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Titelmaster Geometrical and Kinematical Precise Orbit Determination of GOCE Akbar Shabanloui Institute of Geodesy and Geoinformation, University of Bonn.

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Presentation on theme: "Titelmaster Geometrical and Kinematical Precise Orbit Determination of GOCE Akbar Shabanloui Institute of Geodesy and Geoinformation, University of Bonn."— Presentation transcript:

1 Titelmaster Geometrical and Kinematical Precise Orbit Determination of GOCE Akbar Shabanloui Institute of Geodesy and Geoinformation, University of Bonn 7th October 2010 Cologne, Germany

2 Outline 2 o Precise Orbit Determination (POD) principle o GOCE Lagrange receiver (clock) o Zero difference estimation procedure o Results o Conclusions o Geometrical Precise Orbit Determination (GPOD) o Kinematical Precise Orbit Determination (KPOD)

3 Precise Orbit Determination (POD) 3 Credit by ESA

4 Precise Orbit Determination (POD) methods 4 POD

5 Geometrical Precise Orbit Determination (GPOD) 5

6 Precise Orbit Determination (POD) methods 6 POD

7 Kinematical Precise Orbit Determination (KPOD) 7

8 Precise Orbit Determination (POD) methods 8 POD  Geometrical POD : point-wise, positions  Kinematical POD : continous, positions, velocities and accelerations  Dynamical POD : continous, positions, velocities and accelerations based on force function information != KPOD, e.g. Bern

9 GPS LAGRANGE receiver onboard GOCE 9 Credit by ESA

10 10 GNSS receiver on-board GOCE Credit by ESA

11 11 GNSS receiver on-board GOCE o LAGRANGE (Laben GNSS Receiver for Advanced Navigation, Geodesy and Experiments) o 12 chanels, dual frequency (L1 and L2) GPS/GLONASS o The clock of the GOCE LAGRANAGE receiver is not steered to integer seconds (free clock system) o Interpolation of SST observations (Data Screening with triple differenced method) o Interpolation of GPS orbits (Zero differenced)

12 12 GNSS receiver on-board GOCE (Rinex SST) Clock is not steerd to be integer

13 13 Clock jumps of receiver (Nov. 2009) GPS LAGRANGE receiver clock behavior!

14 14 Clock behavior of receiver (Nov. 2009) Clock jumps of 20 ms at ~27 hours can be seen 20 ms

15 15 GPS visibility onboard GOCE (Nov. 2009) 7 < Number of GPS satellites (PRNs) < 12

16 16 7 < Number of GPS satellites (PRNs) < 12 GPS visibility onboard GOCE (Nov. 2009)

17 17 Zero differenced GPOD Credite by ESA

18 Zero Difference Only connection between LEO satellite and GPS satellites, Zero Difference Only connection between LEO satellite and GPS satellites, Geometrical Only pure geometrical relations between LEO and the GPS satellites have to be used, no force models and no constraints, Geometrical Only pure geometrical relations between LEO and the GPS satellites have to be used, no force models and no constraints, Precise Consideration all effects on GPS-SST observations and using precise GNSS satellites ephemerides. Precise Consideration all effects on GPS-SST observations and using precise GNSS satellites ephemerides. Zero differenced GPOD 18

19 Processing concept GPOD Zero differencing procedure (ZD) Phase measurements Code measurements 19

20 Precise Orbit Determination (POD) 20 o No troposphere effect at GOCE altitude (~250 km) o First order ionospheric effect eliminated with Ion-free linear combination o Ambiguity term cannot be solved as Integer (real)! o GPS precise orbits (at 15 minutes) and clocks at 30 sec

21 21 GPS Antenna offsets

22 22 GPS antenna offsets … o GPS receiver offset with respect to GOCE reference frame is constant o Offset with respect to center of mass (COM) is slowly varing! o L1 and L2 (L3) Phase Center Offsets (PCO) are derived from IGS ANTEX (ANTenna Exchange format) o Phase Center Variation (PCV) can be empirical estimated based on carrier phase residuals! (or ANTEX?)

23 23 Geometrical POD – hl-SST

24 24 Ground tracks of GPS, GOCE (2 Nov. 1 Rev.)

25 25 Short arc of GOCE (02 Nov. 2 Rev.) 30 minutes short arc (2009-11-02 02 00 00 - 02 30 00)

26 GPOD – GOCE results 26 Estimated geometrical 3D Pos. - PSO

27 27 Kinematical POD

28 28 Short arc representation LEO orbit can be represented as: Gibbs effect! Precision! Solution? fast convergence! or

29 29 Reference motion Euler-Bernoulli Determination of Euler-Bernoulli coefficients A satellite short arc can be represented with the Euler- Bernoulli term up to degree J as:

30 KPOD – GOCE results 30 Estimated kinematical Pos. (J=4) – PSO (Fourier index 30 and 40)

31 31 Conclusions and recommendations o No gravity field and no force models have been used in the Geometrical and Kinematical modes (advantage). o Kinematical POD can be used to recover the Earth’s gravity field model based on the hl-SST methods, (GOCE SST model). o Empirical PCV results should improve POD of GOCE! o GNSS-GOCE satellites configuration and geometrical strength play an important role in POD. o Estimated Geometrical Precise Orbit can be used to estimate kinematical POD of GOCE.

32 Thank you for your attention! Thank you for your attention!


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