TCT testbed RF Testbed for TCT D Fallon - Electronics Research Inc L Yan, G Hanson, S Patch - UWM.

Slides:



Advertisements
Similar presentations
5th Collaboration Meeting on X-band Accelerator Structure Design and Test Program. May 2011 Review of waveguide components development for CLIC I. Syratchev,
Advertisements

Ultrasound Microscopy and High Frequency Coded Signals Antti Meriläinen, Edward Hæggström.
30 th September 2004 High Power RF Couplers James Rogers High Power RF Couplers ELSRF Daresbury Laboratory.
BEPCII RF POWER SYSTEM RF group, IHEP Sep ~ April 1.The 1 st transmitter had finished installing,commissioning and SAT (Site Acceptance Test).
FDWAVE : USING THE FD TELESCOPES TO DETECT THE MICRO WAVE RADIATION PRODUCED BY ATMOSPHERIC SHOWERS Simulation C. Di Giulio, for FDWAVE Chicago, October.
Transmission Lines Demonstration High Frequency Electronics Course EE527 Andrew Rusek Oakland University Winter 2007 Demonstration is based on the materials.
Project by Santiago Yeomans, Chad Cummins, Gboyega Adeola Guitar Signal Transmitter.
8. Wave Reflection & Transmission
OUTLINE Introduction „Tera-to-Nano“: Our Novel Near-Field Antenna 80 GHz CW Frequency Domain Measurements Picosecond Pulse Time Domain Measurements 2D.
x z y 0 a b 0 0 a x EyEy z rectangular waveguides TE 10 mode.
ECE 501 Introduction to BME
Antennas Lecture 9.
TE 21 Second-Harmonic Gyro-TWT Amplifier with an Axis-Encircling Beam S.B. Harriet*, D.B. McDermott, and N.C. Luhmann, Jr. Department of Applied Science,
Polytechnic University© 2002 by H. L. Bertoni1 III. Spherical Waves and Radiation Antennas radiate spherical waves into free space Receiving antennas,
ENE 428 Microwave Engineering
Introduction to Vector Network Analyzer (VNA)
Review Doppler Radar (Fig. 3.1) A simplified block diagram 10/29-11/11/2013METR
CLIC Drive Beam Linac Rolf Wegner. Outline Introduction: CLIC Drive Beam Concept Drive Beam Modules (modulator, klystron, accelerating structure) Optimisation.
FractalComs Exploring the limits of Fractal Electrodynamics for the future telecommunication technologies INFORMATION SOCIETY TECHNOLOGIES (IST) PROGRAMME.
RADAR Detection of Extensive Air Showers Nils Scharf III. Physikalisches Institut A Bad Honnef Nils Scharf III. Physikalisches Institut A Bad.
George David Associate Professor Ultrasound Physics 04: Scanner ‘97.
Microwave Engineering, 3rd Edition by David M. Pozar Copyright © 2004 John Wiley & Sons Figure 3.1 (p. 92) (a) General two-conductor transmission line.
Lecture 6.
Efficient design of a C-band aperture-coupled stacked microstrip array using Nexxim and Designer Alberto Di Maria German Aerospace Centre (DLR) – Microwaves.
rectangular waveguides x z y 0 a b 0 TE or H mode.
Phased Array Feeds John O’Sullivan SKANZ 2012 CSIRO Astronomy and Space Science,
1 Fourth Year Final Project - BGU HF Electromagnetic Vector Sensor Students: Roy Nevo, Yiftach Barash Advisors: Mr. Benny Almog Prof. Reuven Shavit
Device Noise Two figures of merit for noisy devices
Building Three-Dimensional Images Using a Time-Reversal Chaotic Cavity
Near Field Antenna Measurements for Cellular Phone Certification Ahlia M. Tillman, John Rzasa, Bandar Hakim, Quirino Balzano, and Christopher C. Davis.
Plate acoustic waves in ferroelectric wafers V. A. Klymko Department of Physics and Astronomy University of Mississippi.
Plane Wave Echo Particle Image Velocimetry Samuel Rodriguez, Xavier Jacob, Vincent Gibiat PHASE University Paul Sabatier.
Clustered Surface RF Production Scheme Chris Adolphsen Chris Nantista SLAC.
704MHz Warm RF Cavity for LEReC Binping Xiao Collider-Accelerator Department, BNL July 8, 2015 LEReC Warm Cavity Review Meeting  July 8, 2015.
1 RS ENE 428 Microwave Engineering Lecture 4 Reflection and Transmission at Oblique Incidence, Transmission Lines.
MULTI-MODE GENERATOR FOR THE COLD TEST OF BROADBAND QUASI-OPTICAL GYROTRON MODE CONVERTERS D. Wagner 1, M. Thumm 2, G. Gantenbein 2, J. Flamm 2, J. Neilson.
Ultrasound Simulations using REC and SAFT Presenter: Tony Podkowa November 13, 2012 Advisor: Dr José R. Sánchez Department of Electrical and Computer Engineering.
University of Kansas 2004 ITTC Summer Lecture Series Network Analyzer Operation John Paden.
Ultrasound Physics Reflections & Attenuation ‘97.
So far, we have considered plane waves in an infinite homogeneous medium. A natural question would arise: what happens if a plane wave hits some object?
Effects of RF Pulses on Circuits and Systems – Pieces UMCUUI C 1 UIUCUH MURI Team Experience in EM Penetration and Coupling Pieces.
1 The University of Mississippi Department of Electrical Engineering Center of Applied Electromagnetic Systems Research (CAESR) Atef Z. Elsherbeni
ENE 428 Microwave Engineering
1 ENE 428 Microwave Engineering Lecture 11 Excitation of Waveguides and Microwave Resonator.
TOSHIBA RF Receiver for HDTV Final Design Review 4/21/2005 Team: Josue Caballero, Brett DiCio, Daniel Hooper, Efosa Ojomo, George Sewell.
Brit and the Rad Lab at MIT Radiation Laboratory Series: Documented developments from the Rad Lab Volume 19 (copyright 1949): Waveforms- edited by B. Chance.
ECE 4710: Lecture #37 1 Link Budget Analysis  BER baseband performance determined by signal to noise ratio ( S / N ) at input to detector (product, envelope,
Evaluation of the TE 12 Mode in Circular Waveguides for Low-Loss High Power Transportation Sami G. Tantawi, C. Nantista K. Fant, G. Bowden, N. Kroll, and.
1 EuroTeV High Bandwidth Wall Current Monitor Alessandro D’Elia AB-BI-PI.
Doc.: IEEE yy/xxxxr0 Submission March 2005 Kobayashi, Trachewsky, Dalton, Broadcom Corp.Slide 1 Controlled Over the Air Test Methdology Update Notice:
1 John McCloskey NASA/GSFC Chief EMC Engineer Code 565 Building 29, room Fundamentals of EMC Dipole Antenna.
Study & Design of Micro-strip Patch Antenna
30GHz system improvements Jan Kovermann RF meeting
Preamplifier R&D at University of Montreal for the drift chamber J.P. Martin, Paul Taras.
Antennas and Propagation
HF Wire Antennas, EMI Contest Stations WCARC November 2016 VE3KL
Nicolas Fagnoni – Cosmology on Safari – 14th February 2017
How does a klystron work? TE-MPE Section Meeting Karolina Kulesz
Ultrasound.
Beam Measurement Characterization and Optics Tolerance Analysis of a 900 GHz HEB receiver for the ASTE telescope Alvaro Gonzalez, K. Kaneko, Y. Uzawa.
Prototyping Status September 11, 2012
Phased Array Feeds SKANZ 2012 John O’Sullivan
Frequency Reconfigurable Microstrip Patch Antenna
System Considerations for Submillimeter Receiver
ENE 428 Microwave Engineering
Summary of Lecture 18 导波条件 图解法求波导模式 边界条件 波导中模式耦合的微扰理论
A THEORETICAL MODEL for MAGNETIC FIELD IMAGING with “SWISS ROLLS” STRUCTURES V. Yannopapas J. B. Pendry M. C. K. Wiltshire J. Hajnal.
ENE 428 Microwave Engineering
ENE 428 Microwave Engineering
Presentation transcript:

TCT testbed RF Testbed for TCT D Fallon - Electronics Research Inc L Yan, G Hanson, S Patch - UWM

TCT testbed Goal - controlled illumination for large FOV imaging - illuminate with high-power, broadband (short) pulse w/108 MHz carrier freq - control polarization of E field - quantify  P inc, both power and envelope  P trans,  P inc - P trans - P baseline = power loss in object Feng et al ‘01 Wisc ‘07 optimized match ~10ns uncontrolled E- field & loss ?match?

TCT testbed TCT Wave Eq Model + homog ICs for I(t)=  (t) thermal mechanical electrical

TCT testbed Quantitative Imaging Challenges partial scan data - iterative recon transducer aperture size - integrating detectors acoustic attenuation - corr. for aphysical model variable soundspeed E field pattern/optical fluence corr. broadband data required, including low freqs unwanted EM coupling to US measurements transducer response - freq dependent & has limited sensitivity - anisotropic

TCT testbed E-field pattern & Acoustic Source SOP to solve in frequency domain near carrier frequency. 1) E is wave-like. At 100 MHz, air ~300cm, H20 ~33cm, fat ~70cm, muscle ~40cm  2) tangential BCs force continuity of E x n Solve Helmholtz in frequency domain

TCT testbed E-field in TCT Testbed Power in Very nearly TE 103 Aluminum walls & DI water not lossy, waves resonate I(t) ~ H(t). acoustic window E-field on central plane inside Surface current add output port E ~ 0.9 TE TE 103 I(t) ~  (t)

TCT testbed TCT Testbed - hardware Translators - Sherry Yan, George Hanson, UWM-EE. Port design - & duck - courtesy Dan Fallon, ERI, Inc. S 21 power from port 1 out port 2 S 21 = dB or P out = 0.88 P in S 11 = dB or P refl = P in T = Maine springtime room temp

TCT testbed System Signal Generator - Rohde&Schwarz (SML01) Pulsed Amplifier - QEI Corp 50kW pulsed amp-QEI Corp tunable carrier freq carrier freq  108MHz

TCT testbed Pulse profiles - time & freq Remove carrier frequency (108 MHz)  MHz transducers do badly with 500ns pulse - 5 MHz transducers do well with 500ns pulse

TCT testbed S-parameters Measure - incident & reflected power at each port: P inc, P ref, P trans, P load - for carrier freqs 70:130 MHz, w/4 microsec pulses (Eckhart) Compute (in dB scale) - S 11, power reflected, ideal -  dB - S 21, power transmitted, ideal 0 dB

TCT testbed S-parameters S 11 S 21 MHz

TCT testbed E-field measurements Slotted top & monopole antenna fabricated at UWM G. Becker, M Rhodes

TCT testbed Can see a balloon qualitative

TCT testbed Conclusions Testbed performs essentially as a transmission line, preserving short temporal pulse shape. Bandwidth of testbed greater than bandwidth of QEI pulses. Chimney shields effectively

TCT testbed Thanks WUWM for lending dir coupler line sections Tom May (WUWM Chief Engineer) for system setup Andrew Eckhart for collecting S-param data Mike Schrauth for developing positioners Mark Rhodes & Jerry Becker for slotted top & antenna