Summary of temperature mapping developments G. Ciovati, M. Champion AES Cavity Meeting, JLab, August 28 th 2007.

Slides:



Advertisements
Similar presentations
Tom Powers Practical Aspects of SRF Cavity Testing and Operations SRF Workshop 2011 Tutorial Session.
Advertisements

New Optical Inspection Results at JLab An in-depth update since Chicago meeting ILC08 (Highlights reported in US Regional Talk by Mark Champion) Rong-Li.
Liquid H 2 Absorber Production Contents (1)MICE Absorber Status (2)MICE Absorber Modification (3)Plan/Schedule (4)Summary MICE CM-23 in HARBIN Shigeru.
T. Saeki (KEK) 15 May 2014 AWLC2014 at FNAL
Manchester 09/sept/2008A.Falou & P.Cornebise {LAL-Orsay}1 CALICE Meeting/ Manchester Sept 2008 SLAB Integration & Thermal Measurements.
ILC Activities at Cornell June 7, 2011 Temp and Current vs. Time.
1 Superconducting Magnets for the MICE Channel Michael A. Green Oxford University Physics Department Oxford OX1-3RH, UK.
Diagnostics system for SPL cavities & 2 nd sound Cryolab Kitty Liao CERN BE-RF-KS 1 5 th SPL collaboration meeting 25 November 2010.
Slide # 1 Examples of pressure sensor packaging Temperature characteristics of a piezoresistive pressure sensor. Transfer function at three different temperatures.
Cavity Vertical Test and Diagnostics Kitty Liao Second Open Collaboration Meeting on Superconducting Linacs for High Power Proton Beams.
WUT Experience in Measurements of the Heat Transfer Thought SC Cable Electrical Insulation Jaroslaw Polinski*, Maciej Chorowski*, Michal Strychalski*,
Spectrometer Solenoid Update Steve Virostek Lawrence Berkeley National Lab Roy Preece Rutherford Appleton Lab October 28, 2011 MICE Collaboration Meeting.
M. FOUAIDY Thin films applied to superconducting RF cavitiesLegnaro Oct.10, 2006 improved accuracy and sensitivity as compared to the usual RF method RS.
ILC PM Meeting S0 Webex Global Design Effort 1 S0/S1 Next Steps Lutz Lilje GDE.
ILC08 Chicago Global Design Effort 1 Discussion of Optical Inspection and Temperature mapping Results Several new inspection and mapping systems.
Workshop on Beam losses, heat deposition and quench levels for LHC magnets, Geneva, 3-4 March 2005 Liquid helium heat transfer in superconducting cable.
TILC09 AAP Review Lutz Lilje Global Design Effort 1 Cavity Gradient R&D.
Seminar ON SMART SENSOR Submitted by : SUBIR KUMAR GHOSH Roll No. IN-14/04 Electrical & Instrumentation Deptt. B.E 7th Semester JORHAT ENGINEERING COLLEGE,
Cavity Productions at DESY DESY -MPY- FNAL Overview on the cavity productions Review of cavity performance Some conclusions.
IHEP 1.3 GHz Cryomodule and Cryogenics IHEP Cryogenic group 2nd Workshop of the IHEP 1.3 GHz SRF R&D Project Dec 2 nd, 2009.
Summary of Main Linac SCRF-part H. Hayano, ILC08 at UIC.
2-D FEM MODELING OF MICROWAVE HEATING OF COAL PARTICLES EGEE 520 SEMESTER PRESENTATION by Ojogbane M. Achimugu May 3 rd 2007.
3 June 2012 BE-KT Innovation Day Prevessin, CERN, Switzerland
1 Numerical study of the thermal behavior of an Nb 3 Sn high field magnet in He II Slawomir PIETROWICZ, Bertrand BAUDOUY CEA Saclay Irfu, SACM Gif-sur-Yvette.
/18 Cryogenic thermometry for refrigerant distribution system of JT-60SA Kyohei NATSUME, Haruyuki MURAKAMI, Kaname KIZU, Kiyoshi YOSHIDA, Yoshihiko KOIDE.
Global Design Effort 1 S0 Status High-Gradient cavities Lutz Lilje DESY supplement by H. Hayano 04Sep2008 EC
TTC Meeting, Frascati, 5-7 December Summary of EP discussions at Oct SMTF meeting at FNAL T. Tajima (LANL), C. Boffo (FNAL)
AMS-RICH Detector. J. Berdugo – CIEMAT (Madrid, Spain) 1 AMS-02 Phase II Flight Safety Review AMS Ring Imaging CHerenkov PURPOSE: 1.Precise measurement.
R.L. Geng, 5/27-31,2013 ECFA LC2013, DESY 1 Update on Raising Q0 at Ultra-High Gradient via Large-Grain Niobium Material Rongli Geng Jefferson Lab ECFA.
UNCOOLED IR DETECTOR TEMPERATURE CONTROL Performed by : Shimon Amir Yogev Ben-Simon Instructor : Arie Nakhmani 1 TECHNION - ISRAEL INSTITUTE OF TECHNOLOGY.
Preparation for the 3He Injection Test
HiGrade-Kickoff DESY Global Design Effort 1 ILC-HiGrade WP6 High-Gradient cavities Lutz Lilje DESY.
Update on S0 Work in the Americas Region Mark Champion 17 June 2008.
KEK-STF Vertical Test and Diagnostics Brief History & Future Plan Vertical Test Facility Cavity Diagnostic System Example of MHI#7 Cavity Summary of T-mapping.
Diagnostics Tests and Studies for SPL cavities Kitty Liao CERN BE-RF-KS First Open Collaboration Meeting on Superconducting Linacs for High Power Proton.
MLI Summary Chris Adolphsen SLAC. Summary of MLI Talks Quadrupoles (V. Kashikhin) –Expect test of a SLAC/CIEMAT and FNAL cos(2phi), ~ 60 T/m, SC Quads.
Americas S0 Cavity (Tesla-style) Test Philosophy and Test Status results from JLab, Cornell and FNAL C.M. Ginsburg (FNAL) GDE SCRF Meeting April 21, 2008.
S1 global: thermal analysis TILC09, April 19th, 2009 Serena Barbanotti Paolo Pierini.
1 Modeling of heat transfer in an accelerator superconducting coil with a ceramic insulation in supercritical helium S. Pietrowicz, B. Baudouy, CEA Saclay/
5 K Shield Study of STF Cryomodule (up-dated) Norihito Ohuchi KEK 2008/4/21-251FNAL-SCRF-Meeting.
Summary of Results and Development of Online Monitor for T-mapping/X-ray-mapping in KEK-STF Y. Yamamoto, H. Hayano, E. Kako, S. Noguchi, M. Satoh, T. Shishido,
High Q 0 preservation Andy Hocker Fermilab TTC CW Workshop, 13-JUN-2013.
MLI Update Chris Adolphsen SLAC. CAVITY VESSEL T4CM QUAD T4CM BPM QUADS LEADS 80K BLOCK 4K BLOCK Quadrupole Package.
August 16, 2007ILC Video Conference at FNAL Update on testing of Jlab fabricated 9-cell cavities P. Kneisel, G. Ciovati.
Americas Report C.M. Ginsburg (FNAL) for the FNAL/ANL, JLab, and Cornell (no report this time) cavity teams S0 Meeting 7.June 2011.
Superconducting Cryogen Free Splittable Quadrupole for Linear Accelerators Progress Report V. Kashikhin for the FNAL Superconducting Magnet Team (presented.
SRF Test Facilities – Functions and Costs Alexander Romanenko Test Facilities Review 17 Mar 2015.
ILC-HiGrade annual meeting - 22 November 2010 ILC-HiGrade Meeting Cavity-Treatment at CEA Saclay (WP6) F. Eozénou.
Possible Relationship Between Defect Pre-Heating and Defect Size H. Padamsee Cornell S0 Meeting, Jan 26, 2009.
Plasma cleaning Laser re-melting technique at FANL M. Ge, G. Wu, J. Ruan, J. Ozelis, T. Nicol, D. Sergatskov, D. Hicks, L. Cooley Fermi National Accelerator.
WP10 General Meeting, Giovanni Volpini, CERN 1 December 2015 Test progress INFN 1.
LCLS-II Prototype Cryomodule Darryl Orris 21 January 2015 Final Design Review: Instrumentation.
S A Griffiths CM42 June 2015 Electrical & Control.
July 5th,2006John Mammosser, Jlab ILC – Electropolish Development (EP) Plans/Progress/Problems/Performance Jefferson Lab J. Mammosser, L. Phillips, C.
MECH 373 Instrumentation and Measurements
XFEL beamline loads and HOM coupler for CW
Calorimeter Mu2e Development electronics Front-end Review
Results on second sound method
Masaru Sawamura (JAEA)
Y. Yamamoto, H. Hayano, E. Kako, S. Noguchi, M. Sato, T. Shishido, K
Vertical Test System and T-mapping/X-ray-mapping at KEK-STF
The resistance of a thermistor changes from 30k to 12k when the temperature changes from 20C to 70 C Calculate the sensitivity if resistance is taken.
5K Shield Study & HL Measurements
ILC Main Linac Superconducting Splittable Quadrupole
Prototyping with Micro-controllers, Sensors, and Materials
Manufacturing Processes
Magnetic Field Sensors and Measurements in Cryomodules
Optical fiber based sensors for low temperature and superconductors
Benefits & Advantages of Pogo Pins
Presentation transcript:

Summary of temperature mapping developments G. Ciovati, M. Champion AES Cavity Meeting, JLab, August 28 th 2007

Outline Existing capabilities –Cornell 1-cell system, 1.5 GHz –DESY 1- and 9-cell system, 1.3 GHz –KEK 1-cell systems, 0.5 GHz –Saclay 1-cell system, 1.3 GHz –JLab 1-cell system, 1.5 GHz Development projects –FNAL 1- and 9-cell system, 1.3 GHz –LANL 9-cell system, 1.3 GHz –JLab, 2-cell system, 1.3 GHz

Rotating vs. fixed systems Rotating T-map systems compared to fixed ones have: Reduced number of thermometers and cavity preparation time Longer data acquisition time Ability to detect only “stable” losses Reduced sensitivity in superfluid He

Existing capabilities

Cornell 1-cell 1.5 GHz 768 Allen-Bradley 100  (1/8W) resistors, distributed in 36 boards, 10  spaced.

Thermometer design features: –High sensitivity at 2 K (  15  /mK) –Time response 7 ms –Linear response, between 1  K – 1 K for power flux between 1  W/cm 2 – 1 W/cm 2 –Linear self-heating as a function of the dissipated power in the resistor (  1 mK for 0.2  W) Apiezon N grease used to improve thermal contact

2 feedthrough boxes on top of the test stand for wiring inside/outside of cryostat National Instruments data acquisition system, 140ms/scan J. Knobloch, Ph.D. Thesis, Cornell University, 1997

DESY 1- and 9-cell system, 1.3 GHz The 1-cell system is a copy of the Cornell design The 9-cell system is rotating, 116 thermometers distributed in 9 arms. 5  angular steps, about 1h for complete map.

Thermometers for rotating system: –100  Allen-Bradley resistors housed in a silver block, spring loaded contact –The thermometer efficiency depends on contact pressure and heat power level Ag block Epoxy T. Junquera et al., Proc. of the 1995 PAC, p.1648 Q. S. Shu et al., Proc. of the 1995 PAC, p.1639 and Proc. of the 7 th SRF Workshop, p. 523

In addition, DESY has an “equator” T-map system with Cornell-style thermometers 72 thermometers divided in 24 boards, 15  spaced Courtesy W.-D. Moeller

KEK 1-cell systems, 0.5 GHz Two systems for 0.5 GHz single cells: –fixed, 1332 resistors (51  Allen-Bradley), 36 boards, 10  spacing, 48 s/scan –Rotating, 25 resistors, 2 s/scan, 2-6 min/turn T. Takahashi et al., KEK Preprint (1993) T. Tajima et al., KEK Preprint (1992)

Saclay 1-cell system 1.3 GHz 60 thermometers (developed for DESY 9- cell system) distributed on 6 arms, 60  spaced J. Lesrel et al., Proc. of the 1998 EPAC, p.1861 M. Fouaidy et al., Proc. of the 1996 EPAC, WEP043L

JLab 1-cell system 1.5 GHz Based on Cornell design. 576 resistors distributed in 36 boards, 10  spacing

1 feedthrough box on top of the test stand for wiring inside/outside of cryostat National Instruments data acquisition system, 1MS/s, 15ms/scan G. Ciovati et al., JLAB Tech Note TN (2005)

Developments

LANL 9-cell system, 1.3 GHz 5508 Allen-Bradley (100  ) sensors per meridian cell, 10  spaced 36 G-10 boards cover 3 cells, 108 boards total 12 boards (40  coverage) will be powered at a time to reduce the number of cables out of the cryostat to  720 Power switching done in the cryostat Expected  2s/scan First test expected by 09/15/07

The excitation voltage is multiplexed between all sensors, the readout voltage occurs on the same wire for 9 sensors Sensitivity at 2 K expected to be mV/mK Voltage (mV) A. Canabal et al., Proc. of the 2007 PAC, p. 2406

JLab 2-cell system, 1.3 GHz Build a system to map the equator region of 2/9 cells of ILC cavity identified as suspect for quench location by TM 010 pass-band measurements Share resources (Data acquisition, software) with the existing single-cell system 320 Allen-Bradley (100  ) Cornell-style thermometers, 11  spacing, covering from weld to  3 cm down along equator

KEK 1- and 9-cell systems 1.3 GHz Use RuO 2 sensors Make shape-independent system (film resistors) K. Saito, private communication

FNAL 1- and 9-cell system 1.3 GHz Fixed systems, 960 diodes/cell, 16 sensors/board, 6  spacing Interchangeable boards between 1- and 9- cell systems Diode sensor ~1mmx1mm sensing area Kapton w/ printed circuit Flex shown in compressed state as if contacting the cavity G10 board

Standard multiplexing scheme works with diodes, reduce no. of cables (one 64-pin cable/cell) Commercial 1N4148 –  10 mK resolution measured at 4 K –Temperature sensitivity (dV/dT at 2 K) and thermometer efficiency are yet to be determined

“In house” data acquisition system Expected  1 min/scan for 9-cell system A. Mukherjee, private communication Card assembly, only 3 shown for clarity. 60 cards/ cell Helium flow holes Support system for intial assembly Cage PCB

Conclusions T-mapping is the most common diagnostic tool for SRF cavities In the design of new systems, fixed ones are preferred Systems with thousands of sensors are being built for 9-cell cavities, multiplexing schemes will be used to reduce cabling New sensors are being considered (RuO 2, diodes) to replace Allen-Bradley (discontinued, expensive)