Instrumentation for cryogenics at CERN

Slides:



Advertisements
Similar presentations
André Augustinus 15 March 2003 DCS Workshop Safety Interlocks.
Advertisements

Analog-to-Digital Converter (ADC) And
TE / CRG / Paulo Gomes The Control System for the LHC tunnel cryogenics, p. 1 CERN Portuguese Teachers Programme, 7 Sep 2011 Dr. Paulo Gomes on behalf.
Beam Loss Analysis Tool for the CTF3 PETS Tank M. Velasco, T. Lefevre, R. Scheidegger, M. Wood, J. Hebden, G. Simpson Northwestern University, Evanston,
LECC 2006 Ewald Effinger AB-BI-BL The LHC beam loss monitoring system’s data acquisition card Ewald Effinger AB-BI-BL.
Classification of Instruments :
DCS LEB Workshop ‘98, Rome, Detector Control System, H.J.Burckhart,1 Detector Control System H.J Burckhart, CERN u Motivation and Scope u Detector and.
Juan Casas1 st June 2007 Instrumentation and controls challenges Juan Casas CERN AT.
Metra Mess- und Frequenztechnik Radebeul / Germany Piezoelectric Accelerometers Theory & Application.
Lecture 5: PID Control.
Cryogenic Systems Juan Casas (TE-CRG-CI) In behalf of the CRG team R2E and Availability Workshop - Cryogenic Systems - JCC
LHC Beam Screen Heaters: System overview, consolidation needs and project planning 4 February TE-CRG/JCC (Beam Screen Heater Review) 1.
CRYOGENICS AND POWERING
21/01/02 - ECAL Cooling - Arnaud Hormiere ST/CV 1 Development of ECAL COOLING PLANT Application to a Super Module.
LHC ARC Commissioning report during LS1 Agenda: VRGPE documentation (former VRJGE) Active Penning modification By-Pass Valves modification LHC ARC commissioning.
Seminar ON SMART SENSOR Submitted by : SUBIR KUMAR GHOSH Roll No. IN-14/04 Electrical & Instrumentation Deptt. B.E 7th Semester JORHAT ENGINEERING COLLEGE,
Accelerators for ADS March 2014 CERN Approach for a reliable cryogenic system T. Junquera (ACS) *Work supported by the EU, FP7 MAX contract number.
The Radiation Tolerant Electronics for the LHC Cryogenic Controls: Basic Design and First Operational Experience J. Casas, G. Fernandez Peñacoba & M. A.
Radiation Tolerant Electronics New Policy? Ph. Farthouat, CERN.
LHC Cryogenics Control: INTEGRATION OF THE INDUSTRIAL CONTROLS (UNICOS) AND FRONT-END SOFTWARE ARCHITECTURE (FESA) APPLICATIONS Enrique BLANCO Controls.
Acquisition Crate Design BI Technical Board 26 August 2011 Beam Loss Monitoring Section William Vigano’ 26 August
Radiation Tolerant Electronics Expected changes Ph. Farthouat, CERN.
Chiller control system Lukasz Zwalinski – PH/DT.
Chiller control system Specification meeting Lukasz Zwalinski – PH/DT.
FP420 Low and high voltage supply INFN/Univ. of Torino July A presentation intended to stimulate the discussion on which.
L. Serio COPING WITH TRANSIENTS L. SERIO CERN, Geneva (Switzerland)
LHC Beam Loss Monitors, B.Dehning 1/15 LHC Beam loss Monitors Loss monitor specifications Radiation tolerant Electronics Ionisation chamber development.
1 Association Euratom-CEA P. Libeyre Pioneering superconductivity 23rd SOFT, Venice 21 September 2004 PIONEERING SUPERCONDUCTING MAGNETS IN LARGE TOKAMAKS.
Process Definition of the Operation Modes for Super-FRS Magnet Testing CSCY - CrYogenic department in Common System, GSI, Darmstadt Y. Xiang, F. Wamers.
JRA on Development of High Temperature SC Link Motivation Work Packages Partners & resources Amalia Ballarino Esgard open meeting CERN,
Superconducting Technologies for the Next Generation of Accelerators CERN, Globe of Science and Innovation 4-5 December Superconducting Links for the Hi-Lumi.
The integration of 420 m detectors into the LHC
The Control System for the LHC tunnel cryogenics Controlling Cool Accelerators Controle da Criogenia de Aceleradores de Partículas Dr. Paulo Gomes CERN.
Mike Struik / LHC-CRI INSTRUMENTATION FEEDTHROUGH SYSTEM FOR LHC MACHINE ARC QUADRUPOLE MAGNETS. 123rd LHC Vacuum Design Meeting 19 April 1999.
1 Radiation worries in the cavern L.Jirdén
E.Sbrissa EP/TA3 - IC ATLAS EDR_MAG Magnet Project Fault analysis, QA & Failure rate.
TWEPP Paris, 09 Radiation Tests on the complete system of the instrumentation electronics for the LHC Cryogenics at the CNGS test facility Evangelia Gousiou.
BASIC AUTOMATIC CONTROLS UNIT 16 ADVANCED AUTOMATIC CONTROLS
TE-MPE-CP, RD, 28-Sep Problems with QPS DAQ Systems During LHC Operation, 1 st Results from 2010 CNRAD Tests R. Denz TE-MPE-CP.
NMLTA Protection System Update -Loss Monitors- Arden Warner September 2 nd, 2009.
ILC : Type IV Cryomodule Design Meeting Main cryogenic issues, L. Tavian, AT-ACR C ryostat issues, V.Parma, AT-CRI CERN, January 2006.
LCLS-II Prototype Cryomodule Darryl Orris 21 January 2015 Final Design Review: Instrumentation.
INTRODUCTION TO ELECTRONIC INSTRUMENTATION
Temperature sensors Temperature is the most often-measured environmental quantity. This might be expected since most physical, electronic, chemical, mechanical,
Process Simulation for the LCLS-II Cryogenic Systems
UNICOS: UNified Industrial COntrol System CPC (Continuous Process Control) Basic course SESSION 3: PLC basics UCPC 6 UNICOS-Continuous Process Control.
IT-4189 Supply and installation of a cryogenic distribution system
Cryo equipment strategy in the R2E context
SCADA for Remote Industrial Plant
L'instrumentation et le contrôle de la cryogénie
OVERVIEW Impact of Modelling and simulation in Mechatronics system
Ideas and design concepts, and challenges
TYPES OF ERROR Types of static error Gross error/human error
Hollow e- lens, Cryogenic aspects
Circuits description and requirements - Closed Session-
Irradiation test of Pressure Transducers for the LHC machine
Overview of Temperature Measurement ME 115
Control System Instrumentation
Mathew C. Wright January 26, 2009
TPC Detector Control System
The pros and cons of in-situ testing – going beyond the test standards
Radiation tolerant fibres for LHC controls and communications
RADIATION induced failures in LHC 28th June 2011
Measurements & Error Analysis
Operation of Target Safety System (TSS)
Instruments & Electrical Measurements Lecture 3
Optical fiber based sensors for low temperature and superconductors
Cryogenic management of the LHC Run 2 dynamic heat loads
F.Pasdeloup, H.Prin, L. Williams
J. Fleiter, S. C. Hopkins, A. Ballarino
Presentation transcript:

Instrumentation for cryogenics at CERN Juan Casas CERN TE-CRG European Cryogenics Days - 2016 CERN

Overview Introduction Turn-key facilities Radiation areas: LHC tunnel Measurement channel acquisition design under radiation constraints Radiation qualification Operational results Conclusions European Cryogenics Days - 2016 CERN

CERN: Cryogenics Refrigerators & most distribution equipment: turn-key procurement Cryogenics in accelerator areas: particular constraints => non-commercial parts European Cryogenics Days - 2016 CERN

Instrumentation: Turn-key procurement Sensors, actuators, electronics, etc.  available from industry European Cryogenics Days - 2016 CERN

Instrumentation: Turn-key procurement CERN limit of supply: PLC and Remote IO (RIO) Present Trend: Move toward smart sensors Typically connected to industrial fieldbuses (profibus: CERN supported fieldbus) Most are available for 4-20 mA HART but its features seldom used @ CERN Provide new features and a wider array of diagnostics data Accuracy/resolution figures set by sensor and not by RIO Additional cost partially offset by simplified cabling + removal of RIO However industrial/commercial solutions not fully satisfactory for: Reading cryogenic temperature sensors (<20 K) problems with electrical cabinet integration or RIO signal resolution Superconducting LHe level gauges: Supplied by different vendors and wide array of active measurement lengths Signal conditioner usually lack terminals for remote disabling to avoid burnout. => CERN custom analog signal conditioners are provided for these applications European Cryogenics Days - 2016 CERN

Instrumentation: Requirements Most measurement requirements are satisfied by standard industrial apparatus; to the extent that it looks as if the data-sheets sets the process requirements…. However some applications require a closer look-up: Modified instrument for cryo-operation (example: Coriolis mass flow meters) Temperature measurement concerns: Platinum thermometers do not have an “official” conversion below 72 K Class A ± 0.3 K @ 73 K Used at CERN down to 30 K: does satisfies table below? Sensors with little literature concerning accuracy (example: CLTS) Long term drift Actual measurement performance difficult to assess European Cryogenics Days - 2016 CERN

Instrumentation: CERN thermal anchoring Most challenging LHC measurement channel is temperature: Superconducting magnet temperature is a control parameter Accuracy has a direct impact in regulation band Accuracy budget is 0.01 K split in the sensor & electronics Temperature sensors followed a very strict selection and QA procedure Thermal anchoring compatible with large series production was designed: calibration in “final” conditions & provide reliable measurement under vacuum. European Cryogenics Days - 2016 CERN

Instrumentation: Thermometer Stability Long term stability is difficult to assess; thermal cycles are used to accelerate ageing Test: 100 Temperature cycles between 4.5 – 300 K in GHe (no humidity) Only CERNOX satisfies the accuracy requirements above 4 K This imposes complete control of all parameters affecting the measurement like individual calibration, signal conditioning, thermal anchor, etc. European Cryogenics Days - 2016 CERN

Instrumentation: Radiation Design Turn-key equipment trend towards smart fieldbus instruments Radiation => fieldbus instruments: the dumber the better….. Example LHC case: European Cryogenics Days - 2016 CERN

Instrumentation: Radiation Design Radiation is a very challenging environment that require: Radiation dose maps from calculation-intensive simulation (FLUKA modelling) Optimize location of sensor, conditioning electronics (& PLC) Design, select or customize sensor and/or signal conditioning electronics Suitable irradiation test-area (particle type, dose rate, etc.) Reference comparison apparatus, usually not rad-hard Strict QA policy for procurement and management of spare parts Dealing with obsolescent parts for machines with a lifespan > 20 years => Whenever possible avoid radiation tolerant equipment! In an accelerator environment fast particles may appear in radiation free areas: May cause malfunction and unforeseen stops Requires consolidation without appropriate test-time LHC cold-compressors, valve-boxes & HTS leads thermometers were victim of radiation events and relocating the sensitive equipment was the solution: Magnetic bearings controls within maximum tolerable cable length Use of LHC split SIPART valve positioners Relocate RIO and profibus interfaces Consolidate HTS leads temperature measurement cards ….. European Cryogenics Days - 2016 CERN

Instrumentation: Radiation Design Radiation maps required to set experimental qualification doses LHC case: Cold devices need to be rad-hard Electronics can be “radtol” (< 1 kGy) if placed at centre & below the dipoles. Long straight areas: radiation far too high => electronics in protected areas => Use as much radtol electronics to save cable cost European Cryogenics Days - 2016 CERN

Cold Instrumentation: Radiation Design Cold Instruments need to be rad-hard Assumed rad-hard by design: superconducting LHe level meters Same material as magnets BEWARE: Radiation qualification shall be performed in final operational conditions Thin film Ge sensors reported in 1997 to be rad-hard! Excellent LHC candidate Irradiation @ room temperature Drift is deduced from calibration before & after irradiation. OK for LHC use CERN irradiation test: Complete repair after annealing at room temperature! Drift not visible in previous report 2 orders of magnitude OFF Not usable in LHC conditions European Cryogenics Days - 2016 CERN

Cold Instrumentation: Radiation Design Radiation tests in cold conditions are extremely difficult to perform: Select/design cold-sensors, CERN case: selection from commercial catalogues Require a reference comparison instrument Temperature sensors <-> LHe bath saturation pressure & bulb, remote sensor Continuous filling LHe filling Remote analog electrical signals acquisition. Accumulated dose still too low comparing to worst LHC zones after 20 years operation. European Cryogenics Days - 2016 CERN

Warm Instrumentation: Radiation Design LHC instrumentation exposed to radiation is made of mostly: Thermometers that cannot be changed => qualification is mandatory Pressure sensors => qualified for ranges 0-2 and 0-20 bara Valves that are (were) considered intrinsically radhard: On/OFF pneumatic made of basic elements (coils, magnets,..) Proportional valve: split design, assumes rad-hard piezo electric element Electrical heaters … European Cryogenics Days - 2016 CERN

Instrumentation: Signal Conditioning Radiation Design Signal conditioning radiation hardness is limited by the weakest component. Radiation effects induce drift (similar to temperature effects) and change the state of digital circuits (can be a simple memory upset or a destructive event) Analog signal conditioning relies on: Passive comparison bridge, comparison resistor (low TCR, qualified) Rad-hard by design ¼ micrometer IBM tek ASIC Accuracy set by amplifier and ADC non-linearities Local control performed by anti-fuse FPGA with triplicated logic Commercial microFIP communication interface: found to be rad-tol Note that new versions (same part number) are sensitive to radiation All mathematical calculations done remotely by FEC European Cryogenics Days - 2016 CERN

Instrumentation: Signal Conditioning Radiation Design All individual components need to be qualified: Select, qualify, procure & maintain Both total dose and singular/transient effects need to be evaluated Radiation effects require compensation Adequate duplication of readings may be required ADC Accuracy European Cryogenics Days - 2016 CERN

Instrumentation: Signal Conditioning Radiation Design Fast particles affect digital or power devices via Single Event Effects (SEE) Digital status of digital circuits can be corrupted by Single Event Upsets (SEU) Non destructive SEU can be tackled: By design at the electronics card level Repaired by performing a “reset” or a power cycle Such events can provoke unexpected operational scenarios like shown here below: SEU affects a LHC HTS superconducting current lead temperature sensor => “negative” temperature => beam dump Once temperature increases readout looks “normal” but > 100 K instead of < 50 K => current lead quench when increasing magnets current Repaired by electronics reset. European Cryogenics Days - 2016 CERN

Instrumentation: Signal Treatment Radiation Design SEU when foreseen during the design phase can be tackled effectively However, if not expected to occur they can be very disruptive, for the LHC: Appeared in 2011 (due to increase in luminosity) and first events caused a systematic beam dump Operational experience permitted to implement appropriate procedures => no more systematic beam dump WFIP tunnel electronics consolidated by end 2011 => No more SEU SEU prone commercial equipment relocated by end 2012 => No more SEU European Cryogenics Days - 2016 CERN

Instrumentation: Signal Treatment Radiation Design LHC chain made of “dumb” sensor but full chain is equivalent to a “smart” device Example - LHC pressure measurement chain: Sensor is made of sensitive membrane and temperature sensor (rad-hard) WFIP electronics (rad-tol) acquire signals for measuring membrane reference membrane temperature sensor Temperature correction => 20 fold accuracy improvement Performed by remote commercial control computer Performance equivalent to a modern fieldbus based sensor European Cryogenics Days - 2016 CERN

Instrumentation: Signal Treatment Radiation Design LHC chain made of “dumb” sensor but full chain is equivalent to a “smart” device LHC temperature measurement chain: Excellent immunity against radiation and ambient temperature effects Raw data permit to estimate temperature oscillation of cryo-crates Equipment in LHC underground area: Test in climatic chamber: European Cryogenics Days - 2016 CERN

Instrumentation: LHC thermometry LHC temperature readout is of “laboratory” quality in spite: Very hostile environment, worse than typical industrial installation Sheer quantity of measuring channels (9’000) Individual calibration => require QA during manufacturing Once installed difficult/impossible to exchange Cross-check possible for superfluid pressurized bath => dispersion within ± 0.005 K European Cryogenics Days - 2016 CERN

Conclusions Radiation environments impose cumbersome qualification procedures and usually (always?) involve management of obsolescent parts Whenever possible avoid radiation areas Temperature readings are not trivial and in the range 6 to 50 K the requirements are hardly met by just a few sensors; and this only if appropriate thermal anchoring procedures and signal conditioning is applied. The LHC accelerator imposed the investigation of radiation tolerant electronics in order to save cabling cost, remote electronics may be possible but would require up to 3 km long cables and ECM may become a problem => local electronics nevertheless mandatory The LHC demonstrates that it is possible to perform laboratory-like measurement within a radiation environment, but this require the understanding of all the elements of the complete measurement chain. European Cryogenics Days - 2016 CERN