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SLR-Mail No.59

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Date:1997-05-09 12:00:00
Sender:Natalia Parkhomenko <[Mailed Andy Sinclair <ats@ast.cam.ac.uk>]>
Subject:[SLR-Mail] No. 59: Request for ZEYA tracking
Author:Natalia Parkhomenko
Content:********************************************************************************
SLR Electronic Mail 1997-05-09 12:00:00 UTC Message No. 59
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Author: Natalia Parkhomenko
Subject: Request for ZEYA tracking
Subject: Appeal to Global SLR Network



(via A.T. Sinclair)

Dear collegues,
Up to now six SLR stations of the world SLR society have done
successful ranging sessions of the ZEYA satellite. We are very
grateful to everyone who sent us observation data.
In addition to previously given information on the ZEYA
satellite we are now sending you additional information on the
refletion model of the ZEYA retroreflector system. The SLR
measurements are made for solving of space geodesy problem and radio
navigation systems calibration, as well as for testing of technical
solutions adopted in the precision WESTPAC satellite design which is
to be launched in accordance with the WPLTN program.
To achieve minimum target error of ranging which is determined
by the retroreflector system design and the accuracy in their
alignment relative to the ZEYA satellite mass center, for any
direction of the incoming laser beam only one retroreflector is used.
This is made by limiting the field of view (FOV) of each
retroreflector by means of cylindricals bafflers, so that each single
retroreflector has a FOV of 35 deg.
The number of retroreflectors we managed to place on board of
ZEYA is 20, which is three times less than on the WESTPAC satellite.
All retroreflectors are positioned at equal distances from the space
craft mass center and so that all perpendiculars to the
retroreflector input aperture are passing through the satellite´s
center. The systematic displacement is here 419 mm.
As follows from the radio frequency measurements analysis, the
ZEYA satellite is now on a sun - synchronous orbit with an apogee 499
km, perygee of 471 km, and inclination of 97.27 deg. The spacecraft
is rotating with a rate of 65 rpm around its axis directed towards
the nadir point, when the satellite is approximetily at 78 deg. N
latitude and 24 deg. E longitude.
As a result the total FOV all ZEYA retroreflectors is covering a
little bit more than one third of all possible directions of the
incoming beam, and the dead zones are positioned so that the
spacecraft´s rotation causes no more than two or three gaps in return
signals, in average no more then two gaps per three radiated laser
pulses.
Because of the spacecraft design features, there is some
irregularity in the retroreflector positions. This irregularity may
possibly cause some reduction or even temporary loss of return
signals. The satellite´s rotation axis precession may be a cause of
irregular return signal strenghts by different passes. Such
information is for us of great value.
To avoid long intervals of return signal abcence because of
stroboscopic effects, the best pulse repetition rate by ranging
should be 5 to 10 times more than the ZEYA spacecraft rotation rate,
and so should be 5...10 Hz.
Besides the ivestigation of the possibility of achieving the
highest range measurement accuracy, the destination of retroreflector
on board of ZEYA is also to continue investigations of the possible
Fizeau effect influence on the total velocity aberration angle.
Therefore on board of the the ZEYA satellite retroreflectors are
placed with narrow, nearly diffraction-limited reflection patterns,
having a FWHM angular width of approx. 5 arc sec at 532nm at normal
incidence.
The retroreflectors are made of fuzed silica with a refraction
index of 1.461; the reflecting surfaces of each cube corner are
aluminium-coated; the cube corner prism height is 18.9mm. The
effective aperture diameter of the the retroreflector, determinied by
the inner diameter of the cylindrical baffle, is 26.9 mm.
In case of the Fizeau effect influence, these retroreflectors
must partly compensate the velocity aberation; the remaining velocity
aberration shold be 1.7 to 3.4 arc sec, and the narrow (5 arc sec)
reflection pattern should help to get sufficiently stronger return
signals.
If there is no influence of the Fizeau effect, the signal
reflection towards the ground station will be possible only for slant
incidence angles at the retroreflector, when its reflection pattern
is broadened along the satellite´s flight direction; then the return
signal strenght will be an order of magnitude less than if the Fizeau
effect compensation is present.
We are very lager to know the details of the satellite
observation condition in different practical situations of ZEYA
ranging, especially information on the passes where data on every
part of the observation zone are present.
Since the begining of May the ZEYA will be visible in the
reflected sunlight during nighttime for the SLR stations located in
the northern hemisphere.
Dear collegues, regarding the above any your messages, including
session features, details of signal strenght measurements, etc.,
would be very useful and could help to achive better accuracy and
effectivity of retroreflectors for future satellites.
We ask you:
1. To take part in ZEYA observations during May and June of this
year.
2. To send us data in the FULL RATE format.
3. To report the parameters of SLR stations making ZEYA
observations, necessary for signal energy calculations (for
comparision with measurment data).
4 To report any data on the return signal levels, absolute
and/or compared to other satellites.
5. To report any features (including negative onse) of the
measurement sessions.

With best regards
V.Shargorodsky



[Mailed From: Andy Sinclair ]
[Mailed From: ”Natalia N. Parkhomenko” ]

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