1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.
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Transcript of 1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.
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ILC Push-Pull : Platform
Marco Oriunno, SLAC
ILD Workshop, Paris May 24, 2011
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ILD SiD
ILD and SiD differences
Weight= 15 ktonnes Weight= 10 ktonnes
ILD SiD
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Option 1, ILD and SiD moving on the floor
Option 2, ILD on a platform, SiD moving on the floor
Option 3, ILD and SiD on platforms
Impact of this option has been studied by ILD
Not favorable to SiD – heavy impact on CE
Under Study
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Trade off study - Conclusion
SiD with Platform ILD withPlatform
Mandatory requirements SiD ILD
Design Change Impact None High
Vibrations Amplification Low Low
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Push-Pull with platforms
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Thicker platform ?
Extra Height to accommodate the difference of the two detectors
2.2 m3.8 m
20 m 20 m
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Gripper Jacks on rail
Rails
Rollers
Anti-seismic support
Gripper jacks
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Motion system
Gripper Jacks, 1’000 T
DL-G1000 gripper jack for load out of offshore structures (1000 tonnes push / pull capacity)
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SiD nominal mass: Barrel 5000 T; (each) Door 2500 T
Dimensions:Z = 20.0 mX = 20.0 mDelta Y = 9 m (Top of Platform to beamline)
Positioning Tolerance on beamlineConsider points Z=+-max, X=0. Position to + 1mm wrt references in X,Y,ZConsider points Z=+-max, X=+-max: Position to +- 1 wrt references in Y.
SiD Platform Functional Requirements
Static Deformations: <+-2 mm
Vibration Transfer Function from ground : Amplification < 1.5 between 1 and 100 Hz.
Seismic stability: Appropriate for selected site. (Beamline must be designed with sufficient compliance that VXD will survive)
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SiD Platform Functional Requirements
Wall clearance ~10 mm. Platform comes to side wall, there is no apron or apron matches platform elevation.
gap,10 mm
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SiD Platform Functional Requirements
Surface Features: Steel Surface near legsSteel rails for doors“Receptacles” for tie seismic tiedowns of SiD Barrel and DoorsRemovable Safety railings
Detector Top View Platform Top View
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SiD Platform Functional Requirements
Reliability: Transport modularity must be such that repairs/replacement/maintenance can be accomplished in garage position and within 20 elapsed days.
Any equipment required for transport shall reside below the platform surface.
Transport equipment shall not eject particulates that reach platform surface (need spec on how much)
Accelerations: < 0.01 g
Transport velocity: V>1 mm/s after acceleration
Life: 100 motion cycles.
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QD0 supported from the doors
QD0
1. SLD Experience
2. QD0 push-pull with the detector
3. Low L* ~ 3.5 m
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Sub-nanometric stability of the focusing system is required to maintain the luminosity to within a few percent of the design value.
Ground motion is a source of vibrations which would continuously misaligning the focusing elements.
The design of the support of the QD0 is a fundamental issue
QD0+
QD0-
QF+
QF-
IP plane
Luminosity Loss & Vibrations
5.7 nm
640 nm
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Luminosity Loss & Vibrations
Most acute luminosity loss mechanism due to relative jitter of final focusing magnet elements : Ground Motion and Mechanical vibration sources
Max. Integrated relative displacement: 200 nm > 5 Hz
Luminosity loss due to beam offset in SD0 (beamsize growth) and IP misalignment of beams
98%96%
Definition: Luminosty ~ Collision Rate at the Interaction point
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Luminosity feedback systems and stability
Two Luminosity Feedback systems are implemented in ILC :
• A 5 Hz to control the orbit in the BDS (low frequency)
QD0 alignment accuracy: ± 200 nm and 0.1 μrad from a line determined by QF1s, stable over the 200ms time interval between bunch trains
• A Intra-train system to address ground motion and mechanical disturbances (high frequency~1000 Hz)
QD0 vibration stability: Δ(QD0(e+)-QD0(e-)) < 50 nm within 1ms long bunch train “
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Vibrations : Absolute, Relative and Coherent and motion
Relative displacement spectrum
Coherence :
If P1=P2, then : Jo = 0th Bessel functionL= distance between pointsv = speed of sound in rock, ~3 km/s
P1 P2
Ground Motion Model (A.Sery)
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QF12 x L*
FD
M
K C
CfKf
QF12 x L*
FD
M
K C
CfKf
QD0 Supports
High Coherence
Low Coherence
Door DoorBarrel
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IP Region Final Doublet : QD0+QF1
Platform Transfer Function
Ground Vibration models
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GM Induced Jitter @ IP (Vertical Offset between e- and e+ beams at IP) with and without QD0 TF
GM’C’
GM’B’
GM’A’
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2121
Platform Simulation
Benchmark with exp.data
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CMS Platform (as built)
2200
20.5 m
Iron re-bars (equivalent th. 25 mm)
Iron re-bars (equivalent th. 25 mm)
Concrete, 2150 mm
Total thick. 2.2 m
Plate Model: zero thickness with bending stiffness around the middle plane
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Bencmark with static test done on the platform
Dummy load = 2500 tons, Weight of the platform = 1780 tonsMax sag at the center = 3.5 mm
N.B. = Platform Simply supported on the edges
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Mode 1
Mode 5
Mode 4
Mode 3
Mode 2
Mode FREQ 1 20.17 2 41.12 3 53.24 4 72.76 5 73.28 6 95.85
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100
101
102
10-22
10-21
10-20
10-19
10-18
10-17
10-16
10-15
10-14
Hz
m2/Hz
PSD - Damp. 6.5%PSD - Damp. 4%PSD - Damp. 2%PSD - Exp.PSD - Ground
Resonance at ~20 Hz
Simulations vs. Measured PSD (Platform Center)
Peaks 80 and 90 Hz
)()()(2
fPgroundfFtfSy
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Integrated Displacement (r.m.s.)
100
101
102
10-11
10-10
10-9
10-8
10-7
10-6
Hz
m
Damp. 2%Damp. 4%Damp. 6.5%Exp.Ground
Hz
f
dffPx100
2
1
)(
Damp. 2% Damp. 4% Damp. 6.5%
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• Platforms are a technically acceptable solutions for the push pull, which preserves the respective design of the detectors and does not amplify the ground vibrations.
• The platforms must be designed according to a set of Functional Requirements, specifying the static and dynamic performances. These requirements will be defined by the detectors.
• The design and construction of the platforms becomes a task of the CFS group, which will develop the project along the requirements list and together with the detectors.
Conclusions
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o The effects of vibrations on beam stability remain a subject which need further studies.
o Benchmarking of the FEM and experimental data is in progress : good results so far
o Start the optimization of the Experimental Area, integration of the platforms
o Decide on a Push-pull mechanism : Rollers, Air-pads, hydraulic jacks, etc.
o All above only achievable as common task MDI / CFS
The work ahead
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33M.Oriunno, Eugene, Or Nov.2010
Bonus Material
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Sub-nanometric stability of the focusing system is required to maintain the luminosity to within a few percent of the design value.
Ground motion is a source of vibrations which would continuously misaligning the focusing elements.
The design of the support of the QD0 is a fundamental issue
QD0+
QD0-
QF+
QF-
IP plane
Luminosity Loss & Vibrations
5.7 nm
640 nm
![Page 35: 1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.](https://reader035.fdocuments.us/reader035/viewer/2022062719/56649ee55503460f94bf4ee7/html5/thumbnails/35.jpg)
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Luminosity Loss & Vibrations
Most acute luminosity loss mechanism due to relative jitter of final focusing magnet elements : Ground Motion and Mechanical vibration sources
Max. Integrated relative displacement: 200 nm > 5 Hz
Luminosity loss due to beam offset in SD0 (beamsize growth) and IP misalignment of beams
98%96%
Definition: Luminosty ~ Collision Rate at the Interaction point
![Page 36: 1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.](https://reader035.fdocuments.us/reader035/viewer/2022062719/56649ee55503460f94bf4ee7/html5/thumbnails/36.jpg)
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Luminosity feedback systems and stability
Two Luminosity Feedback systems are implemented in ILC :
• A 5 Hz to control the orbit in the BDS (low frequency)
QD0 alignment accuracy: ± 200 nm and 0.1 μrad from a line determined by QF1s, stable over the 200ms time interval between bunch trains
• A Intra-train system to address ground motion and mechanical disturbances (high frequency~1000 Hz)
QD0 vibration stability: Δ(QD0(e+)-QD0(e-)) < 50 nm within 1ms long bunch train “
![Page 37: 1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.](https://reader035.fdocuments.us/reader035/viewer/2022062719/56649ee55503460f94bf4ee7/html5/thumbnails/37.jpg)
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Vibrations : Absolute, Relative and Coherent and motion
Relative displacement spectrum
Coherence :
If P1=P2, then : Jo = 0th Bessel functionL= distance between pointsv = speed of sound in rock, ~3 km/s
P1 P2
Ground Motion Model (A.Sery)
![Page 38: 1 ILC Push-Pull : Platform Marco Oriunno, SLAC ILD Workshop, Paris May 24, 2011.](https://reader035.fdocuments.us/reader035/viewer/2022062719/56649ee55503460f94bf4ee7/html5/thumbnails/38.jpg)
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QF12 x L*
FD
M
K C
CfKf
QF12 x L*
FD
M
K C
CfKf
QD0 Supports
High Coherence
Low Coherence
Door DoorBarrel
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QD0
Kfoot
Kplatform
M door
QD0Considered Rigid onnection
Floor Elasticity, not included
SiD Vibration Model : 1 degree of freedom M,K,C oscillator
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4040
1st Mode, 2.38 Hz 2nd Mode, 5.15 Hz 3rd Mode, 5.45 Hz
4th Mode, 6.53 Hz 5th Mode, 10.42 Hz 6th Mode, 13.7 Hz
Vertical motion
SiD Free Vibration Mode
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Kfoot
Kplatform
M door
QD01st mode system
SiD Vibration Model : 1 degree of freedom M,K,C oscillator
22
22
pf
pfn ff
fff
f foot = 10 Hz from FEA, f platform =
6 Hz, supported edges
30 Hz, int.support, door-on-barrel
15 Hz, int. support, door-on-platform
f n =
5 Hz
9 Hz
8 Hz
c = 2%
ff = 1st mode SiD foot
fp = 1t mode platform
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fo = 5 Hz fo = 10 Hz
PSD PSD
Integrated r.s.m. displacement
Integrated r.s.m. displacement
Random vibration Studies : SiD on the floor without platform
30 nm20 nm
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fn = 5 Hz
fn = 8 Hz
fn = 9 Hz fn = 10 Hz
Free span, supported edges
∞ Rigid Platform
30 nm 25 nm
22 nm 20 nm
Random vibration Studies : SiD on platform
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IP Region Final Doublet : QD0+QF1
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GM Induced Jitter @ IP (Vertical Offset between e- and e+ beams at IP) with and without QD0 TF
GM’C’
GM’B’
GM’A’