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Graz in Space 2008
Graz SLR System
Daniel Kucharski
IWF / SatGeo
Satellite Laser Ranging
• Range measurements to the satellites- time of flight of the ultrashort laser pulses- mm precision station-satellite- for: POD, science
SLR – geodetic technique
‘time of flight’ measurement of the laser pulses
SLR measurements
- scientific studies of the Earth / Atmosphere / Oceans systems, determination of the temporal mass redistribution, EOP
- determination of the geocentric positionof an Earth satellite (precise calibration ofradar altimeters)
- allow to determine the stations’ positions, their tectonic motion with respect to the geocenter
- support research in fundamental physics. SLRmeasurements of LAGEOS 1and 2 have measured the Lense-Thirring “drag” of the referenceframe. A third LAGEOS-type satellite has been proposed forrelativity studies.
SLR measurements
The satellites
Currently 35 objects
- active: altimetry, gravitometry, navigation
- passive: geodynamic
LAGEOS-1 i 2
426 CCRs
60 cm diameter
Mass 411 kg, 405 kg
~6000 km above the surface
Fully passive, geodesy
Ajisai
1436 CCRs + 318 mirrors
685 kg
Diameter 215 cm
1500 km above the Earth
Fully passive, geodesy
GPS-35 i 36
Panels with 32 CCRs
Navigation system,
time transfer
ERS-2, Envisat
9 CCRs
800 km above the ground
remote sensing and environmental monitoring
1200 km
altimetry, oceanography
The Moon
The Moon
SLR stations on the world
Graz SLR stationGRAZ The other
stations2 kHz 5 - 10 Hz
35 – 200 mJ
35 – 200 ps
532 nm
0.4 mJ
10 ps
532 nm
Laser pulse
Energy / puls
Puls width
Wavelength
High accuracy of the distance measurements
200 times more measurements per second -> POD
LAGEOS-1 pass
GPS 35: Average # of Pts/NP in 2004
845
357
215
155
129
95 67 62 46 32 30 30 20 18 12 7 30200400600800
1000
Gra
z
Mat
era
Gra
sse
Riy
adh
Mon
umen
t
Wet
tzel
l
Kog
anei
Mt S
trom
lo
McD
onal
dH
erst
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ceu
Yarr
agad
ee
Zim
mer
wal
d
Mai
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k 1
Sim
osat
o
Pots
dam
Cha
ngch
un
Bei
jing
Graz kHz SLR - statistics
SLR Graz: Routine - Calibrations 2003-2005;10 Hz: 500 Returns; kHz: 10 000 Returns / CAL
-4
-3
-2
-1
0
1
2
3
4
2003 2003.5 2004 2004.5 2005 2005.5
Peak
min
us M
ean
[mm
] CAL Peak minus Mean [mm]
Graz kHz SLR - calibration
Up Component: -3.53 ± 0.07 mm / year (≈100 k years until sea level)East Component: 22.15 ± 0.07 mm / yearNorth Component: 14.85 ± 0.10 mm / year
Graz station – position motion
Graz kHz SLR – new applications
Satellite spin measurementsGravity Probe – B, 650 km, 75s AJISAI, 1500 km, 2sLAGEOS – 1, 2, 6000 km, 5000s, 600sETALON –1 , 2, 19000 km, 65 s
Atmospheric seeing measurementsmonitoring the atm. condition of the way of a laser pulse
Space debris trackinghelps to monitor them, POD
Graz kHz SLR – Spin GP-BLense-Thirring “drag”
650 km
Only Graz kHz SLR station was able to measure the spin of the spacecraft
Graz kHz SLR – Spin GP-B8 CCRs, 10cm dia.
RMSLASER-OnBoard = 0.98 s
Graz kHz SLR – Spin GP-B
Graz kHz SLR – Spin AJISAI
Spectral analysis of kHz SLR data
Graz kHz SLR – Spin AJISAI
AJISAI SPIN RATE 2003/10 - 2005/06; corrected for apparent Spin 195 passes with >300 k points; ± 48 s around CA used (40 k min)
0.500
0.505
0.510
0.515
0.520
0.525
2003.8 2004.2 2004.6 2005.0 2005.4Year
Spin
Rat
e [H
z]
6-Retro
9 Retro
12 Retro
Graz kHz SLR –LAGEOS-1
T=5775 s
Graz kHz SLR – ETALON-1, 2
Real
obs.
Sim:
30 s
66 s
100 s
~70k returns/h
Graz kHz SLR – ETALON-1, 2
Spin period of the ETALONs is increasing by a value of about 0.5 s/year
RMS ~1%
Spin parameters - applicationImproving the accuracy of the perturbations’ models
The magnetic torque
( ) ( ) BBVBBVmagnetic ××′′−⋅×′=Γ ϖαϖϖα Bertotti and Iess, 1991
The gravitational torque
( )( )( )( )LnLnACLm
nalgravitatio ×⋅−−−=Γ 1cos343 2
2
2
ϑ Farinella et al., 1996
Solar radiation pressure causes a torque:
( )suncrossR
offset rscAhCI
×=Γ 0 Vokrouhlicky, 1996
Bertotti, B., and Iess, L. The rotation of LAGEOS, J. Geophys. Res., 96 (B1), 2431-2440, 1991
Farinella, P., Vokrouhlicky, D., Barlier F. The rotation of LAGEOS and ist long-term semimajor axis decay, J. Geophys. Res., 101 (B8), 17,861-17,892, 1996
Vokrouhlicky, D. Non-gravitational effects on LAGEOS’ rotation. Geophys. Res. Lett., 23, 3079-3082, 1996
Graz kHz SLR – LAGEOS-2
Full 15 years spin period history,
Only Graz kHz system can measure L2 spin of more than 100s
Study of various perturbations and RE
Graz kHz SLR – atm. seeing
Laser Beam Backscatter is monitored by ISIT; => into PC;Real Time Image Processing: Determine Peak of Laser Beam;At 25 fps: Store peak coordinates in file;Post Processing: Get Area of Coordinates;FWHM of this area => Astr. Seeing (arc secs)Calibrate with standard astronomical methods
Graz kHz SLR – seeing
- more accurate range measurements = improvement of POD (navigation systems HEO, LEO)
- much more scientific data: spin determination of various sat.
- kHz SLR allows to investigate the values of the SP and their changes, that gives an unique possibility to study the tiny petrurbating forces (RE)
- more information about the atmospheric conditions: seeing measurements over the station
Graz – the first kHz SLR system