• High Power Laser and Particle Beams
  • Vol. 34, Issue 4, 044001 (2022)
Xudong Zhang, Wenjun Chen, Xiaodong Zhang, Guozhen Sun, Bin Zhang, Shaoming Wang, and Jiandong Yuan
Author Affiliations
  • Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China
  • show less
    DOI: 10.11884/HPLPB202234.210260 Cite this Article
    Xudong Zhang, Wenjun Chen, Xiaodong Zhang, Guozhen Sun, Bin Zhang, Shaoming Wang, Jiandong Yuan. Analysis on deformation of partial control network of particle accelerator[J]. High Power Laser and Particle Beams, 2022, 34(4): 044001 Copy Citation Text show less
    Schematic diagram of three-dimensional coordinate system transformation
    Fig. 1. Schematic diagram of three-dimensional coordinate system transformation
    SESRI Experimental Terminal 2 Control Network
    Fig. 2. SESRI Experimental Terminal 2 Control Network
    Residuals and weights of each point after the initial adjustment
    Fig. 3. Residuals and weights of each point after the initial adjustment
    Residuals and weights of each point after the second adjustment
    Fig. 4. Residuals and weights of each point after the second adjustment
    calculationstranslation factor/mmrotation factor/(°)factornumber of iterations
    ΔXΔYΔZαβγk
    100000011
    0000001
    25555551.002947
    55554.999 99951.002
    31010101010101.0011005
    101010109.999 999101.001
    42020202020200.9991085
    2020202020200.999
    54040404040400.9981521
    404039.999 9994040400.998
    66060606060600.9971068
    60606059.999 99960600.997
    Table 1. Simulation calculation
    pointthe first phase (2021.4)the second phase (2021.6)
    X/mm Y/mm Z/mm X/mm Y/mm Z/mm
    L55−5092.17879.6214895.656286.72−15526.63821.79
    L57−2 261.04879.2817717.092815.70−17509.32822.15
    L59−3120.62879.2221412.56−520.04−15701.26822.40
    L60−4107.95−821.7224779.41−3505.58−13857.21−878.36
    L61−4107.01877.2024777.54−3503.76−13858.44820.70
    L62−4074.18−817.6727037.53−5692.02−13291.53−874.05
    L63−4077.77876.9127033.99−5687.46−13288.83820.64
    L64−6897.19−773.8729870.60−7676.14−9818.57−830.23
    L65−6897.30880.7229867.91−7673.23−9819.01824.42
    L67−9746.56894.0232716.15−9665.07−6316.66837.73
    L68−13217.29−822.3831985.43−8041.08−3163.51−879.28
    L69−13215.11879.5931991.11−8046.88−3164.01822.76
    L70−16050.40−820.9229166.76−4572.37−1178.27−878.59
    L71−16047.74874.5329165.73−4571.81−1180.86816.96
    L72−18878.70−809.5226339.60−1096.73800.14−867.90
    L73−18879.30879.6526340.53−1097.19801.22821.38
    L74−21711.32−841.1523519.472373.332784.62−900.23
    L75−21710.28846.7623519.112373.622783.72787.79
    L76−23062.45−815.8620935.805222.753403.02−875.45
    L77−23061.11882.0920947.335211.703405.02822.63
    L78−22368.90−818.9619093.136816.012245.99−878.70
    L79−22309.74883.2519037.436854.432174.44823.70
    L80−19511.28−781.7216233.698816.34−1267.34−841.25
    L81−19509.35875.0016238.178811.89−1267.75815.53
    L82−16684.40−808.8213405.9210794.26−4742.76−868.25
    L83−16690.55881.7713407.8010794.50−4735.99822.43
    Table 2. Two-phase observations of SESRI Experimental Terminal 2
    calculationtranslation factor/mmrotation factor/(°)factor
    ΔXΔYΔZαβγk
    SA−18 397.5658.425 070.3189.974 0374.637 72179.96750.999 926
    this article−18 397.5558.4025 070.3189.974374.637 71179.967 80.999 926
    difference0.009 4−0.001 50.000 30.00027−0.000 010.000 234−0.000 000 4
    Table 3. Fitting parameters obtained by two methods
    Xudong Zhang, Wenjun Chen, Xiaodong Zhang, Guozhen Sun, Bin Zhang, Shaoming Wang, Jiandong Yuan. Analysis on deformation of partial control network of particle accelerator[J]. High Power Laser and Particle Beams, 2022, 34(4): 044001
    Download Citation