Magnet Transfer Function Measurements M Guinchard Mechanical Measurement

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Magnet Transfer Function Measurements M. Guinchard- Mechanical Measurement Laboratory H 0 (ω) 12/29/2021

Magnet Transfer Function Measurements M. Guinchard- Mechanical Measurement Laboratory H 0 (ω) 12/29/2021

Outline 1. Introduction to Experimental Modal Analysis (EMA) 2. Previous measurements 3. Measurement in

Outline 1. Introduction to Experimental Modal Analysis (EMA) 2. Previous measurements 3. Measurement in practice 4. HL-LHC String Measurements 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 2

Experimental Modal Analysis (EMA) • A technique to evaluate the modal characteristics of a

Experimental Modal Analysis (EMA) • A technique to evaluate the modal characteristics of a structure • Natural frequencies • Damping • Mode shapes • Why to use the experimental modal analysis? • Anticipate problems related to vibrations • Support to failure analysis • Verification of FEA-models At CERN the technique is particularly important due to the high sensitivity and/or fragility of CERN structures like detectors or magnets. 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 3

Time Output Input Acceleration Force [N] Experimental Modal Analysis (EMA) F F T Time

Time Output Input Acceleration Force [N] Experimental Modal Analysis (EMA) F F T Time Acceleration Force [N] F F T Frequency I(ω) Frequency O(ω) H(ω) 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 4

Previous measurements Q 1 spare magnet installed in stand alone at SM 18 (HL-LHC

Previous measurements Q 1 spare magnet installed in stand alone at SM 18 (HL-LHC Civil Engineering Study) CM-Q 2 CM-IP Jack-IP H 0 (ω) Jack-Q 2 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 5

Previous measurements Q 1 spare magnet installed in stand alone at SM 18 (HL-LHC

Previous measurements Q 1 spare magnet installed in stand alone at SM 18 (HL-LHC Civil Engineering Study) Vertical Lateral 21. 5 Hz 8. 4 Hz H 0 (ω) 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 6

Previous measurements MQXA Cold mass (FEA benchmark for HL-LHC) Vertical Modes 1 st 2

Previous measurements MQXA Cold mass (FEA benchmark for HL-LHC) Vertical Modes 1 st 2 nd 65. 9 Hz 23. 5 Hz Lateral Modes 1 st 2 nd 25. 7 Hz 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 63. 4 Hz 7

Why to perform these measurements? The first bending mode of LHC triplet magnets (around

Why to perform these measurements? The first bending mode of LHC triplet magnets (around 22 Hz) can be easily excited… And we need to anticipate the situation for HL-LHC !!! - HL-LHC Civil engineering study ; Vibrator truck excitation @22 Hz on ATLAS parking ; LHC beam oscillation clearly visible ! - HL-LHC Civil engineering activities ; Compaction of the shaft platform – Compactor excitation around 25 Hz ; LHC beam oscillation clearly visible ! Courtesy of M. Schaumann Injection optics R 2015 a_A 11 C 11 A 10 L 10, Courtesy of Jorg Wenninger 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 8

HL-LHC String Measurements Goal of the measurements : Determine experimentally the transfer functions (TF)

HL-LHC String Measurements Goal of the measurements : Determine experimentally the transfer functions (TF) between the floor (close to the jacks) and the cold mass for several magnets in different configurations : - Standalone magnet → FEA Benchmark. - Magnet interconnected → Effect of additional stiffness needs to be evaluated, considered as negligible today; - Magnet at cold temperature → Effect of additional cryogenic liquid mass needs to be evaluated; Boundary conditions : Measurements must be done with the real supporting conditions as the supports (jacks), fixations on the floor and load repartitions between supports ! The supporting conditions must stay for the overall measurement process ! 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 9 H 0 (ω)

HL-LHC String Measurements Measurement methods : - Standalone magnet → As for Q 1

HL-LHC String Measurements Measurement methods : - Standalone magnet → As for Q 1 spare magnet with hammer excitation; - Magnet interconnected → Floor excitation and the cold mass response will be measured on the floor – No instrumentation inside the magnet - Magnet at cold temperature → Floor excitation and the cold mass response will be measured on the floor – No instrumentation inside the magnet Schedule : The activity is forecaste for 2022 with the following duration: - Standalone magnet → Expected duration for installation and measurements : 3 Days per magnet. Magnet interconnected → Expected duration for installation and measurements : 1 Day per magnet. Magnet at cold temperature → Expected duration for installation and measurements : 1 Day per magnet Analysis and reporting : 3 days per magnet 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard 10

Discussion / Questions 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard

Discussion / Questions 12/29/2021 Magnet Transfer Function Measurements - M. Guinchard