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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

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