20010720 report
Transit step : measures from the sky and from inclinometry
Summary
Measurement of the 'transit error' step-size can be made using
inclinometry. The initial measurement agrees with contemporaneous
measures on the sky. The method
provides a daytime method of monitoring this characteristic.
The new measures also suggest that the corrective algorithm
is currently overcorrecting the defect.
The
most recent attempt to measure the 'transit'
step-size by tracking an astronomical source through transit
suggested that the 8" step being used was an overcorrection,
but the data were of a rather poor quality. It was suggested at
that time that a repeat experiment was needed : here it is :
The data clearly show an overcorrection by the algorithm by about 5".
The curve fitting suggests that the (semi-)amplitude at the
horizon be reduced from 4.0" to 1.3". At this level the effect
is almost negligible, but since its size may vary with antenna
balancing we cannot henceforth disregard it, sadly.
Allsky pointing was also performed the same night. The behaviour
of the elevation residuals as a function of azimuth is shown
below :
The data show a 4.7" difference in elevation residual between east
and west, in agreement with that measured by the transit
tracking experiment above. Adopting an average of these 2 figues of 4.8" -
or 2.4" in the semi-amplitude, and therefore 2.7" at the horizon -
the value of SCURVE.AMP in the telescope model was changed from 4.0" to
1.3" on 20 July - i.e the full-amplitude of the defect is now expected to
be 2.6".
During daywork on July 19, an inclinometer was placed on the TMU and the
telescope tipped over to about 10 degrees and the TMU positioned so that
the inclinometer was horizontal. A fictitious source was tracked through
transit. The elevation range was such that the inclinometer stayed
within 200" of the horizontal, and therefore, within its range of
utility. Adopting a scaling factor of 20mv/" as determined
for all our inclinometers, the tilt of the TMU in acrseconds
is plotted below as a function of azimuth (with a zero-point of 180
degrees). Click on the image for a better view :
The inclinometry-tailored version of the telescope control
software omits application of the corrective algorithm.
A defect is visible at azimuth 180.2.
A quadratic curve was fit to the data and a portion of this fit
is shown below :
. . . and the residuals of the data about the curve are shown next :
Despite the noise at each end of this segment, and the uncertainty
in finding the quadratic curve that best fits the data immediately
surrounding the defect - and which impacts the baseline through
this segment - the data may be interpreted
as revealing a 3" (full-)amplitude step, centered at 180.2, and
of semi-width 0.1 degrees. The (full-)amplitude at the horizon
is then 3"/cos(10) which is still essentially 3", in very good
agreement with the measurements on the sky reported above.
Conclusion
The inclinometry and sky measurements agree in their estimate of the
current amplitide of the 'transit-error' step-size (now ~2.6").
The inclinometer may be adopted as the routine method for monitoring of
this defect.
Acknowledgement must be made that Adrian Webster (UKATC) first suggested
this inclinometry technique. Thanks also to Firmin for yet another
adjustment to the inclinometry software, and to Peter for help with the
levelling.
Iain Coulson
Latest Update : 21 Jul 2001
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