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PEM (Center)
tatsuki.washimi - 11:07 Tuesday 30 April 2024 (29357) Print this report
IFI Sack hammering

[YokozaWashimi]

We moved the 3-axial accelerometer and the impact hammer from the OMC area to the IFI area.

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tatsuki.washimi - 15:54 Thursday 02 May 2024 (29383) Print this report

[Komori, Tanaka, YokozaWashimi]

We performed the Hammering test for the IFI stack (+X, +Y side stack).

  • optical table -> optical table
  • top stack -> optical table
  • middle stack -> optical table
  • bottom stack -> optical table
  • base plate -> optical table
  • ground -> optical table
  • nothing -> optical table (as a reference)
  • base plate -> base plate
  • ground (leg) -> base plate
  • ground (leg) -> ground
  • ground (concrete) -> ground
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tatsuki.washimi - 19:14 Monday 06 May 2024 (29399) Print this report

I estimated the transfer function from the base plate vibration to the optical table vibration, by
TF(impact@base -> ACC@table) / TF(impact@base -> ACC@base)

I also did the same calculation for the Ground (z) ->Table case, but the results became over 1 for many frequencies. I need to investigate whether my analysis is correct or not...

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tatsuki.washimi - 18:14 Friday 10 May 2024 (29464) Print this report

I'm updating the hammering test analysis.

Generally, one event should be a single pulse, and multiple pulse events due to bounding need to be removed from an analysis.

It can be realized by using a time-over-threshold (ToT) automatically. In this case, I request it be less than 0.02s.

After choosing single pulse events, the transfer functions became smooth and the coherence became larger.

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tatsuki.washimi - 18:27 Friday 10 May 2024 (29465) Print this report

Same analysis for other measurements.

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tatsuki.washimi - 18:45 Monday 13 May 2024 (29482) Print this report

I plotted the transfer functions from the impact hammer to the accelerometer, by selecting the single pulses and requesting the coherence >0.5. 
The results when the accelerometer was put on the ground were not good coherence and difficult to use.

I also evaluated the transfer functions from the Base vibration to the Table vibration, by

H(a_\mathrm{B}\to a_\mathrm{T}) = \frac{H(F_\mathrm{B}\to a_\mathrm{T}) }{H(F_\mathrm{B}\to a_\mathrm{B}) }

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