1 Vibrations studies at KEKB/Belle KEK Hiroshi Yamaoka.

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Presentation transcript:

1 Vibrations studies at KEKB/Belle KEK Hiroshi Yamaoka

2 Detector floor - Is it possible to evaluate these vibrations by FEM? - Are those calculations consistent with measurements? Introduction Vibration measurements have been done at KEKB/Belle. ? ? ? ? ? ? ? ? ? Measure vibrations at KEKB KEKB floor concrete shield: 300tons Belle: 1300tons 10m Belle Platform

3 Vibration data QCS boat KEKB floor Detector floor

4 Calculations Respond vibration is calculated between two positions. ? ? ? ? QCS magnet KEKB floor At KEKB KEKB floor concrete shield: 300tons Belle: 1300tons 10m Belle Platform INPUT OUTPUT 1. Detector floor  KEKB floor 2. KEKB floor  QCS magnet 3. Detector floor  Belle platform 4. Belle platform  End cap/ Barrel yoke (Not yet: Sorry)  Needs special technique due to large model

5 KEKB floor Concrete shield 300 tons Calculation 1. Detector floor  KEKB floor Material Concrete E=30GPa Density=2.3 Damping= 2% Fixed Weight of Concrete shield 300tons Weight of magnets 2tons 20m

6 30Hz 58Hz 65Hz 81Hz Concrete E=30GPa Density=2.3 Damping= 2% Deformation: 0.01mm Deformation Natural frequencies

7 KEKB Floor Concrete shield Respond P.S.D. at KEKB-concrete floor Detector floor(B4 Floor) Concrete E=30GPa Density=2.3 Damping= 2%

8 Detector Floor(B4) KEKB Floor Concrete shield Integrated amplitudes of KEKB-concrete floor Concrete E=30GPa Density=2.3 Damping= 2% 99nm 101nm 10nm 9nm 6nm 74nm 61nm 65nm 63nm 10nm 4nm 10nm 3nm 56nm 52nm 50nm 44nm 5nm 3nm

9 MAC(Modal Assurance Criteria) Modal assurance criteria quantitatively compare all the possible combinations of test and analysis mode shape pairs. ModeFreq. Damping(%) 130.4Hz Hz Hz Hz Hz 8.02E-2 f2f2 fnfn f1f1 Damping ratio measurement 5th 3rd 2nd 4th 5th 1 st 4th 3rd 2nd 1st FEM Test MAC=1: Mode shape pairs is exactly match MAC=0: pairs that are completely independent 1st: 31Hz 3rd: 457Hz 5th: 1022Hz 4th: 534Hz FEM 2nd: 192Hz Cantilever Test 1st: 30Hz 3rd: 419Hz 2nd: 188Hz 5th: 992Hz 4th: 584Hz Damping ratio

10 No.Freq.(Hz) damping (%) Damping ratio should be assumed to 0.5% in FEM. 2% damping seems too high. Measurement result-A No. Freq.(Hz) damping (%) Measurement result-B Bus bar line for horn magnet

11 2. Vibrations of KEKB-floor and QCS Floor QCS Floor QCS

12 500kg QC2RP 1250kg QC1RE 1370kg 5. Support-rods(Forward)  Spring elements k=12521kg/mm per rod 4. Support-rods(Backward)  Spring elements k=6171kg/mm per rod 3. Thread bolts  10-M30 6-M24 Pre-tension: Not defined Coil 1. Loads - Self-weight - QC1RE: 1370kg - QC2RP: 1250kg - Box: 500kg 2. Materials Cryostat: SUS Coil: Cu Supp.-rod: Ti-alloy QCS table: SS400 Fixed Cryostat  Respond amplitude was calculated and check consistency btwn calc. and meas. QCSboat Magnet table Movable table QCSboat Magnet table Movable table QCS KEKB QCS support system damp=0.5%

13 Modal calculation 14Hz 20Hz 44Hz 48Hz Deformation 2.1mm

14 Response amplitude (Vertical direction) QCS-t QCS-s Coil-t Coil-s Calculation: damp=0.5% MeasurementCalculation:

15 Steel E=211GPa Density=7.85 Damping= 0.5% On the floor On the Platform Weight of End cap = 300 tons(Total) Weight of End cap = 300 tons(Total) Weight of Barrel yoke = 650 tons(Total) Fixed The belle platform *The weight of end-caps and barrel yoke are taken into account. The platform is assembled with square pipes reinforced by ribs m FEM model

16 4.6Hz11Hz16Hz 54Hz 85Hz Deformation: 2mm 300tons 650tons Deformation Natural frequencies *The weight of end-caps and barrel yoke are taken into account.

17 On the floor On the Platform Vibrations(P.S.D.) Beam dir. Perpend.

18 Vibrations(Amplitude) Beam dir. Perpend. 72nm 82nm 88nm 13nm 9nm 6nm 4nm 102nm 67nm 56nm 57nm 10nm 3nm 4nm 2nm 68nm 52nm 51nm 13nm 2nm 5nm 2nm

19 4. Belle platform  End cap/ Barrel yoke Sorry, this issue hasn’t finished yet. Because,  The size of FEM model is very big.  Needs special techniques to reduce the size. Detector floor ? ? ? ? KEKB floor concrete shield Barrel yoke 10m Belle Platform 1 3 End Cap

20 5. Vibration measurement at KEK Vibration measurement during the magnet excitation - Power supply - Data logger 20m

21 End-yoke Perpend.Beam-dir.Vertical Barrel-yoke Perpend.Beam-dir.Vertical Vibration Measurement during the magnet excitation  Vibrations when the magnet excitation shows different behavior, Effect of magnetic force should be taken into account in the calculation.

22 Other measurement: Effect of the QCS magnet cooling-down ? ? P.S.D. in the vertical direction - What happened at 12:00??  Cooling just had been begun.

23 Conclusions Vibration analysis has been performed and compared to measurement data. 1. Detector floor  KEKB floor Good consistency, FEM model is simple. Vibration effect is small above 1Hz/10Hz because of high natural frequencies. 2. KEKB floor  QCS magnet Good consistency. 3. Detector floor  Belle platform Relatively good. If the FEM model makes more precisely, it will become better consistency. 4. Detector floor  End caps/Barrel yoke: Not yet. Some special techniques for FEM needed due to very large model. Effect of the magnetic force should be taken into account. Vibration measurements at KEK - Belle roll-out will be done in early/middle of Dec.  Vibration during roll-out will be measured. - Vertex detector will be removed from the Belle in mid. Nov.  Vibration at central region will be measured. Detector level was adjusted to the beam level 12 years ago. Re-adjustment to the beam level hasn't been done so far. Detector level also hasn't measured.  Detector level will be measured before roll-out.

24

25 Comparison of ground motion with various sites Reference: Ground motion at KEK is relatively high.

26 2.6% I=4132A 800ton Support Positions Sensors(SP500) Measured E.Y. static deformations 1.5T The Belle solenoid magnet/Yoke

27

28 End-yoke Perpend.Beam-dir.Vertical Barrel-yoke Perpend.Beam-dir.Vertical  Vibrations when the magnet excitation shows different behavior, Effect of magnetic force should be taken into account in the calculation.

29 - What happened at 12:00??  Cooling just had been begun. Pressure in the N 2 tubes. 10:3712:3714:3716:37 Temperature of N 2 -shield Temperature of Coil Oscillated  Oscillations around 1Hz at 12:00 were observed in all directions. On the QCS On the N2 tube

30 ConcreteStrength(N/mm 2) : FcDensity(kN/m 3 ):  GeneralFc ≦ < Fc ≦ < Fc ≦ 6025 Young’s modulus: E c E c = 3.35 x 10 4 x ( γ/24 ) 2 x ( Fc/60 ) 1/3 Ex.) Fc = 21 N/mm 2 E c21 =3.35 x 10 4 x {(24-1)/24} 2 x (21/60) 1/3 = (N/mm 2 )