20000922 report
Inclinometry - first with new TCS - signature of wheel flaw ?
Inclinometry was taken for the first time with the new TCS
Datasets HST mean leg temperatures Humidity
start start middle end %
( 20000713_3 cw 02:45 6.8 6.2 5.9 70 )
20000922 cw 10:15 3.4 4.7 6.0 30
The difference between these models is shown below :
- The new dataset contains electronic spikes at azimuths 43, 361
and 373 - these are removed before the creation of the new model.
- With these spikes removed, the formal differences in
(F1,F2,F3)
are described by the rms scatters of
(0.69", 0.64", 0.82")
cf
(0.52", 0.26", 0.41")
previously.
- The new data show a strong ripple of frequency ~8.8 degrees.
Analysis of the raw data show it to arise from the right side of the
antenna. Previous manifestations of this ripple
have been interpreted
(successfully in at least one case) as a diagnostic of a broken wheel,
although subsequent analysis offered an alternative interpretation -
that of slippage of a (permanently) defective wheel generating a phase
error that manifests as a ripple. Slippage could occur if the load changes
- and both the amplitude (about 1" peak to peak, as last time) and the
symmetry
data below tend to support this hypothesis in this case also.
However, some precautionary inspection will be performed soon.
Installation of the spare inclinometer
on the 'radial' arms (beams) going from the central bearing
towards the wheels will allow
unambiguous identification of the wheel involved, although
it is already narrowed down to the right side and the rear-right wheel
was the prime suspect last time around. Fourier analysis
of recent data should show when the damage or slippage occurred.
- Installation of the new track model is pending.
- The symmetry has remained less than
optimal since the central bearing load adjustment on 06 June 2000
- see the plot -
but is currently worse than it has been in about 2 years. This may
be related to the new wheel problem, but in any case may reflect a
separate need for a new c.b. load adjustment.
2000 09 27
The Fourier analysis program (/home/imc/pointing/progs/incft.exe) was
re-written to use the PDA Fourier algorithms (rather than those
from the NAG library, to which we now no longer have updates or access).
Analysis of the difference data below reveals low power even in
older data at the 8.8 deg. frequency expected from a single revolution of
one of the wheels,
but an order of magnitude more power and general overall consistency
in the most recent difference data :
| Difference data (by date) |
  |
TX (Ch1) |
TY (Ch2) |
LX (Ch4) |
LY (Ch5) |
RX (Ch7) |
RY (Ch8) |
| c2000_0922-0714 |
power wavelength o |
0.09 8.8 |
0.15 8.8 |
0.09 8.8 |
0.05 8.8 |
0.10 8.8 |
0.15 8.8 |
| c2000_0714-0701 |
power wavelength o |
0.01 8.8 |
0.02 8.8 |
0.02 8.8 |
0.03 8.8 |
0.01 9.2 |
0.02 8.8 |
| c2000_0701-0607 |
power wavelength o |
0.02 8.8 |
0.02 8.8 |
0.02 8.8 |
0.03 8.8 |
0.03 8.8 |
0.03 8.8 |
Only the Left A-frame Y axis inclinometer sees none of the
8.8 degree ripple, suggesting the problem lies on the right side
of the antenna, as suggested above. Inspection of the wheels is underway.
2000 10 03
A meeting was held to discuss these results and concluded that
the signature is of a wheel misalignment rather than defect - link
here.
Fourier transform analysis of inclinometry data will provide
a useful method of monitoring the problem.
Iain Coulson
22 Sep 2000 - updated 09 Oct 2000
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