015 Compact Integrated Antennas Designs and Applications for the MC1321x, MC1322x, MC1323x, and MKW40/30/20 1 Introduction

More information

Perturbation of near-field scan from connected cables Sørensen, Morten; Franek, Ondrej; Pedersen, Gert F.; Baltsen, Knud A.

Perturbation of near-field scan from connected cables Sørensen, Morten; Franek, Ondrej; Pedersen, Gert F.; Baltsen, Knud A. Aalborg Universitet Perturbation of near-field scan from connected cables Sørensen, Morten; Franek, Ondrej; Pedersen, Gert F.; Baltsen, Knud A.; Ebert, Hans Published in: 2012 IEEE International Symposium

More information

Printed Dipole Array Fed with Parallel Stripline for Ku-band Applications

Printed Dipole Array Fed with Parallel Stripline for Ku-band Applications Printed Dipole Array Fed with Parallel Stripline for Ku-band Applications M. Dogan 1, 3,K. Özsoy 1, 2, and I.Tekin 1, 1 Electronics Engineering, Sabanci University, Istanbul, Turkey 2 Vestek Electronic

More information

RF FRONT END FOR HIGH BANDWIDTH BUNCH ARRIVAL TIME MONITORS IN FREE-ELECTRON LASERS AT DESY

RF FRONT END FOR HIGH BANDWIDTH BUNCH ARRIVAL TIME MONITORS IN FREE-ELECTRON LASERS AT DESY Proceedings of IBIC212, Tsukuba, Japan RF FRONT END FOR HIGH BANDWIDTH BUNCH ARRIVAL TIME MONITORS IN FREE-ELECTRON LASERS AT DESY A. Penirschke #, A. Angelovski, M. Hansli, R. Jakoby, Institut für Mikrowellentechnik

More information

READER COMPONENTS. mifare (14443A) 13.56 MHz RFID Proximity Antennas. November 2002. Revision 1.0 PUBLIC. Philips Semiconductors

READER COMPONENTS. mifare (14443A) 13.56 MHz RFID Proximity Antennas. November 2002. Revision 1.0 PUBLIC. Philips Semiconductors READER COMPONENTS mifare (14443A) 13.56 MHz RFID Proximity Antennas Revision 1.0 PUBLIC November 00 Philips Semiconductors Philips Semiconductors Rev. 1.0 November 00 CONTENTS 1 INTRODUCTION... 3 1.1 Purpose

More information

National Laboratory of Antennas and Microwave Technology Xidian University Xi an, Shaanxi 710071, China

National Laboratory of Antennas and Microwave Technology Xidian University Xi an, Shaanxi 710071, China Progress In Electromagnetics Research, PIER 76, 237 242, 2007 A BROADBAND CPW-FED T-SHAPE SLOT ANTENNA J.-J. Jiao, G. Zhao, F.-S. Zhang, H.-W. Yuan, and Y.-C. Jiao National Laboratory of Antennas and Microwave

More information

FDA Guidelines for Magnetic Resonance Equipment Safety

FDA Guidelines for Magnetic Resonance Equipment Safety FDA Guidelines for Magnetic Resonance Equipment Safety Loren A. Zaremba, Ph.D. Center for Devices and Radiological Health Food and Drug Administration Outline I. Introduction II. Static Magnetic Field

More information

IEC TC106. Standards for the Assessment of Human Exposure to Electric, Magnetic, and Electromagnetic Fields, 0 to 300 GHz

IEC TC106. Standards for the Assessment of Human Exposure to Electric, Magnetic, and Electromagnetic Fields, 0 to 300 GHz International Electrotechnical Commission IEC TC106 Standards for the Assessment of Human Exposure to Electric, Magnetic, and Electromagnetic Fields, 0 to 300 GHz R. C. Petersen Chairman Secretariat and

More information

Finite Difference Time Domain and BPM: Flexible Algorithm Selection Technology

Finite Difference Time Domain and BPM: Flexible Algorithm Selection Technology Finite Difference Time Domain and BPM: Flexible Algorithm Selection Technology 1. Introduction This application note shows the use of the Finite Difference Time Domain (FDTD) module in the calculation

More information

Effects of Cell Phone Radiation on the Head. BEE 4530 Computer-Aided Engineering: Applications to Biomedical Processes

Effects of Cell Phone Radiation on the Head. BEE 4530 Computer-Aided Engineering: Applications to Biomedical Processes Effects of Cell Phone Radiation on the Head BEE 4530 Computer-Aided Engineering: Applications to Biomedical Processes Group 3 Angela Cai Youjin Cho Mytien Nguyen Praveen Polamraju Table of Contents I.

More information

The BESSY HOM Damped Cavity with Ferrite Absorbers. Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides

The BESSY HOM Damped Cavity with Ferrite Absorbers. Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides The BESSY HOM Damped Cavity with Ferrite Absorbers E. Weihreter / BESSY Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides Design of a ferrite loaded ridged circular waveguide

More information

Analysis of the G3LTF Dual Band Feed for 23cm and 13cm Paul Wade W1GHZ 2004 [email protected]

Analysis of the G3LTF Dual Band Feed for 23cm and 13cm Paul Wade W1GHZ 2004 w1ghz@arrl.net Analysis of the G3LTF Dual Band Feed for 23cm and 13cm Paul Wade W1GHZ 2004 [email protected] In the March 2004 edition of the RSGB Microwave Newsletter, G3LTF described 1 a dual band feed for the 23 cm and

More information

Coaxial Cable Feeder Influence on Yagi Antenna Dragoslav Dobričić, YU1AW [email protected]

Coaxial Cable Feeder Influence on Yagi Antenna Dragoslav Dobričić, YU1AW dragan@antennex.com Coaxial Cable Feeder Influence on Yagi Antenna Dragoslav Dobričić, YU1AW [email protected] Introduction o far, in several previous articles [1, 2, 3], we investigated how boom radius and its S distance

More information

Current Probes. User Manual

Current Probes. User Manual Current Probes User Manual ETS-Lindgren L.P. reserves the right to make changes to any product described herein in order to improve function, design, or for any other reason. Nothing contained herein shall

More information

a leap ahead in analog

a leap ahead in analog EMV Contactless Payment Systems based on AS3911 Overview and System Simulations Giuliano Manzi, PhD Mannheim, May 23 25, 2012 CST EUROPEAN USER CONFERENCE 2012 a leap ahead in analog OUTLINE AS3911 OVERVIEW

More information

Pre-Compliance Test Method for Radiated Emissions of Automotive Components Using Scattering Parameter Transfer Functions

Pre-Compliance Test Method for Radiated Emissions of Automotive Components Using Scattering Parameter Transfer Functions PreCompliance Test Method for Radiated Emissions of Automotive Components Using Scattering Parameter Transfer Functions D. Schneider 1*, S. Tenbohlen 1, W. Köhler 1 1 Institute of Power Transmission and

More information

Shielding Effectiveness Test Method. Harbour s LL, SB, and SS Coaxial Cables. Designs for Improved Shielding Effectiveness

Shielding Effectiveness Test Method. Harbour s LL, SB, and SS Coaxial Cables. Designs for Improved Shielding Effectiveness Shielding Effectiveness Test Method Harbour s LL, SB, and SS Coaxial Cables Designs for Improved Shielding Effectiveness Harbour Industries 4744 Shelburne Road Shelburne Vermont 05482 USA 802-985-3311

More information

Numerical Modelling of E-M Occupational Exposures associated with MRI

Numerical Modelling of E-M Occupational Exposures associated with MRI Numerical Modelling of E-M Occupational Exposures associated with MRI Jeff Hand and Yan Li Imaging Sciences Dept, Imperial College London, Hammersmith Hospital Campus Physical Agents Directive (EMFs) 2004/40/EC

More information

Broadband Slotted Coaxial Broadcast Antenna Technology

Broadband Slotted Coaxial Broadcast Antenna Technology Broadband Slotted Coaxial Broadcast Antenna Technology Summary Slotted coaxial antennas have many advantages over traditional broadband panel antennas including much smaller size and wind load, higher

More information

Copyright 1996 IEEE. Reprinted from IEEE MTT-S International Microwave Symposium 1996

Copyright 1996 IEEE. Reprinted from IEEE MTT-S International Microwave Symposium 1996 Copyright 1996 IEEE Reprinted from IEEE MTT-S International Microwave Symposium 1996 This material is posted here with permission of the IEEE. Such permission of the IEEE does not in any way imply IEEE

More information

Breast MRI Quality Control

Breast MRI Quality Control Donna M. Reeve, MS, DABR, DABMP Department of Imaging Physics Educational Objectives Discuss the importance of breast MRI quality control (QC). Provide an overview of the new ACR Breast MRI Accreditation

More information

AVR2006: Design and characterization of the Radio Controller Board's 2.4GHz PCB Antenna. Application Note. Features.

AVR2006: Design and characterization of the Radio Controller Board's 2.4GHz PCB Antenna. Application Note. Features. AVR26: Design and characterization of the Radio Controller Board's 2.4GHz PCB Antenna Features Radiation pattern Impedance measurements WIPL design files NEC model Application Note 1 Introduction This

More information

Franz Hirtenfelder and Stephen Murray, CST Computer Simulation Technology and W. L. Gore and Associates (Gore) March 5, 2015

Franz Hirtenfelder and Stephen Murray, CST Computer Simulation Technology and W. L. Gore and Associates (Gore) March 5, 2015 1 of 7 3/17/2015 9:38 AM Home Franz Hirtenfelder and Stephen Murray, CST Computer Simulation Technology and W. L. Gore and Associates (Gore) March 5, 2015 Editor s Note: A cable that leaks electromagnetic

More information

Design and Certification of ASH Radio Systems for Japan

Design and Certification of ASH Radio Systems for Japan Design and Certification of ASH Radio Systems for Japan RFM s second-generation ASH radio hybrids are being used in a wide variety of applications in Japan, operating under the Japanese BIJAKU radio regulations.

More information

Human Exposure to Outdoor PLC System

Human Exposure to Outdoor PLC System 1602 PIERS Proceedings, Marrakesh, MOROCCO, March 20 23, 2011 Human Exposure to Outdoor PLC System Vicko Doric 1, Dragan Poljak 1, and Khalil El Khamlichi Drissi 2 1 University of Split, Croatia 2 Blaise

More information

Current Probes, More Useful Than You Think

Current Probes, More Useful Than You Think Current Probes, More Useful Than You Think Training and design help in most areas of Electrical Engineering Copyright 1998 Institute of Electrical and Electronics Engineers. Reprinted from the IEEE 1998

More information

EMC Expert System for Architecture Design

EMC Expert System for Architecture Design EMC Expert System for Architecture Design EMC Expert System for Architecture Design Marcel van Doorn [email protected] Philips Electromagnetics Competence Center High Tech Campus 26, 5656 AE

More information

Weekend Antennas No. 1 A Bobtail Curtain for 2m

Weekend Antennas No. 1 A Bobtail Curtain for 2m Weekend Antennas No. 1 A Bobtail Curtain for 2m Welcome to the first installment of my new column, which I hope will become a regular feature in Radio ZS. Each installment will present a practical and

More information

GE Medical Systems Training in Partnership. Module 8: IQ: Acquisition Time

GE Medical Systems Training in Partnership. Module 8: IQ: Acquisition Time Module 8: IQ: Acquisition Time IQ : Acquisition Time Objectives...Describe types of data acquisition modes....compute acquisition times for 2D and 3D scans. 2D Acquisitions The 2D mode acquires and reconstructs

More information

ANSYS for Tablet Computer Design

ANSYS for Tablet Computer Design ANSYS for Tablet Computer Design Steven G. Pytel, PhD. Signal Integrity Product Manager 1 Confidence by Design Chicago, IL June 14, 2012 Tablets in our daily lives Tablets are very entertaining, stylish

More information

EM Noise Mitigation in Circuit Boards and Cavities

EM Noise Mitigation in Circuit Boards and Cavities EM Noise Mitigation in Circuit Boards and Cavities Faculty (UMD): Omar M. Ramahi, Neil Goldsman and John Rodgers Visiting Professors (Finland): Fad Seydou Graduate Students (UMD): Xin Wu, Lin Li, Baharak

More information

Model 3140. BiConiLog Antenna MANUAL EMC TEST SYSTEMS, L.P. MARCH 2002 REV C PN 399258

Model 3140. BiConiLog Antenna MANUAL EMC TEST SYSTEMS, L.P. MARCH 2002 REV C PN 399258 Model 3140 BiConiLog Antenna MANUAL EMC TEST SYSTEMS, L.P. MARCH 2002 MODEL 3140 BICONILOG ANTENNA EMC Test Systems, L.P. reserves the right to make changes to any product described herein in order to

More information

2. The Vector Network Analyzer

2. The Vector Network Analyzer ECE 584 Laboratory Experiments 2. The Vector Network Analyzer Introduction: In this experiment we will learn to use a Vector Network Analyzer to measure the magnitude and phase of reflection and transmission

More information

Automotive Glass Antenna for Worldwide Cellular Phone Coverage

Automotive Glass Antenna for Worldwide Cellular Phone Coverage In cooperation with: Laboratorio Antenne e Microonde Automotive Glass Antenna for Worldwide Cellular Phone Coverage Author: M. Cerretelli, ASK Industries SpA & University of Florence (IT) Presenter: Simone

More information

Antenna Basic Concepts

Antenna Basic Concepts ANTENNA An antenna is a device to transmit and/or receive electromagnetic waves. Electromagnetic waves are often referred to as radio waves. Most antennas are resonant devices, which operate efficiently

More information