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lucia.trozzo - 18:33 Friday 31 May 2024 (29715) Print this report
Preliminary works to the test the Inertial damping control

Today I started the preliminary work to implement the inertial control in the IP stage. I started by checking the diagonalisation of the LVDT and actuators.  While shaking the IP, I noticed that there was a LVDT sensor coupling. So I decided to try and better decouple the sensing by measuring the decoupling matrix. I measured the TFs along L, T and Y and measured the value of the coupling TFs L_{T,Y}/L_L to the IP resonance along L, LVDT_{L,Y}/LVDT_T , the IP resonance along T and LVDT_{L,T}/LVDT_Y to the IP resonance along Y to calculate the new matrices of S_L. Unfortunately the IP mode along L and T is almost the same and the matrix I found does not make sense. I decided to keep the old matrix.

I then checked that the actuators were correctly diagonalised by moving the inverted pendulum in DC. I found some residual coupling and decided to change the ACT_ALIGN matrix (D). I decided to decouple the actuation by measuring the decoupling matrix pushing the IP in DC. Here the new matrix I found:

D_new=

0.9879 -0.2508 -0.0625
-0.0786 0.9672 -0.1394
-0.0765 0.1148 1.0002

I tested the new matrix and it worked fine. Before starting the diagonalisation of the inertial sensors (ACC and GEO), I intercalibrate the accelerometer signals ACC_{H1,H2,H3} to the geophone GEO_{H1,H2,H3} by measuring the ratio of the spectra GEO_{H1} /ACC_{H1} GEO_{H2} /ACC_{H2},GEO_{H2} /ACC_{H2} at frequency 0.207 Hz. The estimated calibration factors are: cal_H1=0.1482; cal_H2=0.3287; cal_H3=0.1616.
I implemented these numbers in the MEDM and took the spectra of the geophones and accelerometers. Figure 1 and Figure 2 show the spectra of the geophones and accelerometers before and after calibration. It seems that the signals are calibrated.
At this point I measured the TFs along L, T and Y and measured the value of the coupling TFs ACC_{T,Y}/ACC_L ,GEO_{T,Y}/GEO_L at the IP resonance along L, ACC_{L,Y}/ACC_T , GEO_{L,Y}/GEO_L at the IP resonance along T and ACC_{L,T}/ACC_Y , GEO_{L,T}/GEO_Y at the IP resonance along Y to calculate the new matrices of S_G and S_A. Also for the inertial sensors, I found it difficult to decouple L2T and T2L due to the degeneration of the IP mode along La and T. I decided to keep only the row of the matrix related to the degree of freedom Y.

S_A =  [ 1   0  0;    0    1    0;   -0.1320   -0.1707    0.9718]
S_G=[1   0   0 ;   0    1   0 ;  -0.0768   -0.1866    1.0142]

After implementing these into MEDM, I measured the TFs again and the coupling was reduced.

Next things to do:

Measure all the TFs: GEO/LVDT, ACC/LVDT, IS/LVDT to design the phase compensators.

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lucia.trozzo - 18:06 Tuesday 04 June 2024 (29750) Print this report

I continued the preliminary work to put in operation the IP inertial controls. I measured all the TFs: GEO/LVDT ACC/LVDT, IS/LVDT to measure the phase gap below 0.1 Hz and shape the phase compensators as done for the others TypeA IP. The TF along L was fine (see pic 1); the coherence was good and also the GEO/LVDT and ACC/LVDT were fine. Otherwise, for the T d.o.f. Looking at Pic 2, the TF ACC/LVDT (blue line) is noisy. This could be due to residual sensing coupling. As previously said, it is difficult to disentangle L and T. Nevertheless, I did another trial. I added the matrix from Pic 3 to MEDM and measured again the TF: ACC__{L,T}/LVDT_{L,T} and TF: GEO__{L,T}/LVDT_{L,T} again. Along L the TF is the same as before, but along T it is better (Pic4). This matrix seems to help decouple L and T. Then I tried to shape the phase compensators. I added these filters to MEDM as Ph_C and tested them. At this point I built the inertial sensors IS_{L,T} and measured the TF: IS{L,T}/LVDT_{L,T}. The TF along L looks fine (Pic10). The TF along T still has a phase jump around 0.06 Hz (see Pic 9). I don't know why. I need to investigate more.

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