Precise Point Positioning
Matthieu Lonchay Performances under Ionospheric Scintillations
Geomatics Unit
PhD Meeting
19 June 2012
NGI, The University of Nottingham
University of Nottingham, UK
Nottingham Geospatial Institute
Handling
Project
Softwares
Geometry
We installed two Septentrio receivers in the Geophysical Center of Dourbes (RMI)
SWANS Project
Geophysical Center of Dourbes (RMI) Septentrio PolaRx3eG
Very Short Baseline
GioveA and GioveB (E1 – E5) GPS 01/25 (L1 – L5)
1-year data set Brussels
Liège Dourbes
2 m
SWANS Project
Geophysical Center of Dourbes (RMI) Septentrio PolaRx3eG
Very Short Baseline
GioveA and GioveB (E1 – E5) GPS 01/25 (L1 – L5)
1-year data set
We installed two Septentrio receivers in the Geophysical Center of Dourbes (RMI)
We designed a preprocessing method based on this new data set
Clock Slips Compensation
Cycle Slips
Detection Data Quality Assessment
SBF RINEX MATLAB Tools Orbits Observation Geometry RINEX Other …
Handling
Project
Softwares
Geometry
0h 1h 2h 6h 12h 18h 24h 0 5 -5 Time [h] Error [m] North error East error Up error
0h 1h 2h 6h 12h 18h 24h 0 5 -5 Time [h] Error [m] North error East error Up error
0h 1h 2h 6h 12h 18h 24h 0 5 -5 Time [h] Error [m] North error East error Up error
- Cycle slips
- Ambiguity resolution processes - Additional convergence time - Measurement noise
- Signal power fluctuations - Lost signals - Geometry troubles - Signal delay Signal phase fluctuations Signal delay Signal amplitude fluctuations P POS
DOP
Ionospheric Scintillations involve physical effects on GNSS signals
WP1 – Signals WP3 – Stochasticity WP5 – Ambiguity WP4 – Model WP2 – Geometry WP0 – GNSS Tools
PPP performances under Ionospheric Scintillations can be improved by using several strategies
Handling
Project
Softwares
Geometry
gLAB is a free and open source multipurpose GNSS data processing and analysis software
ESA/gAGE (UPC)
GNSS Data Processing Tool GNSS Data Analysis Tool Support
Multipurpose
Scientific Professional Educational
AgLAB is a MATLAB software which exploits gLAB to process large network data sets
Automatic downloading Processing (SPP/PPP) Output Data Format Report Files Errors Detection 0 1 2 3 4 5 6 7 8 9 x 104 -2 0 2 4 6 8 10 12 N E S W 0° 30° 60°
AgLAB is a MATLAB software which exploits gLAB to process large network data sets
Automatic downloading Processing (SPP/PPP) Output Data Format Report Files
Errors Detection Galileo?
Rinex v3.0?
Triple Frequency Data? Simulated Data Processing?
0 1 2 3 4 5 6 7 8 9 x 104 -0.2 -0.15 -0.1 -0.05 0 0.05 0.1 0.15 3 4 5 6 7 8 9 x 104 -0.25 -0.2 -0.15 -0.1 -0.05 0 0.05 0.1 0 1 2 3 4 5 6 7 8 9 x 104 -0.15 -0.1 -0.05 0 0.05 0.1
Handling
Project
Softwares
Geometry
Signal amplitude fluctuations
Ionospheric Scintillations
No signal
P
POS
DOP
Ionospheric Scintillations
6h 9h 12h 3 4 5 6 7 8 9 10 11 12 Time [h] Satellites No scintillation Scintillations No Scintillations Scintillations Ionospheric Scintillations
6h 9h 12h 3 4 5 6 7 8 9 10 11 12 Time [h] Satellites No scintillation Scintillations No Scintillations Scintillations Ionospheric Scintillations
6h 9h 12h 0 5 10 15 40 Time [h] PDOP No Scintillations Scintillations No Scintillations Scintillations
Ionospheric Scintillations reduce the satellite geometry quality
No Scintillations Scintillations 6h 9h 12h 0 5 10 15 40 Time [h] PDOP No Scintillations Scintillations No Scintillations Scintillations
Ionospheric Scintillations reduce the satellite geometry quality
The geometric effect of Ionospheric Scintillations is a major effect for satellite positioning
0h 3h 6h 9h 12h 15h 18h 21h 24h 0 5 10 15 20 25 30 35 40 45 50 Time [h] Position Error [m] Edinburgh 324/03
The geometric effect of Ionospheric Scintillations is a major effect for satellite positioning
0h 3h 6h 9h 12h 15h 18h 21h 24h 0 10 20 30 40 50 60 70 80 90 100 Time [h] PDOP 0h 3h 6h 9h 12h 15h 18h 21h 24h 0 5 10 15 Time [h] Satellite tracked
The geometric effect of Ionospheric Scintillations is a major effect for satellite positioning
0h 3h 6h 9h 12h 15h 18h 21h 24h 0 10 20 30 40 50 60 70 80 90 100 Time [h] PDOP 0h 3h 6h 9h 12h 15h 18h 21h 24h 0 5 10 15 Time [h] Satellite tracked
N E S W 0° 30° 60° NORM0010.11O 09h00m00s UT G01 G03 G06 G07 G16 G18 G19 G21 G22
Ionospheric Scintillations produce unbalanced satellite geometry
T1 DOP = 2.36 DOP = 13.78 T2 N E S W 0° 30° 60° N E S W 0° 30° 60°
High DOP values are not only due to a small number of tracked satellites
T1 T2
47
.
3
N
N
0
.
04
N E S W 0° 30° 60° N E S W 0° 30° 60°High DOP values are correlated to a normal matrix close to a singular state
0 N 1 1 ˆ ( ) N A A Qx T 1 sin cos cos sin cos ... ... ... ... 1 sin cos cos sin cos 1 sin cos cos sin cos 2 2 2 2 2 1 1 1 1 1 n n n n n A
Any linear dependence?
A conical satellite geometry drives the DOP to infinite values
T1 DOP = 2.36 DOP = 13.78 T2 N E S W 0° 30° 60° N E S W 0° 30° 60°
High DOP values are not only due to a small number of tracked satellites
T1 T2 T1 DOP = 2.36 DOP = 13.78 T2 N E S W 0° 30° 60° N E S W 0° 30° 60°
A nearly conical satellite geometry drives the DOP to critical values
T1 T2 T1 DOP = 2.36 DOP = 13.78 T2 N E S W 0° 30° 60° N E S W 0° 30° 60°
A nearly conical satellite geometry deteriorates the satellite geometry quality
0 1 2 3 4 5 6 7 8 9 x 104 -20 -10 0 10 20 30 40 50 60 No problem Problem
Ionospheric Scintillations increase the probability to encounter conical satellite geometries
8 10 13 17 21 24 26 27 28 N E S W 0° 30° 60° Nb sat: 9 |N|: 51.3472 PDOP: 1.431 8 16 26 27 N E S W 0° 30° 60° Nb sat: 4 |N|: 0.004485 PDOP: 43.1737
DOY/YY 27960 08 09 10 15 18 21 26 27 28 29 31 N E S W 0° 30° 60° DOY/YY 27960 08 09 10 15 18 21 26 27 28 29 31 N E S W 0° 30° 60° DOY/YY 40470 05 07 09 14 30 N E S W 0° 30° 60°
Coherent Observation Weigthing Scheme
N E S W 0° 30° 60° MLAT0010.11O 01h23m00s UT
The combined use of GPS and Galileo satellites improves the satellite geometry quality
N E S W 0° 30° 60° MLAT0010.11O 01h23m00s UT
The combined use of GPS and Galileo satellites improves the satellite geometry quality
0h 3h 6h 9h 12h 0 1 2 3 4 5 10 Time [h] PDOP
The combined use of GPS and Galileo satellites improves the satellite geometry quality
0h 3h 6h 9h 12h 0 1 2 3 4 5 10 Time [h] PDOP
The combined use of GPS and Galileo satellites improves the satellite geometry quality
Quantify the improvement of PPP’s performances involved by the expanded GPS-Galileo satellite geometry - Precision - Time convergence - Reliability Ionospheric Scintillations Scintillations/Geometry/WP2/Objectives
Handling
Project
Softwares
Geometry
Signal amplitude fluctuations
Ionospheric Scintillations degrade satellite signal quality
Measurement error
P
POS
DOP
Ionospheric Scintillations degrade receiver measurement precision
2 2 1 2 2 2 21 1 12 2 1...
...
...
..
..
..
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n n n n n
The PPP stochastic model considers receiver measures to be independent/uncorrelated
2 2 2 2 1...
0
0
...
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0
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The PPP stochastic model considers receiver measures to be independent/uncorrelated
“Everything is related to everything else, but near things are more related than
distant things.”
First law of Geography…
S1C [dB-Hz] 2h 3h 4h 5h 6h 7h Time [h] 44 45 46 47 47 48 49 44 45 46 47 48 49 S1C [dB-Hz] S1C [dB-Hz]
Satellite Signals are affected differently by Ionospheric Scintillations
N E S W 0° 30° 60° MLAT0010.11O 03h00m00s UT
Satellite Signals are affected differently by Ionospheric Scintillations
N E S W 0° 30° 60° MLAT0010.11O 03h00m00s UT
Spatial Auto-Correlation (SAC) can be exploited to generate a new PPP stochastic model
N E S W 0° 30° 60° MLAT0010.11O 03h00m00s UT
Spatial Auto-Correlation (SAC) can be exploited to generate a new PPP stochastic model
N E S W 0° 30° 60° MLAT0010.11O 03h00m00s UT
Spatial Auto-Correlation (SAC) can be exploited to generate a new PPP stochastic model
2 2 1 2 2 2 21 1 12 2 1...
...
...
..
..
..
..
n n n n n
N E S W 0° 30° 60° MLAT0010.11O 01h23m00s UT 2 ) ( ) )( ( v v v v v v w w N I i i j i ij j i ij j i ij ij
d
w
1
i i S C v 1 SAC SAC random ‐1 0 1Spatial Auto-Correlation (SAC) is measured by computing SAC indices on satellite geometries
N E S W 0° 30° 60° MLAT0010.11O 01h23m00s UT 2 ) ( ) )( ( v v v v v v w w N I i i j i ij j i ij j i ij ij
d
w
1
i i S C v 1Spatial Auto-Correlation (SAC) is measured by computing SAC indices on satellite geometries
0h 3h 6h 9h 12h -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 Time [h] Moran's I
Spatial Auto-Correlation (SAC) is fluctuating in time
Perspective 1: several SAC indices exist with their own specificities
Moran’s I Geary’s C
Mantel’s Γ
Getis and Ord’s index LISA tests
Perspective 2: a Least Square Adjustment to fit a polynomial surface on satellite geometries
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,
(
f
S
Perspective 3: a Principal Components Analysis (PCA) to study the correlation between variables
n
...
2 1 n
...
2 1n
...
2
1
nv
v
v
...
2 1 ? v v ?Perspective 4: a SAC detection based on other observables
Signal Strength (S1C)
Tracking error (Conker model) ܵସ
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Perspective 5: more realistic simulations with potentially more tracked satellites
Handling
Project
Softwares
Geometry
Precise Point Positioning
Matthieu Lonchay Performances under Ionospheric Scintillations
Geomatics Unit
PhD Meeting
19 June 2012
NGI, The University of Nottingham
University of Nottingham, UK
Nottingham Geospatial Institute