Slow Ground Motion Studies at Fermilab James T Volk Accelerator Division Andrey Chupyra, Shavkat Singatulin, Budker Institute of Nuclear Physics Vladimir.

Slides:

Advertisements

Similar presentations

The MINER A Operations Report All Experimenters Meeting Howard Budd, University of Rochester Aug 6, 2012.

Advertisements

Q15. Fluid Motion.

Physics Quicky A Stone Thrown Downward

MTest Facility Low Energy Beam Erik Ramberg AEM 15 October, 2007.

Graphing in Science.

Fluid in Motion.

Ground motion data J Volk The first graph is the difference in two sensors 90 meter apart in MINOS hall the data shows the earth tides and also tilting.

PENNSYLVANIA Pennsylvania is home to 12,440,621 people Pennsylvania is approximately 46,055 square feet. That makes Pennsylvania the 33 rd largest state.

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

Diamonds in CDF Peter Dong, UCLA Ricardo Eusebi, FNAL Anna Sfyrla, Geneva Rick Tesarek, FNAL Rainer Wallny, UCLA With much help from Jonathan Lewis (FNAL)

Projectiles The red ball is given a velocity U at an angle  to the horizontal U  The time taken for the ball to move up and down is the same time as.

Notes – Pressure & Buoyant Force

The MINER A Operations Report All Experimenters Meeting Howard Budd, University of Rochester Nov

Hydrostatic Level Systems at Fermilab and SURF J Volk V Shiltsev Fermilab A Chupyra M Kondaurov S Singatulin Budker Institute of Nuclear Physics D Fratta,

Tevatron Alignment ( ) 1 WBS Tevatron Alignment Ray Stefanski January 21, 2004 Run IIA Alignment.

Yuji Otake, Akito Araya and Kazuo Hidano

Projectile Motion Review

Quad-to-quad correlated motion in FLASH Ramila Amirikas, Alessandro Bertolini DESY Hamburg XFEL beam dynamics meeting, February 25 st 2008.

Do you think Ms. Chavez can go through an small index card?

1 Alternative assembly option of ILD Y.Sugimoto 2010/10/18 ILD Integration

Installation of HLS at the ATF2 Mika Masuzawa, Masanori Satoh and Ryuhei Sugahara (KEK) Georg Gassner and Robert Ruland (SLAC) 1.Motivation 2.What is HLS?

CC focuses on controlling outcomes. CC controls change, making sure that its impact is assessed and that every effort is made to prevent erosion of functionality.

Beams Division Seminar Configuration Management in the Tevatron – Alignment Ray Stefanski March 6, 2003.

Projectiles calculations Calculating the components of a vector using trigonometry and vertical and horizontal problems.

Projectiles Horizontal Projection Horizontally: Vertically: Vertical acceleration g  9.8 To investigate the motion of a projectile, its horizontal and.

Calculating pressure Pressure = Force / Area Example – A 1000 N person is standing on 2 feet. The area of the person’s feet is.2 m 2. What is the pressure.

1 Liquid Argon Dark Matter: Synergies with R&D for Neutrino Detectors: Chemically clean Argon for drifting electrons and light output (Oxygen and H20 relevant.

MBA Magnets MultiBend Achromat Magnets 9/27/2013 Review By Mark Jaski.

One Dimensional Projectile Motion Activity #5 Imagine throwing the ball straight up and letting it come back down as in experiment #3 while underneath.

J T Volk Fermilab April 2008 Ground Motion Studies at Fermi National Accelerator Laboratory James T Volk Applications Physicist II Vladimir Shiltsev, Shavkat.

Deformations and Movements of CERN installations Mark Jones M. Jones, 28/10/2015 FCC Infrastructure and Operation Meeting.

CHAPTER 6 MOTION IN 2 DIMENSIONS.

International Workshop on Accelerator Alignment Jim Volk Valentin Ivanov Shavkat Signatulin Virgil Bocean Gary Coppola Rick Ford O’Sheg Oshinowo George.

Earthquakes Part 2 Remember- earthquakes usually occur along faults in the earth’s lithosphere. (San Andreas Fault) - Normal Fault - Reverse Fault - Strike.

If the sum of all the forces acting on a moving object is zero, the object will (1) slow down and stop (2) change the direction of its motion (3) accelerate.

WHITE BOARD TIME !! CONSERVE ENERGY. E T = PE G + KE + PE S When comparing the energy at two different positions on a system, the total energy at one.

NLC - The Next Linear Collider Project Mike Woods May 1999 Vibrations and the NLC IR Welcome to the NanoWorld !

Chapter 14 Work, Power, and Machines. Section 1 Work and Power.

1 Mice Collaboration Meeting CM33 Glasgow University 25 th – 29 th June 2012 STFC Daresbury Laboratory Electrical Infrastructure Report Authors : Ian Mullacrane.

FPD STATUS Carlos Avila Uniandes/UTA 1. FPD overview 2. Roman pot and detector status 3. FPD readout integration status 4. Software status 5. Stand-alone.

: a substance that has the capacity to flow and assume the form of the container it has been placed in. Fluid: a substance that has the capacity to flow.

EXAMPLE 1 Subtracting Integers –56 – (–9) = – = –47 –14 – 21 = –14 + (–21) = –35 Add the opposite of –9. Add. Add the opposite of 21. Add. a. –56.

Vladimir Sirotenko, Feb FPD: Runs & hisDB Oracle Databases Goal: access information about FPD experimental setup and accelerator conditions which.

F James T Volk Arpil Permanent Magnets for Linear Colliders James T Volk Fermilab.

ILC Cryogenic System Shallow versus Deep Tunnel Tom Peterson Dubna Meeting 5 June 2008.

Neutron Shield/Muon Veto (WBS 1.3) and Underground Installation Issues (WBS 1.6) May 11, 2009 Erik Ramberg.

Chapter 10 Fluids Pressure in Fluids Pressure is defined as the force per unit area. Pressure is a scalar; the units of pressure in the SI system.

Vibration issues at Linear Colliders:

Fluids Objectives: Pressure inside fluids Hydraulic Lift

Physics Support Materials Higher Mechanics and Properties of Matter

BIOLOGY GRADE 10 CSEC GROUP

S.Ecklund, C.LeCocq, R.Pushor, R.Ruland, A.Seryi, Z.Wolf

Monday, January 29, 2018 (Discussion – The Ocean in Motion: Waves; DE Techbook Assignment – Ocean Waves)

Name ______________ Date ____________

Describing Motion Power Point 02.

y = B t - 1, x = t - 9 are the parametric equations of the curve

Ch. 3: What is a Fluid? Particle Model

Pressure Chapter 3.3.

Pressure Level Sensor OTT PLS

Vertical Motion Problems

Plotting Points Guided Notes

y = C t - 1, x = t - 6 are the parametric equations of the curve

Motion in Two Dimensions

Velocity and Acceleration

August 29 AP physics.

Alignment Diagnostic System Status

Mechanics Chapter 6 Motion due to Gravity

Presentation transcript:

Slow Ground Motion Studies at Fermilab James T Volk Accelerator Division Andrey Chupyra, Shavkat Singatulin, Budker Institute of Nuclear Physics Vladimir Shiltsev, Sten Hansen, Terry Kiper Fermilab Principle that water seeks its own level

There are two types of HLS systems in use James T Volk May 2009 Budker Institute of Nuclear Physics Fermilab designed Tevatron style Balluff proximity sensor Capacitive sensor Water pool Air line Water line

Fermilab Design Tevatron Style James T Volk May channel readout card Ether net interface Balluff sensor and pool Power supply RS232 port Pa per in IWAA-08 J Volk

Tevatron Sensors on Quad James T Volk May 2009 In the circle is a water level pot on a Tevatron quadrupole Air Line Water line

Tevatron Quad Movement James T Volk May 2009 Tev access underway CHL changing Compressors

B 43 motion with Tev ramp James T Volk May 2009

B0 and D0 Low Beta Quads James T Volk May 2009 Bo low beta quad shielding removed D0 low beta quad

D0 low beta quad motion James T Volk May 2009

Difference in sensors on CQ5 and DQ5 James T Volk May 2009 Date Micro meters B3 Dumped burned up Changes in tunnel temp and pressure

Layout of MINOS water level James T Volk May 2009 MINOS detector 30 meters Not to scale  direction Sensor Water line Depth of floor 100 meters below grade 406 feet above sea level Maquoketa shale Location of Horizontal and Vertical seismometer New sensors

January 2006 MINOS Difference in two sensors 90 meters apart James T Volk May 2009

FFT of MINOS data difference between two sensors December 2007

Difference in two sensors 90 meters Apart MINOS hall 36 months of data James T Volk May 2009