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44<br />
Annex p1 Optical system<br />
B. 1 Background<br />
This dcsign explorcs whnt might be achicvrd tising existing<br />
space or military quality subsystems to build a high<br />
rcsolution imaging systcm. The spacecraft has a space-<br />
qualifird vcrsion of a commcrcial tclcscopc rnountrtl such<br />
that it can bc rotatcd about an nxis aligned within - lo of<br />
the dircction of travcl. A lincscan imager is niountcd at thc<br />
focus of L)ic tclcscope. aligncd so that it swecps a swath<br />
along he direction of travel (puslibroom).<br />
The dcsign prcscntcd hcrc can provide 2 kin square imagcs<br />
with a spatial resolution of I m. The image region is<br />
selected by rotating thc tclcscopc for tlic acrosk-track<br />
dimcnsian and sclccting thc tirnc of rccording for he<br />
along-track dircction. Thc position of the satcllitc nlust be<br />
dcterminrd to - 50 m in all thrcc dimensions and the<br />
orientation of the tclcscoF to - I mrad in thrcc dirrctions<br />
to permit the centre of thc irnagc IO hc sclcctctl to an<br />
accuracy of - 0.5 km.<br />
a 8.2 Telescope and sensor<br />
The primary optical systcni is a spacc-qualirictl vcrsion of<br />
tile standard Qiicstar 12" telcscopc. Thc kcy piiraiiiclcrs of<br />
its specification arc:<br />
0<br />
-. rcsolution:<br />
. focal Icngth:<br />
- apcrturc:<br />
0.38 arc scc<br />
4.57 2 ni m<br />
30.5 iii rn<br />
- dimensions: -I ni long. -3.50iiiiii tliamctcr<br />
-<br />
~<br />
mass:<br />
vibration tolerance:<br />
-SSkg<br />
I0g<br />
I '<br />
- moterial: invar<br />
. price: - 5 200 k<br />
It is undcrstood that this tclcscopc has hccri iiscd on US<br />
military spacecraft.<br />
Thc baseline dcsign is to use thc Kcticon KAZO4HJ chargc<br />
coupled dcvicc (CCD) detcctor opc'rnting in timc delay<br />
intcgration (TDI) mode. It has to he'configcirctt so that its<br />
long axis of 2048 sensors is pcrpcndiculnr to tlrc track of<br />
thc spacecraft and the clock frcqucvcy in thc transvcrw<br />
(short) axis of M dctcctors is synchronous with t!ic velocity<br />
of he spacccraft.<br />
The signal'iioisc ratio of thc dctcctor. D. is giwn hy:<br />
D = r a A T s/N<br />
v/hcrc:<br />
r is thc radiance of the Earth. assumctl to be of thc<br />
order of I00Wm-2sr-1. (This figure is sufficicntly<br />
conservative la includc largc sun txriith anglcs<br />
cncountcrcd at high latitudes.)<br />
a is thc, area of yound ma pdd onto one pixel of thc<br />
dctccror (nssiI.,Icd to tx I ni $ ) 1<br />
A is the solid tin IC wbtcndcd by thc telescope<br />
aperture (0.45 x \b-f2st at an altitude of 4(H)km)<br />
T is thc integrating timc. dcfincd as the limc taken for<br />
1<br />
I<br />
the spacecraft to fly 64m (85ms)<br />
s is the smsilivity of the detector (480 nV I-')<br />
N is the detecm noise level (200 pV RMS)<br />
The signalhoise ratio is thus - 1OOO.<br />
The detector pixels arc appoximately 2Spm square. This<br />
requires the focal Icngth of thc optical tclcscope lo be 1Om.<br />
A sccondary lens will be nccdcd but this docs not have to<br />
be of particularly high optical quality. Thc type of lens<br />
used as a a2 tclcconvcrtnr for 3Smrn SLR cameras would<br />
probably be suitable.<br />
R.3 Navigation and positioning;<br />
If it is assumed that the nominal 2km square image must be<br />
ccntrcd on the target position with an accuracy of f 5OOm.<br />
it is necessary to know the orientation of the tclcscope to an<br />
accuracy of the order of 0.5 mrad.<br />
Navigation information will be derived from a GPS<br />
rcccivcr and oricntation is obtaincd from a star sensor.<br />
A possihlc iniplcmcntation of the GPS rcccivcr is to carry<br />
out thc signal acquisition ~ t l<br />
processing in software within<br />
the on-board proccssing system. A baselinc dcsign using a<br />
singlc.transputcr cxists and would mcct the rcquiremcnts<br />
with a power consumption of 4SW. It is likcly hat a more<br />
approprintc proccssor could he used to rctlucc his.<br />
The star scnror is mounted on thc tclcscope to cnsurc that<br />
thcrc is a constant angle betwccn the two. If it is assumed<br />
that the prapcrtics of the star scnsor are:<br />
. ficld of view: 25O<br />
- niimhcr of stars for rcliablc fix: 6<br />
(hcncc ncrd to iisc stars of 5th magnitudcj<br />
- spacccraft roll ratc: IO rnrad s.I<br />
(= - I revolution cvcry IO minutcs)<br />
. integration he: SO ms<br />
- flux from 5th magnitude star: 2.5 x IOl4 W<br />
- detector sensitivity and noise: as Kcticon abnvc<br />
- sensor apcrturc: 40 mrn diamctcr<br />
~ dctcctor<br />
array: 500 x 500 elements<br />
then it will bc capable of meeting the targct of 0.5 mrad<br />
accuracy if it is possible to intcrpolatc to onc half of a pixel<br />
with a signal/noisc ratio of around 70. This is considcrcd to<br />
bc well within thc pcrformnncc of currcnt interpolation<br />
algorithms. I