Stave 4008 Z rubyballs coordinates

Slides:



Advertisements
Similar presentations
Computer Vision, Robert Pless
Advertisements

QR Code Recognition Based On Image Processing
1 Jim Thomas - LBL SSD Survey Update Jim Thomas Lawrence Berkeley National Laboratory 3/21/2013.
Z x 725 Sensor Mark 140 x Sensor Coordinates Bump Bond Pad Ø = 12/ FE PAD#2 110 x 210 LM Structure FE Chip Coordinates Bump.
Survey(s) of TT8 10/12 TT 8 after wall1 16/12 TT 8 Standalone.
Status Update on Mechanical Prototype in Rome November 6,
A synthetic camera model to test calibration procedures A four step procedure (last slide) based on an initial position (LookAt) and 13 parameters: ( 
Optical Alignment with Computer Generated Holograms
3-D Geometry.
Lotte Verbunt Investigation of leaf positioning accuracy of two types of Siemens MLCs making use of an EPID.
Stave # 1 Metrology Eric VIGEOLAS, WG2 July the 12th 2011.
PROBABILITY AND SAMPLES: THE DISTRIBUTION OF SAMPLE MEANS.
Velo to T Alignment - Reminder General Strategy  Perform relative VELO-to-IT/OT alignment using  X,  Y at the center of magnet and  X,  Y (each.
QA during Stave Core Assembly Stephanie Qing Yang (Oxford) 25 th Sept 2014 WP4 f2f meeting at RAL.
SHIFTS: f ( x )  d ________________________ _______________________ Result for the whole graph _________________________.
Measurement report of Boostec girders Control after receipt Sylvain GRIFFET, 13/12/2010 Measurements performed on the 1 st and 2 nd of December 2010 with.
Platform positioning during MDT construction Tool for the platform positioning Ph. Schune J.-Ch. Barrière P RAXIAL A LIGNMENT S YSTEM (barrel) positioning.
The LiC Detector Toy M. Valentan, M. Regler, R. Frühwirth Austrian Academy of Sciences Institute of High Energy Physics, Vienna InputSimulation ReconstructionOutput.
POLAR COORDINATES (Ch )
Cavalier Fabien on behalf LAL group Orsay GWDAW 10 December, 14 th 2005 Reconstruction of Source Location using the Virgo-LIGO network Presentation of.
Measurement report of Boostec girders 1/13 Sylvain GRIFFET, 15/11/2010 Measurements performed on the 28th of October 2010 with the Laser Tracker LTD500.
10/03/2005 V.Kostyukhin 1 # Raw survey data file. # # All coordinates are in SURVEY reference system # assuming that stave is placed horizontally on flat.
Tests with JT0623 & JT0947 at Indiana University Nagoya PMT database test results for JT0623 at 3220V: This tube has somewhat higher than usual gain. 5×10.
Preparation of wall position Alignment of A and C side in closed position Creation of reference system Translation of reference system to open position.
ATLAS EXPERIMENT INTEGRATION TASK: SPACE MANAGEMENT Tatiana Klioutchnikova 05/06/
Photogrammetry for Large Structures M. Kesteven CASS, CSIRO From Antikythera to the SKA Kerastari Workshop, June
ATLAS Pixel Detector Discussion of Tolerances November 12, 1998 Pixel Mechanics D. Bintinger, LBNL E. Anderssen, LBNL/CERN.
1.Check Laser track of B=0 run and exclude some tracks in order to get precise GGV eff, which in turn is used when extract T1, T2 value by pos-B and neg-B.
Status Brussels GANTRY Ê Try to assemble modules with good precision 4 different calibration plates (Karlsruhe and Bari) 4 determination of pin positions.
Feature based deformable registration of neuroimages using interest point and feature selection Leonid Teverovskiy Center for Automated Learning and Discovery.
BARREL ALIGNMENT PLATFORM POSITIONING Goal: Positioning of the platforms at their nominal position on the MDT chambers (No position measurement in a database).
COMP322/S2000/L91 Direct Kinematics- The Arm Equation Link Coordinates and Kinematics Parameters (Cont‘d) Another example: A 5-axis articulated robot (Rhino.
A.Ostaptchouk AMS Meeting at CERN, 16 July Measurements of Octagon Walls with 3D CMM Characteristics of 3D CMM Measurement program Results of insert.
1/10 Tatsuya KUME Mechanical Engineering Center, High Energy Accelerator Research Organization (KEK) ATF2-IN2P3-KEK kick-off meeting (Oct. 10, 2006) Phase.
Production Readiness Review at PNPI Chamber assembling: Main production and quality control steps 30 January 2004 – G.Alkhazov 1.Input components control.
Welded joints.
Status Brussels GANTRY Ê New measurements of pin positions 4 using short pins rather than long ones 4 improved the precision Ë Cross-check of precision.
Circles Finding with Clustering Method By: Shimon Machluf.
Loading stave 4000  Receiving test of modules : No problem despite some damages at one edge of few modules (AMS) One MCC failure in one module, reworked.
Year 7: Length and Area Perimeter The perimeter of a shape is the total distance around the edge of a shape. Perimeter is measured in cm A regular shape.
Status VELO alignment 1.NIKHEF 3D measurements 2.Photogrammetry 3.Calliper checks in x-direction 4.Photogrammetry again Jo van den Brand May 23, 2006.
PIXEL ladder alignment Hidemitsu ASANO. Photo analysis & survey beam data (with zero magnetic field) ① SVX standalone tracking Global Tracking Strategy.
Company LOGO Technology and Application of Laser Tracker in Large Space Measurement Yang Fan, Li Guangyun, Fan Baixing IWAA2014 in Beijing, China Zhengzhou.
Grid Pix Field Simulations and precision needed for a module Peter Kluit, Jan Timmermans Prepared 16 May 2016.
TE-MSC. 07/04/2016 Jose Ferradas TE-MSC-MDT Alejandro Carlon TE-MSC-MDT Juan Carlos Perez TE-MSC-MDT On behalf to MSC-MDT section and Coil working group.
Biagio Di Micco  mass measurement   mass measurement blessing of the final result Biagio Di Micco.
BM&N STS ladders assembly in VLHEP
ATLAS pixel module assembly flow
Planar distortions for SCT Barrel Modules
Transformations and Symmetry
Sector 002 Assembly status report
Grid Pix Field Simulations and precision needed for a module
Sensor Wafer: Final Layout
Integration and alignment of ATLAS SCT
Status Brussels GANTRY
LCLS Undulator Fiducialization
Barrel stave allocation on the PP0 exhaust fitting
Evaluation of Turbine Blade Measuring
آشنايی با اصول و پايه های يک آزمايش
Alignment of the first two magnet system modules of Wendelstein 7-X
Station and Module Support Frames
Transformations Day 1 Notes Slideshow.
Outer Tracker Nominal Position
Comments on TRD rail system
Harm de Grijs Planes- the surface areas defined by abrupt variations of direction.
Determining the Function Obtained from a Series of Transformations.
Unit 37 Further Transformations
Recent Results on TRT Alignment
Circles
Translation in Homogeneous Coordinates
Presentation transcript:

Stave 4008 Z rubyballs coordinates Genova stave Measurement accuracy (check): Distance between crosses of the same module Measurement accuracy: X ~4m Z ~10m Z X Stave 4008 Z rubyballs coordinates R1 R2 R2-R1 Survey -412.9781 412.9962 825.974 Load(db) -413.0563 412.9367 825.993 Distance between FE pads of the same module X rubyballs coordinates R1 R2 Survey -0.0082 -0.0051 Load(db) -5.9749 6.0060 CMM problem?

Genova stave Survey data translated to load reference frame Coordinates of centers of modules Angles (rot. around Y) (rad) Zmeas Ztheor Zmeas-Ztheo Xmeas Angle -370.3440 -370.3100 -0.0340 0.1398 0.000123 -308.5780 -308.5920 0.0140 0.2038 -0.001561 -246.8510 -246.8730 0.0220 0.1600 0.000756 -185.1250 -185.1550 0.0300 0.1303 -0.002653 -123.3780 -123.4370 0.0590 0.0874 0.000613 -61.6630 -61.7183 0.0553 0.1046 -0.000088 -0.0514 0.0000 -0.0514 0.0587 0.000058 61.6831 61.7183 -0.0352 0.0475 0.000184 123.4430 123.4370 0.0060 0.0340 -0.000090 185.1880 185.1550 0.0330 0.1081 -0.000062 246.8470 246.8730 -0.0260 0.1081 -0.000300 308.5730 308.5920 -0.0190 0.1089 -0.000595 370.2580 370.3100 -0.0520 0.0851 0.000080 Z difference (mm) X difference (mm) Load and Survey coordinate systems are defined up to statistical measurement errors (transformation accuracy ~10m now). To improve accuracy the rubyball positions must be measured several times in both systems.

Wuppertal stave “stave coordinate system” data 2 measurement datasets exist for one stave: “survey coordinate system” data with shift in X z=0 : at rubyball centre Z axis joins rubyball centers “stave coordinate system” data z=0 : edge of stave side A x=0 : centerline of the stave Measurement accuracy: X ~4m Z ~7m Stave 4003 Z rubyballs coordinates from database (no measurements of rubyballs in this dataset) Measurement accuracy: Distance between crosses of the same module Z X R1 R2 R2-R1 Load(db) -412.9170 412.9194 825.836 X rubyballs coordinates R1 R2 Load(db) -5.9656 6.0060

Wuppertal stave “stave coordinate system” data Coordinate transformation: -no transformation in X direction -z=0 is placed in the middle between 2 rubyballs (Zrb-Zedge=3.151mm) Coordinates of centers of modules Angles (rot. around Y) (rad) Zmeas Ztheor Zmea-Ztheo Xmeas Angle -369.9630 -370.3100 0.3470 0.1552 -0.001150 -308.2450 -308.5920 0.3470 0.1050 0.000214 -246.5360 -246.8730 0.3370 0.0648 0.000250 -184.7980 -185.1550 0.3570 0.0333 -0.000058 -123.0930 -123.4370 0.3440 0.0298 0.000986 -61.3880 -61.7183 0.3303 0.0085 0.000843 -0.0340 0.0000 -0.0340 0.0045 0.000307 61.4070 61.7183 -0.3113 -0.1093 0.000468 123.1160 123.4370 -0.3210 -0.0790 0.000590 184.8360 185.1550 -0.3190 -0.0822 0.000538 246.5420 246.8730 -0.3310 -0.0922 0.000759 0.0000 308.5920 0.0000 0.0000 0.000000 369.9780 370.3100 -0.3320 -0.0220 0.000747 X difference (mm) Z difference (mm)

Wuppertal stave “survey coordinate system” data Measurement accuracy: Distance between crosses of the same module Measurement accuracy: X ~62m(???) Z ~7m Z X “survey coordinate system” data have a bad resolution in X direction??? Z positions are close to the “stave coordinate system” ones Stave 4003 Z rubyballs coordinates Angles (rot. around Y) (rad) R1 R2 R2-R1 Survey 825.8 Load(db) -412.9170 412.9194 825.836 ???

Wuppertal stave “survey coordinate system” data Crosses positions Wuppertal “survey coordinate system” data definitely have problems. Are they really the results of survey measurements?

Alignment Sin(200)=0.34 Y 100m X 200 30m Bowed module X Z 100m bow of the module produces a 30m shift of pixel positions in the most sensitive direction (50m pitch). Bad for alignment with required <10m accuracy !!!

Alignment 2D crosses measurements seem not enough for alignment. 3D information is required – bow, deposition angle (deviation from nominal 1.10 ), twist (probably) and glue thickness(probably). Genova stave(no data on twist and glue thickness) Having 3D module positions measurements with ~10m accuracy (seems possible) one needs to measure only a global stave position and stave shape distortions to obtain a good initial pixel position accuracy.

Some conclusions Accuracy of Load<->Survey system transformation is ~10m ( precision of survey checks). Difference in rubyballs distance seems due to Genova CMM problems. Genova and Wuppertal data seem ok (with above accuracy) except for Wuppertal “survey coordinate system” dataset. Problem of measurement procedure or stave? For alignment of Pixel Barrel modules definitely a 3D module position on stave and module shape information are needed. This information can be easily obtained during survey and stored in database ( but it is very difficult to find it in alignment procedure itself).