C63.19 SC8 WG3 meeting, March 26, 2007 Calibration values for dipole validations at new RF probe separation distance of 1.5cm PINS-C item 5.k Jagadish.

Slides:



Advertisements
Similar presentations
Generalized Method for the Determination of Wireless Device RF Interference Level ANSI C63.19 Working Group Submitted for discussion by Stephen Julstrom.
Advertisements

Hardware Design of a 1 GHz Amplifier and Initial Comparison with SimRF Application Note K. Wang, R. Ludwig, S. Bitar, S. Makarov Aug 21, 2011.
RF Modeling efforts on Ion Source at SNS Sung-Woo Lee.
Different Types of Antennas
Quantum System “ Ion flux fraction measurement system.
C63.19 Round Robin Test Plan (by Jim Turner; further editing by Steve Julstrom – 11/20/2009)
AGS CNI Update: Non-linear Corrections to Energy Loss in Si Dead Layer Outline Standard dead layer fitting technique Non-linear corrections Compare results.
A Conformal CPW Folded Slot Antenna Array Printed on a Kapton Substrate Masud A. Aziz Sayan Roy* Layne A. Berge Irfanullah Sanjay Nariyal Benjamin D. Braaten.
Laser Doppler Vibrometer tests Goran Skoro UKNF Meeting 7-8 January 2010 Imperial College London UKNF Target Studies Web Page:
A NEW PRINTED QUASI-LANDSTORFER ANTENNA
Miniature Antenna: Results and Proposed Work March 2008.
Doc.: IEEE /0630r0 Submission May 2015 Intel CorporationSlide 1 Verification of IEEE ad Channel Model for Enterprise Cubical Environment.
MICE RF Cavity Measurements Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory March 26, 2010 University of California, Riverside,
Status of the 201 MHz Cavity and Coupling Coil Module Steve Virostek Lawrence Berkeley National Laboratory MICE Video Conference March 10, 2004.
1 X-band Single Cell and T18_SLAC_2 Test Results at NLCTA Faya Wang Chris Adolphsen Jul
ECLOUD Calculations of Coherent Tune Shifts for the April 2007 Measurements - Thanks to Marco for clarifying the drift/dipole weighting - - Thanks to Gerry.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
University of Split, FESB Short Term Scientific Mission of COST 286 Beneficiary: Jacek Skrzypczynski, Wroclaw University of Technology Host: Vesna Roje,
Matching of molybdenum waveguide. Comparison of measurements and HFSS calculations for molybdenum waveguide, sigma_moly = 1.87e8 1/(Ohm-m) V.Dolgashev,
What is your Objective? THE PROBLEM  Curiosity???????? ???????? Observation is a key element here!!!
BA , 1 Principles of Acoustic Measurements Exercises: Basic Concepts of Sound Measuring Sound Measuring Sound in Practice Basic Frequency Analysis.
Swinging Pendulum Engineering Lab Background Info This activity shows the engineering importance of understanding the laws of mechanical energy. More.
STANDARDS AND COMPLIANCE TESTING P. Bernardi Department of Electronic Engineering - University of Rome "La Sapienza"
Full Wave Modeling of Body Area Path Loss and Related Antenna Modeling S. Makarov & G. Noetscher Ant. Lab ECE Dept., WPI, MA.
Update of the ground motion generator of A. Seryi for ATF2 thanks to ground motion measurements in the ATF2 beam line 1 Benoît BOLZONATF2 software task.
FractalComs Exploring the limits of Fractal Electrodynamics for the future telecommunication technologies INFORMATION SOCIETY TECHNOLOGIES (IST) PROGRAMME.
WG8 N 1673 Late DIN comment to FCD Ballot ISO/IEC /FPDAM8 = WG8 N 1638 (SC17 N 3836) Source:
PMP Progress Report Activities since GRPE 58 Heavy Duty Validation testing Exercise completed in October Draft report and draft proposal to insert PN measurement.
A SMALL PASSIVE UHF RFID TAG FOR METALLIC ITEM IDENTIFICATION Mun Leng Ng Auto-ID Adelaide School of Electrical & Electronic Engineering University.
Designing and Manufacturing Microstrip Antenna for Wireless Communication at 2.4 GHz Monday December 27, 2010 Presented for Undergraduate Thesis ByRachmansyah.
18/10/20151 Calibration of Input-Matching and its Center Frequency for an Inductively Degenerated Low Noise Amplifier Laboratory of Electronics and Information.
Near Field Antenna Measurements for Cellular Phone Certification Ahlia M. Tillman, John Rzasa, Bandar Hakim, Quirino Balzano, and Christopher C. Davis.
Measurement of Integrated PA-to-LNA Isolation on Si CMOS Chip Ryo Minami , JeeYoung Hong , Kenichi Okada , and Akira Matsuzawa Tokyo Institute of Technology,
UWB Antenna Ryan Clarke Roshini Karunaratne Chad Schrader Advisor: Ray Kwok.
1 CERN 1 Mar E-CLOUD Build-up in Grooved Chambers Marco Venturini Center for Beam Physics, LBNL ECL2 -- CERN, 1-2 March 2007.
Beam Pattern for a Single Slot Antenna Larry Isenhower Summer 2002.
S. Kahn 5 June 2003NuFact03 Tetra Cooling RingPage 1 Tetra Cooling Ring Steve Kahn For V. Balbekov, R. Fernow, S. Kahn, R. Raja, Z. Usubov.
1.3GHz Input Coupler for ILC
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
What is your Objective? THE PROBLEM  Curiosity???????? ???????? Observation is a key element here!!!
Modelling and testing of circuit protection of new superconducting magnets for the HL-LHC project 1 st Workshop FTEC 2015 Alejandro Fernandez Navarro.
Receive Antenna Performance Comparison. Receive Antenna Monitoring The receive antenna was installed in its permanent location inside the chamber A spectrum.
A TECHNICAL BRIEFING FOR AMATEUR RADIO OPERATORS
Remcom Inc. 315 S. Allen St., Suite 416  State College, PA  USA Tel:  Fax:   ©
700 MHz Taskgroup Update Last Call July 28 th Issues discussed MHz Dipole Antenna Calibration issues - Articulated Weighing Factors - Modulations.
Ciro Bigongiari, Salvatore Mangano, Results of the optical properties of sea water with the OB system.
Limits of space loss calculations. Near Field / Far Field Far field implies a plane wave. A plane wave is an asymptotic extrapolation of a spherical.
Warm linac simulations (DTL) and errors analysis M. Comunian F. Grespan.
ANTENNA THEORY ANALYSIS AND DESIGN Chapter.2 Problem
1 John McCloskey NASA/GSFC Chief EMC Engineer Code 565 Building 29, room Fundamentals of EMC Dipole Antenna.
Ferrite measurements of Mu2e AC dipole Summer Student Meeting August 25, 2010 Student: Evgeny Bulushev, NSU Supervisor: George Velev, TD\Magnet Systems.
Design of small directive antennas for IoT Habib Mariam Luvuezo Holldry July, 2017.
Hala Esawi Hana Masri Shorouq Abu Assab Supervised by: Dr.Yousef Dama
HPRFM-2013 Simulation Studies on a 10 kW CW Magnetron for Industrial Application   S.K. Vyas, N Shekhawat, S Maurya, V.V.P. Singh MWT Division, Central.
Effective Interest Calculations
CSE598A Analog Mixed Signal CMOS Chip Design
MTUCI DRM- signal protection ratios for several unwanted signals. Researches and MW air tests. Защитные отношения в системе DRM при нескольких мешающих.
Update of CLIC accelerating structure design
2017 Exploration & Production Winter Standards Meeting
Example: calculate the electric field at the electron’s distance away from the proton in a hydrogen atom (5.3x10-11 m). +e -e EP + - D This is the magnitude.
Bunch Tiltmeter Steve Smith SLAC Snowmass July 16, 2001 Update date
Performance Simulations
Scientific Method.
Open Rack Specification 2.1 Update
Scientific Method.
SPS-DQW HOM Measurements
November 7, 2008 The meeting on RIKEN AVF Cyclotron Upgrade Progress report on activity plan Sergey Vorozhtsov.
A Compact Patch Antenna for Ultrawideband Application
Paper review Yun-tae Park Antennas & RF Devices Lab.
700 MHz Taskgroup Update Last Call July 28th Issues discussed
Presentation transcript:

C63.19 SC8 WG3 meeting, March 26, 2007 Calibration values for dipole validations at new RF probe separation distance of 1.5cm PINS-C item 5.k Jagadish Nadakuduti EME Research Engineer, Motorola, Inc. C63.19 SC8 WG3 meeting, March 28, 2006

C63.19 SC8 WG3 meeting, March 26, 2007 Outline Background –C Amendment: Change the RF measurement position from bottom of probe element to the center of element and change the test distance from 10mm to 15mm FDTD simulations Updated Table 4.2 and Table D.4 Measurements Conclusion

C63.19 SC8 WG3 meeting, March 26, 2007 Background: PINS-C item 5.k The RF probe separation distance is 15 mm and the calibration values in table 4.2 were made at 10 mm. These calculations need to be redone at 15 mm distance. 15 mm

C63.19 SC8 WG3 meeting, March 26, 2007 FDTD simulations: E- & H-field patterns Update field values from 10 mm to 15 mm distance

C63.19 SC8 WG3 meeting, March 26, 2007 FDTD simulations: Results at 10 mm Created FDTD models as specified in “D Dipole validation theoretical modeling”. Comparison of FDTD simulations results to those specified in Table D.4. Mod.Freq. (MHz) CW peak E (V/m) existing new CW peak H (A/m) existing new |Zo| (Ω) Return loss (dB) VSWRGain (dBi) CW , , , , CW , , , , 2.29 CW , , , , 2.3 CW , , , , 2.55 Table D-4. Results of FDTD modeling for ‘Thick dipoles’ (existing values vs. new simulation results)

C63.19 SC8 WG3 meeting, March 26, 2007 FDTD simulations: Results at 10 mm contd. CW peak E- and H-field values taken from table D-4 are converted into RMS values. These values are incorporated into Table 4.2. Table 4.2 – Illustrated dipole calculated values (existing and new simulation results) “D Dipole validation theoretical modeling” section describes simulations for ‘thick dipoles’ and has no information on modeling parameters for ‘planar dipoles’. The relatively high difference between values specified in table 4.2 and those from new simulations in case of ‘planar dipoles’ might be because of using different simulation parameters. DipoleFreq. (MHz) E-field values (V/m) existing new differenceH-field values (A/m) existing new difference D.5.1 thick % % D.5.1 thick % % D.5.1 thick % % D.5.1 thick % % D.5.1 planar % % D.5.1 planar % % D.5.1 planar % % D.5.1 planar % %

C63.19 SC8 WG3 meeting, March 26, 2007 Measurements: At 10 and 15 mm of probe separation distance with 100 mW of input power Frequency (MHz) E (V/m)H (A/m) 10 mm15 mm10 mm15 mm Frequency (MHz) E (V/m)H (A/m) 10 mm15 mm10 mm15 mm Thick dipoles Planar dipoles *898.5 MHz thick dipole is not available in the lab

C63.19 SC8 WG3 meeting, March 26, 2007 Updated Table D.4 at 15 mm Mod.Freq. (MHz) CW peak E (V/m) (dB V/m) CW peak H (A/m) (dB A/m) |Zo| (Ω) Return loss (dB) VSWRGain (dBi) CW CW CW CW Table D-4. Results of FDTD modeling at 15 mm

C63.19 SC8 WG3 meeting, March 26, 2007 Table 4.2 at 10 mm with measurement results Table 4.2 – Illustrated dipole calculated and measured values DipoleFreq. (MHz) E-field values (V/m) calculated measured differenceH-field values (A/m) calculated measured difference D.5.1 thick % % D.5.1 thick % % D.5.1 thick D.5.1 thick % % D.5.1 planar % % D.5.1 planar % % D.5.1 planar % % D.5.1 planar % %

C63.19 SC8 WG3 meeting, March 26, 2007 Updated Table 4.2 at 15 mm with measurement results Table 4.2 – Illustrated dipole calculated and measured values DipoleFreq. (MHz) E-field values (V/m) calculated measured differenceH-field values (A/m) calculated measured difference D.5.1 thick % % D.5.1 thick % % D.5.1 thick D.5.1 thick % % D.5.1 planar % % D.5.1 planar % % D.5.1 planar % % D.5.1 planar % %

C63.19 SC8 WG3 meeting, March 26, 2007 Conclusion ‘Planar dipole’ FDTD simulations need to be repeated with the correct parameters. The following sections in C need to be updated with calibration values at 15 mm distance –In Section 4.4: Table 4.2 –In Annex D: Table D.4 Figures D.3 - D.6, D.10 Equations D.1 & D.2 Include ‘Planar dipole’ simulation parameters in section ‘D Dipole validation theoretical modeling’. All of the above tasks can be completed in a time frame of 1-2 months.

C63.19 SC8 WG3 meeting, March 26, 2007 Thank you

C63.19 SC8 WG3 meeting, March 26, 2007 Table 4.2 at 10 mm

C63.19 SC8 WG3 meeting, March 26, 2007 Table D-4 at 10 mm