The wheel lift-off theory as to the origin of "spikes" in the inclinometry difference plots.
Justin Greenhalgh, Jan 25 1999
P/001/21/RJSG (1999)

This note has been assembled from a couple of emails, basically to provide a note for posterity as to how our thoughts were going at the time.

1. Statement of a theory to explain the "spikes" in the inclinometry data.

The antenna is a very stiff structure, and is nominally supported on five points (the central pintle bearing and the four rollers). Because it is so stiff, any variation in the height of the support points, or any thermal distortions in the structure, will have a large effect on the load distribution between the five support points. Study of the figures for stiffness and for thermal distortion show that:

The nominal wheel loads, measured by a strain gauge system of dubious accuracy, are as follows:

wheel 1, front right : 0.66 tonnes
wheel 2, back right : 2.1 t
wheel 3, back left : 3.3 t
wheel 4, front right : 0.7 t

Allowing for the known track profile and the location at which the loads were measured, we would expect the load on wheel 1 to decrease to zero at two points around the track in the absence of any thermal effects.

Furthermore, a prediction of the places where the wheels would lose load, and the extent to which they would lift off, matches the patterns seen in the spikes both in location, magnitude, and general form.

The explanation of the "spikes" is that at times the weight of the telescope is removed from the front wheels by unevenness in the track, the effect being exacerbated intermittently by thermal distortions in the structure of the main frame. When the weight comes off a wheel, the relevant corner of the antenna no longer follows the track profile and so a change in measured profile results. The number of spikes and their size depends upon the magnitude of the thermal effects and the current height of the central bearing relative to the track. The overall pattern and relative size of the spikes is given by the track profile.When the weight comes off a wheel, the wheel itself remains in contact with the track and a gap opens up between the flanged bearing (item 13, OR180051) and its mating part (?Bearing housing yoke, item 3 OR180051). The weight of the roller, motor, and yoke is sufficient to keep the roller in contact with the track and prevent it from spinning.

The "asymmetry" would appear whenever the wheel loads were light, because the inclinometry would be dominated by rear-wheel effects which do not repeat at 180 degrees.

2. Possible tests of the theory were:

S = (dTc - dTn) - W
Where
dTc = delta T when central bearing was adjusted
dTn = delta T now
W = weight offset introduced by central bearing adjustment (or by adding weights)
S = spike height
So we expect to see a set of straight lines of S vs dTn, a different one for each central bearing adjustment.
 3. Possible solutions to the problem were identified as follows:  General agreement was that the first solution was the most appealing although we should revisit if it turns out to be harder than we thought.

4. Analysis of the "Assumptions, Observation, etc" paper in terms of this theory.