The effect upon azimuth of the 102
m shims is expected to be
daz = ROLL * sin(el) + YAW * cos(el)
with a convention for the signs of ROLL and YAW :
daz = + 1.30
* sin(el) - 3.05
*
cos(el) for wheel 1
daz = + 1.30
* sin(el) + 3.05
*
cos(el) for wheel 2
daz = - 1.30
* sin(el) - 3.05
*
cos(el) for wheel 3
daz = - 1.30
* sin(el) + 3.05
*
cos(el) for wheel 4
These formulae yield expected values that may be compared with the 6 measures
tabulated above (sect 5.3.3). The difference is -0.06 +
0.41
, which appears to validate the formulation.
Alternately these equations might be written
daz
= f
* ( +- 1.30 * sin(el) +- 3.05 * cos(el))
if there are scaling factors f
for each wheel.
However, the formal solution
(f
= 0.32 + 0.45,
f
= 0.88,
f
= 0.88,
f
= 1.5 + 1.7)
appears useful only for wheels 2 & 3, and the further assumption of a global
value of f yields 0.90 + 0.94, similarly unconstrained by the
poor elevation coverage of our data.
If there are factors affecting ROLL and YAW separately, ie
daz = +- 1.30 * fR * sin(el) +- 3.05 * fY * cos(el))
where fR and fY are the efficiencies with which tilts in the A-frame
are transmitted to ROLL and YAW, we may determine fR & fY by solving the
6 equations simultaneously.
wheel 1 : 1.30 * fR * sin(62.3) - 3.05 * fY * cos(62.3) = 0.00
wheel 2 : 1.30 * fR * sin(53) + 3.05 * fY * cos(53) = 2.53
wheel 3 : -1.30 * fR * sin(63.5) - 3.05 * fY * cos(63.5) = -2.22
wheel 4 : -1.30 * fR * sin(49.4) + 3.05 * fY * cos(49.4) = 0.30
wheel 4 : -1.30 * fR * sin(68.4) + 3.05 * fY * cos(68.4) = -0.24
wheel 1 : 1.30 * fR * sin(55) - 3.05 * fY * cos(55) = -0.44
. . . give (fR, fY) = (1.00,0.78), with a s.e. of
0.16
.
NB: It is problematic to assign any A-frame tilt to one wheel rather than
the other. This is of no consequence for del, but clearly impacts
the expected value of daz.