Hydrostatic Level Systems at Fermilab and DUSEL J Volk, V Shiltsev Fermilab USA A Chuprya, M Kondaurov, S Singatulin Budker Institute of Nuclear Physicis.

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Presentation transcript:

Hydrostatic Level Systems at Fermilab and DUSEL J Volk, V Shiltsev Fermilab USA A Chuprya, M Kondaurov, S Singatulin Budker Institute of Nuclear Physicis Russia L Stetler, J Van Beek South Dakota School of Mines and Technology USA J Volk Fermilab IWAA 11 Sept 2010

Hydro static water Level Systems HLS J Volk Fermilab IWAA 11 Sept 2010 BUDKER sensor Capacitive pickup Accuracy 1 micrometer Cost $1200 per channel Capacitive sensorWater pool On stand with water and Air line connections Water line Air line

Ultra Sonic Sensor and Electronics J Volk Fermilab IWAA 11 Sept 2010 Water pool and sensor Separate electronics Ultra sonic sensor better than 1 micrometer resolution $4000 per channel

Schematic of Ultra Sonic Sensor J Volk Fermilab IWAA 11 Sept 2010 R1 and R2 are Fixed distances used for calibration OF is water level Target at top is for alignment

Ultra Sound Pulses J Volk Fermilab IWAA 11 Sept 2010 DescriptionMinActualMaxunits Echo pulse duration μsμs Test Frequency56.910MHz Bandwidth at 6 db % Pulse echo sensitivity dB 2 volts per division 20 μs per division GE H10KB5T

Fermilab design Tevatron style J Volk Fermilab IWAA 11 Sept channel readout card Ether net interface Balluff sensor and pool Power supply RS232 port Pa per in IWAA-08 J Volk

Sensors at Fermilab and DUSEL J Volk Fermilab IWAA 11 Sept 2010 NameLocationType of SensorNumber of sensorsSoftware versionOperating system Tev SensorsTevatron quadrupolesBalluff204 ACNET B0Low beta quads B0 interaction region SAS919_Mar-09Windows XP D0Low beta quads D0 interaction region SAS919_Mar-09Windows XP HLS-Minos-2MINOS HallSAS-E704-Mar-10Windows XP ADAPS90581LaFarge Mine North Aurora IlSAS519_Mar-09Windows XP Array A2000-ft level Homestake Gold mine, Lead SD TEV6Windows XP Array B2000-ft level Homestake Gold mine, Lead SD TEV6Windows XP Array C2000 ft level Homestake Gold mine Lead SD SAS-E604-Mar-10Windows XP DUSEL-1MP8 tunnel FermilabSAS-E1204-Mar-10Windows XP HLS-MP8-1MP7 tunnel FermilabULSE304-Mar-10Windows XP HLS-MP8-2MP8 tunnel FermilabULSE1204-Mar-10Windows XP BDPHY14MP8 tunnel FermilabTest and calibration04-Mar-10Windows 7 Hot SparesMP8 tunnel FermilabSAS-E404-Mar-10Windows 7 PK 50Porta Kamp 50 FermilabTest and calibration04-Mar-10Windows XP

Tevatron HLS sensors during quench J Volk Fermilab IWAA 11 Sept 2010

Quench Low Beta Quads B0 Interaction Region J Volk Fermilab IWAA 11 Sept 2010 A side where quench occurred B side response to quench

One Month MINOS Data J Volk Fermilab IWAA 11 Sept 2010

Other types of Ground Motion J Volk Fermilab IWAA 11 Sept 2010 Subsidence caused by earth quakes Floor tilting caused by movement of water Primary Secondary

Five Years of MINOS data J Volk Fermilab IWAA 11 Sept 2010

Two Years of Data From LaFarge Mine J Volk Fermilab IWAA 11 Sept 2010

Chilean Earth Quake of February 27, 2010 J Volk Fermilab IWAA 11 Sept magnitude earthquake as seen By the LaFarge mine HLS Secondary wave tilted floor For 25 minutes 16 μm Spacing 120 m 0.13 μradian

DUSEL Lead South Dakota J Volk Fermilab IWAA 11 Sept 2010 Homestake gold mine Cross section of Homestake gold mine Ross shaftYates Shaft 1.2 km

HLS in 2000 ft Level Homestake Gold Mine DUSEL/Sandford lab J Volk Fermilab IWAA 11 Sept 2010

Array C Budker Sensors 2000 ft level Homestake Gold mine J Volk Fermilab IWAA 11 Sept 2010 Difference in two sensors 2000 ft level

Calibration Stand for Balluff sensors J Volk Fermilab IWAA 11 Sept 2010 Calibration of a Balluff sensor Adjustable stage and micrometer

Balluff Sensor Calibration Data J Volk Fermilab IWAA 11 Sept 2010

View of SAS-E Test Stand J Volk Fermilab IWAA 11 Sept 2010 Single pipe half filled system Pipe diameter 25.4 mm

Two sensors on same system 4 m apart 2 weeks of data J Volk Fermilab IWAA 11 Sept 2010

Adding 50 CC of water to system J Volk Fermilab IWAA 11 Sept 2010

Adding 50 cc of water to SAS-E system J Volk Fermilab IWAA 11 Sept 2010 SN 188SN 189SN 190SN 191SN 193SN 194SN 195SN 196SN 197SN 198SN 199SN 200AverageStd Dev Fill numbermicrons

Adding 50 cc of Water to ULSE Sensors J Volk Fermilab IWAA 11 Sept 2010 Fill numberSN 53SN 57SN 64SN 56SN 63SN 62SN 54SN 55SN 61SN 59SN 58SN 60averagestd dev

Heating of Budker Capacitive Sensors with fixed disk in pool J Volk Fermilab IWAA 11 Sept micro meter per division SN 198SN 188

Heating of Budker Ultra Sonic sensors J Volk Fermilab IWAA 11 Sept 2010 Same scale 1 micro meter per division Sensor 53Sensor 60

Heating of electronics only for Budker Ultrasonic sensor J Volk Fermilab IWAA 11 Sept micro meter per division

Findings From Calibration Studies J Volk Fermilab IWAA 11 Sept 2010 The capacitive sensors calibration is good to 0.5 micro meters as determined by water filling tests. The temperature dependence of the capacitive sensors has a hysteresis and varies from sensor to sensor. This could be an electronic effect and will need more testing. Need to split analog and digital parts test separately. The ultrasonic sensors have a larger temperature dependence than the capacitive sensors. The electronics for the ultrasonic sensors is very stable as measured by separate tests. Change in water level can not be totally accounted for by water expansion. Need to test transponders to fully understand temperature effects.

Conclusions J Volk Fermilab IWAA 11 Sept 2010 HLS can provide useful information for accelerator operations. Resolutions of less than 1 micro meter are possible. Stability test of systems needs more work. Temperature dependence of electronics needs to be studied. There is a need to cross calibrate different systems

J Volk Fermilab IWAA 11 Sept 2010 Danke schön! Thank You For you attention I can be reached at