J. Kissel I've taken new, more comprehensive B&K hammer response measurements of the H1SUSPRM and H1SUSPR3 cages, now that they have newly installed (what I'm calling) Venetian Baffles (see attached HAM2_NewBaffling_WithLabels.pdf for names of baffles) whose installation was finished last week LHO aLOG 39170. These baffles have pretty high-Q, low-frequency drum-head / longitudinal resonances (roughly aligned with ISI / IFO Y axis). PRM Upper: 42.38 & 46.75, 91.00 PRM Lower: 42.38 & 46.75, 75.62 PR3 Upper: 36.75, 75.6 PR3 Lower: 36.75, 83.12 My guess is that the lower frequency of the modes are the baffles bending in longitudinal in concert on the Venetian bracket, and the upper frequencies are their individual longitudinal modes. This mode-shape guess is based only on intuition, and that the lower frequency modes are seen in both upper and lower excitations. The cage's transverse modes appear to be relatively unaffected by the new baffles. I'm little surprised it hasn't stiffened up any of the transverse modes; oh well. These resonances have been identified by comparing against the history or cage resonance measurements for each of the SUS -- see the three pdfs: 2017-10-30_H1SUSPR3_CageResponse.pdf 2017-10-30_H1SUSPRM_CageResponse.pdf 2017-10-30_H1SUSPRMvsPR3_CageResonance_Comparison.pdf Note, also new with these measurements -- data out to 1.1 kHz. The former data is from LHO aLOG 6014 -- VA ON vs OFF data for H1SUSPRM and H1SUSPR3 LHO aLOG 8654 -- Former Cage Baffles on H1SUSPR3 Photos attached (and remaining HitLocations.pdf) are for historical reference for future repetition.
From Stephen and Norna
We (Stephen, Norna, Calum, Cormac) have done further experiments in the lab at Caltech to better understand the effect of the addition of the "Venetian blind" baffles ( D1700256 HSTS BAFFLE ASSY.PRM), on an HSTS and to help with the interpretation of the results seen at LHO.
A few caveats which should be noted:
a) We only have a bare structure - no vibration absorbers, hanging suspension, cables etc. attached. Also not as well dogged down as on site due to potential interference with baffle (our HSTS is not on a spacer). We have included baseline results displaying excitation of this structure without baffles mounted for comparison, see figures 2a and b described below.
b) We only used one baffle panel - so it was either attached at lower or upper position. See figure 1 for set-ups.
Basic findings
1) We show with and without damped baffle in upper position, exciting at top of structure in longitudinal (beam) direction and transverse. Basic conclusion, we do not see noticeable new resonances when exciting structure itself. See figures 2a and 2b
2) We only see extra low frequency ( ~ 40 Hz in our case) resonance introduced by baffle when directly hitting on the baffle. It is not seen when excitation is done to the structure itself. It is also only seen when hitting the baffle in its upper position, not in the lower position. See figure 3 for upper position results.
*We strongly suggest that if time permits, a test where the structure itself is hit in the longitudinal (beam) direction is done at LHO to see if this finding also holds for the PRM suspension now in situ.* From our experience we expect those low frequency peak(s) not to appear or least to be less prominent when the structure itself is excited.
3) The viton O-rings in the attachment units make a significant beneficial difference to the behaviour. Adding a baffle without viton introduces extra features which are suppressed or damped with the introduction of the viton.
See figures 4 (upper) and 5 (lower) baffle results.
4) The viton also adds some damping to the original structure resonances, apart from the first two flagpole resonances at 65 Hz (longitudinal) and 75 Hz (transverse) for our set-up. The dominantly torsional mode at ~160 Hz in our set-up shows some damping, as does the ~350 Hz feature. This can be seen particularly in the transverse results.
See figures 6 (upper) and 7 (lower).
5)We also did some investigations of different tightening levels corresponding to different levels of compression of viton O-rings within the two different flavors of attachment unit, D1700232 and D1700236. Basic result: the system is quite tolerant to different levels of tightening,with similar results over a range from hand tightened plus 1/4 turn to hand + full turn.
We will write this up more fully on the DCC at T1700473, including posting all data sets.
I have added one further set of comparison traces. In figure 8 we show the effect of including the damping O-rings in the baffle attachment units, where we are now comparing the results when hitting directly on the baffle in its upper position, rather than hitting the structure as shown in figure 4. We see again that the damping makes a significant beneficial difference.
WP7195 Hugh, Dave:
Hugh reconnected the CD_[V2,H2]_V inputs to the 3rd ADC chans 2,3 (they were grounded). The model was recompiled, installed, and restarted at 12:04 PDT. No DAQ restart was needed. I cleared various IPC errors on receivers of ISI-HAM5 sender channels post-restart.
Travis and I walked down X-beam manifold in chamber to investigate unknown contamination on the interior wall that Betsy had spotted, a few feet away from oplev flange/baffle. We found two dark brown/black spots near the top/roof of tube, each about the size of a quarter. I was able to scrape some off with a little flat head screw driver and then wipe with IPA wipes to improve/reduce the spots (grinding is needed to remove all). Before and after pictures attached. I wiped until there was no evidence of contaminate on wipe. Then we noticed the side wall was splattered with the same material (photo attached). Its first layer comes off by scraping with a tool, but we did not spend time scraping all 50-some spots. We can go back in to scrape these other spots, but I would first like to send sample in for analysis.
Note that we have seen evidence of higher pressures in XBM (compared to YBM) when it's isolated from beam tube. Could be outgassing from this material. Travis and I inspected YBM and did not find this contaminate.
JPL results here: https://dcc.ligo.org/E1700405
Late last week, we took control of AHU 1 & 2 in the LVEA with the new HVAC controls. This has been a long process and is actually still on going in so far as we still have to take control of AHU-3. I have been monitoring the LVEA all weekend and in an effort to stabilize the temperatures even more, this morning I have increased the air flows in the LVEA from ~12,000 cfm per air handler to ~18,500 cfm. This has already made a considerable improvement and I will continue to monitor.
MEDM screens have been updated.
Everything appears to be "business as usual". There are very marginal downward trends in the osc pressures and amp flow.
Laser Status:
SysStat is good
Front End Power is 35.89W (should be around 30 W)
HPO Output Power is 153.9W
Front End Watch is GREEN
HPO Watch is GREEN
PMC:
It has been locked 10 days, 18 hr 36 minutes (should be days/weeks)
Reflected power = 23.33Watts
Transmitted power = 48.29Watts
PowerSum = 71.62Watts.
FSS:
It has been locked for 0 days 4 hr and 47 min (should be days/weeks)
TPD[V] = 2.786V (min 0.9V)
ISS:
The diffracted power is around 2.7% (should be 3-5%)
Last saturation event was 5 days 23 hours and 10 minutes ago (should be days/weeks)
Possible Issues:
PMC reflected power is high
TITLE: 10/30 Day Shift: 15:00-23:00 UTC (08:00-16:00 PST), all times posted in UTC
STATE of H1: Planned Engineering
OUTGOING OPERATOR: None
CURRENT ENVIRONMENT:
Wind: 17mph Gusts, 12mph 5min avg
Primary useism: 0.06 μm/s
Secondary useism: 0.28 μm/s
QUICK SUMMARY:
14:18 Kissel in early to do some more B&K hammering in HAM2
15:33 (HFD) MSA on site for Bubba
16:05 Kissel out for vent meeting
16:12 more MSA on site for RFAR testing
16:44 Gerardo is in the HAM5 area
16:55 Chandra going in chamber with Betsy and Travis - X Manifold
16:57 Travis heading out to biergarten
17:10 Betsy ou to he biergarten
17:15 Gerardo is out
17:25 Gerardo and Peter into Optics lab
17:27 Fil out to LVEA to put plastic conduit arounf fibers that were pulled on Friday
17:43 Job Shadow student on site
17:44 TJ heading out to HAM 4/5 area.
17:55 Richard and shadow student into LVEA for tour
18:08 Greg into LVEA to take measurements for TCS table
18:18 Kyle to the Y end station
18:27 Noise Eater out of range alarm
18:54 Travis out to reset the Noise Eater
19:13 I will be turning ops over to Corey so I can assist with HAM2 in-chamber work
Members of the Stochastic Group have expressed interest in magnetic coupling for estimates of Schumann Resonance coupling during O2. Automated coupling functions for all injections are not quite ready to be posted at pem.ligo.org, so we are going ahead and posting site-wide magnetic coupling functions from the August 2017 PEM injections here.
Magnetic field injections were made at multiple locations in all 3 LVEA/VEAs and electronics rooms. The LHO injection locations are shown in the first figure below and the injection locations at LLO are similar. The code (started by Julia Kruk and completed by Philippe Nguyen) used the following procedure:
1) Coupling functions (meters of DARM per Tesla) were calculated for each magnetometer (the quadrature sum of the axes), for each of multiple injections in the local area (LVEA/VEA or electronics bay). The coupling function is the DARM signal divided by the magnetometer signal.
2) The coupling functions for each injection for each sensor were narrowed down to a single coupling function for each sensor by picking the minimum coupling factor at each frequency. Selecting the minimum coupling factor eliminates excessively high upper limit coupling factors for sensors that are far from the injection and coupling sites and thus detect small fields for large DARM signals.
3) For the site-wide maximum coupling function given here, the maximum coupling factor at each frequency is picked from the coupling factors for all of the sensors on the LHO/LLO site.
Of course, site coupling will be the combination of coupling at all coupling locations within each site - this is just the largest of these at each frequency. We think that the largest coupling factor is probably a fair estimate for the site because other coupling locations with lower couplings can increase or decrease the overall coupling. But the coupling functions here could be multiplied by a factor like sqrt(2) to be conservative.
Other issues:
There was a large change in magnetic coupling during O2 at LHO, as noted in: https://dcc.ligo.org/DocDB/0144/G1701613/002/GenevaTalkSm.pdf , and we don’t know when it happened. I think that, as Schumann Resonance coupling becomes more important, we should probably push for a continuous magnetic injection at each station, like a calibration line, or at least weekly injections. Back when our magnetic coupling was dominated by permanent magnets on the test masses, it didn’t change for years. But now we tend to be dominated by coupling to cables, and this can change dramatically as electronics and cables change. After talking with Richard M., my best guess is that the change happened May 16th when the ITM ESD power supplies were changed, but that is just a guess. For S3 it might be a good idea to set up a single continuous line injection at the LHO corner station in order to better study coupling variation.
Another consideration for Schumann Resonances is the eddy current shielding due to the steel skin of the buildings. This is not included in these coupling functions because the injection was from within the building. We should measure this, but assuming it is the same as for a chamber, it would be about: 1/sqrt(1 + (f/20)^2), or a factor of 0.93 at 8 Hz and 0.55 at 60 Hz.
Philippe Nguyen, Julia Kruk, Anamaria Effler, Robert Schofield
I noticed a pressure "bump" at Y-end recently and have now confirmed that the ion pump mounted at BT port Y2-8 has been off for the past few days. Today's troubleshooting including re-enabling the High Voltage output. This resulted in power limited (700V @ 0.5 amp) energization (no ion pumping while inadequately energized). Next, the HV cable was moved to he other HV channel with a similar result. The controller-end of the HV cable was disconnected and a VOM used to measure the cable+pump resistance (2.5 Mohm, insufficient output voltage of the meter makes this test "almost" useless). The HV cable was reconnected to the controller and the pump-end disconnected. In this configuration, the controller wouldn't output HV as the cable connector shield wasn't grounded and, it would seem, the cable isn't shorted. I noticed that the pump-end of the HV cable was noticeably "warm" after applying 700V at 0.5 amps. This observation combined with the interpretation that the cable or pump-end connector aren't shorted indicates that the low resistance is internal to the pump itself. Ahhh! The fabled "whisker" theory. Monday, we will adapt a custom HV cable and use the "Big Gun" 10,000V 600 watt power supply to, hopefully, vaporize any troublesome whiskers that have formed between the electrodes.
The pump is probably in a condensing environment at times so there may be conductive buildup on the pump feedthrough or the interior of the cable connector.
I would be surprised at whisker buildup as that pump has not pumped significant gas loads.
Also, I would fake out the interlock at the pump and make sure you can get high volts on the cable alone.
Yes, I'll disconnect the pump-end connector and then ground the shield. This should satisfy the controller and get it to energize the HV output. As John W. points out, the pump-end connector shorting would explain why it was warm and is much more likely than the pump being internally shorted when considering the pumps torr*L exposure history.
(Peter K, Gerardo M)
New OFI table is suspended in cage, some components on the cage assembly were loose, they were re-torqued. The missing corner bracket was installed, and we replaced a couple of bad 1/4-20 flat head socket head cap screws.
Next, table balance and suspension damping.
What is the tan colored staining from? These are Class-A parts?
J. Kissel, C. Vorvick I've processed the data from last week's first B&K adventure into HAM2 which included the HAUX (a.k.a. HAM Auxiliary Suspensions, a.k.a. IMs or Input Mirrors) (LHO aLOG 39096). Recent efforts tightening and torquing the cage bolts to spec (e.g. LHO aLOG 38808) has helped increase the resonance frequencies and Qs of the first bending modes of cage to ~170 Hz in Longitudinal and 220 Hz in Transverse. These modes are significantly better* than those at L1. *Here, by "better" I mean well-defined, high resonance frequencies, and features are similar between suspensions. The data I use from LLO is the same as posted in LLO aLOG 3948 for IMs 1,2, and 4 from their 2012 vent, and the more recent LLO aLOG 25919 for the problematic IM3 from 2016. After discussing with Cheryl, there are several differences that elucidate this difference. (1) While LLO has used the "IO" dog clamps of several varieties (D1100640), LHO has used the champhered-ended "SUS" dog clamps (D1100641). These create a more well-defined contact point. (2) In addition, the layout of dog clamps around the base of the cage is significantly different; LHO revised the original layout, seeing how unstable the originally prescribed appeared. See table below for comparison of layouts: Current Former Original Revised Name Name Layout Layout (LLO) (LHO) IM1 SM1 D1200623 T1400742 IM2 PMMT1 D1200625 T1400743 IM3 PMMT2 D1200626 T1400744 IM4 SM2 D1200624 (not revised) Further confirming the difference -- IM4's clamping configuration does use the IO clamps, in a similar arrangement, and the frequency responses of the cage between H1 and L1 look quite similar -- in Longitudinal, but Transverse remains quite different. In light of this data, I propose two things: (1) At the earliest convenience (if there is still such convenience left), we should ECR Cheryl's improvements, implement them at LLO, and update documentation such that India gets similar benefit. (2) Now that we've stiffened up the resonances, they've become higher Q. We should consider shoving some viton in between the suspension cage, and, say, each of its black-glass cage baffles. It shouldn't need much.
IM4 would likely benefit from additional SUS dog clamps. I'm looking into where they could be installed.
I'm also looking in to options for viton.
The baffles are SiC, and it may be possible to install viton in direct contact with them, but the brittle nature of SiC may not allow for this.
A possible location for installing viton is on the stiffening plate in the cage, which has two 1/4-20 bolt holes available on all of the IMs. These bolt holes are above the SiC baffles, so not near the beam. If viton installed here can effectively damp the resonances, this would be a minimal change to the IM cages.
I've attached a couple drawings of the IM cage stiffening plate and a picture of IM4 showing the available bolt holes.
Here are pictures from my original SUS dog clamp installation on IM4, before the SiC baffle was installed.
J. Warner, S. Appert, T. Shaffer
We had some unexpected time to work on HAM2 baffles after some FedEx kerfluffles, so Jim and I went into HAM2 with some freshly baked parts and an engineer (just in case things got out of hand). This work went really fast with the three of us and we managed to finish up PRM, the last beard baffle, align all of the panels we needed to, and then torque and cap everything. I went into the beam tube to work from there and to be the eyes to align, and of course, I wiped on my way out.
We left the table baffle that sits in front of PR3 off the table for now, but with the mounts bolted down. This way the other crews that still need to do work have a little bit of space to work and won't scratch anything, hopefully. To place this last panel will take only a minute or two so we can easily do it after the major work is all done.
Pictures to come.