Shipborne GNSS for geoid validation
Transcript of Shipborne GNSS for geoid validation
Stavanger, 22.11.2018
Shipborne GNSS for geoid validation
- Examples from the FAMOS project -
Mirjam Bilker-Koivula
Maaria Nordman, Jaakko Kuokkanen, Timo Saari
Hannu Koivula, Pasi Häkli, Sonja Lahtinen, Ulla Kallio
Finnish Geospatial Research Institute, National Land Survey of Finland
Acknowledgement: Jyrki Mononen, Finnish Transport Agency
Stavanger, 22.11.2018
Background & Motivation
• FAMOS project:
– Improve infrastructure for future navigation in the Baltic Sea
– E.g. Hydrographic surveying, gravity surveys, new Baltic
Sea geoid model, GNSS augmentation tests
• Baltic Sea Chart Datum 2000, BSCD2000
– Common height reference for the whole Baltic Sea
– Based on EVRS, epoch 2000
– Zero level defined by the geoid
• Quality assessment of geoid models at sea needed
– GPS-levelling at sea
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Derive geoid heights from GNSS
observations at sea
dN = SSH – ADT – N
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Shipborne GNSS for geoid validation -
Contents
• Background & Motivation
• Calculation process
– GNSS processing
– Reduction to sea surface
– Sea surface modelling
• 3 examples from the FAMOS project
– 2015 Airisto campaign
– 2017 Aranda campaign
– 2018 Geomari campaign
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Calculation process
GNSS post-processing
Result: Ellipsoidal heights at the vessel’s reference
point in the processing coordinate system
Height translation from vessel reference point
to the sea surface
Result: Ellipsoidal heights at the sea surface
Translation from sea surface to geoid surface
Result: Ellipsoidal heights at the geoid surface
Comparison with geoid models
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GNSS post-processing
GNSS base station processing
Result: Consistent reference coordinates for the
processing system
Kinematic processing of vessel GNSS/IMU data
Result: Ellipsoidal height of vessel reference point
in processing coordinate system
Coordinate transformation
Result: Ellipsoidal height of reference point in the
systems related to the geoid models in use
Height reduction from reference point to the
sea level
Result: Ellipsoidal height of the sea level in the
systems related to the geoid models in use
Campaign reference
frame & epoch, e.g.:IGb08 2015.754770
IGS14 2017.432877
IGS14 2018.39315
Geoid model ref.
frame & epochETRF96 1997.000
ETRF2000 2000.000
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Height translation from vessel reference
point to the sea surface
• Reductions
– Pitch and Roll (small effect)
– Heave: short term vertical movements of the vessel
– Static draft: Impact of ships load changes to draft
– Dynamic draft: Squat (velocity effect to draft)
• Result: ellipsoid height at the sea surface
= Sea Surface Height, SSH
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Translation from sea surface to geoid
surface
Height transformation from sea surface to geoid level (zero height)
- remove Absolute Dynamic Topography (ADT)
Sea surface modelling:
• Tide gauge method
– Tide gauges from surrounding countries
– Fit surface
• Physical model method
– Sea surface from Baltic Sea physics analysis and forecast
(Copernicus Marine Environment Monitoring Service ,CMEMS)
– Fit surface to tide gauges
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26.9.2015
Corrected
physical
model
surface
Tide
gauge
surface
Original
physical
model
surface
Computed
correction
surface
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3 FAMOS measurement campaigns
• 2015 Airisto
– Survey vessel
– Dedicated gravity campaign
– GNSS data from vessel’s own navigation system
• 2017 Aranda
– Environmental research vessel
– Piggy-back campaign
– GNSS equipment installed by FGI
• 2018 Geomari
– Geological research vessel
– Dedicated gravity campaign
– GNSS equipment installed by FGI
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Airisto Campaign 2015
• Survey vessel Airisto
(Meritaito Oy)
• Dedicated gravity survey
• 26.9. – 7.10. (Umeå) – 12.10.
• Vessel’s GNSS data stored
• Well determined
– Internal coordinate system
– Squat table
– Static draft readings
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FAMOS 2015 Airisto campaign - GNSS
data analysis Applanix POSPac MMS 7.1
Smooth Best Estimate Trajectory
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Reduction to sea surface
Roll
0 – 5 cmPitch
0 – 4 cm
Static draft
10 cm
Squat
0 – 20 cm
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Reduction to geoid surface
Height transformation from sea surface to
geoid level (zero height) - remove ADT
Sea surface modelling:
• Tide gauge method
– 6 Swedish tide gauges
– 10 Finnish tide gauges
• Physical model method
– Baltic Sea physics analysis and forecast
(Copernicus Marine Environment
Monitoring Service ,CMEMS)
– Fitted to tide gauges
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Comparison with geoid models
Comparison with geoid models: dN = SSHGNSS – ADTmodelled – Ngeoid model
Mean 9.5 cm
SD 5.0 cm
Mean 9.5 cm
SD 1.8 cmMean 15.5 cm
SD 20.9 cm
Mean 15.6 cm
SD 19.1 cm
Mean 0.3 cm
SD 11.5 cm
Mean 0.2 cm
SD 3.2 cm
Mean -3.6 cm
SD 58.8 cm
Mean -3.5 cm
SD 60.4 cm
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Comparison with geoid models
Comparison with geoid models
• 7 lines rejected
• Grand mean and standard deviation
Non-filtered FIN2005N00 model Non-filtered NKG2015 model
Tide gauge surface Physical model Tide gauge surface Physical model
mean (cm) sd (cm) mean (cm) sd (cm) mean (cm) sd (cm) mean (cm) sd (cm)
4.7 10.9 3.7 11.2 3.2 10.9 2.1 11.1
Filtered FIN2005N00 model Filtered NKG2015 model
Tide gauge surface Physical model Tide gauge surface Physical model
mean (cm) sd (cm) mean (cm) sd (cm) mean (cm) sd (cm) mean (cm) sd (cm)
4.7 4.3 3.7 4.3 3.1 4.3 2.1 4.2
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Famos Aranda, 5.6-10.6.2017
• Environmental
research vessel
• Piggyback campaign
• GNSS/IMU
equipment installed
by FGI
• GNSS trajectory calculations
with Inertial Explorer Software
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Squat estimation from GNSS data
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Static Draft
• Readings at three locations during stops at sea
• 1.3 - 2.9 cm/day
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Tide Gauges
• 14 stations in Finland
• 6 stations in Estonia
• 9 stations in Sweden
Geoid Models
• FIN2005N00
• NKG2015
Reduction to geoid level
CMEMS Baltic Sea
physics analysis and
forecast
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Geoid height differences
ΔN = SSH – ADT – N(FIN2005N00)
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GNSS-Geoid comparison Aranda
DOY 156-161
Tide Gauges (cm) Physical Model (cm)
FIN2005N00 NKG2015 FIN2005N00 NKG2015
Mean Std. Mean Std Mean Std Mean Std
Line 1 0 10 -1 9 1 10 0 9
Line 2 -3 9 -4 9 -1 9 -1 9
Line 3 -9 10 -10 9 -9 11 -11 11
Line 4 -17 11 -18 12 -19 10 -20 10
Line 5 -5 8 -7 8 -5 8 -7 8
Line 6 -8 11 -10 11 -8 11 -10 11
Line 7 -8 6 -6 5 -8 6 -6 6
All (1 min) -7 10 -8 10 -7 11 -8 11
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2018 Geomari Campaign
• 21.-25.5.2018
• Dedicated gravity campaign
• GNSS/IMU equipment installed by FGI
• Location measurements in ship coordinates
• Static draft reading in harbours
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Squat estimation
• Majority of time constant speed
• Not much accelerations/decelerations
• No reasonable squat values obtained
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At 5 knots:
< 1 cm
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Tide Gauges
• 4 stations in Finland
• 5 stations in Estonia
Geoid Models
• FIN2005N00
• NKG2015
Reduction to sea level
CMEMS Baltic Sea
physics analysis
and forecast
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-0.2
-0.15
-0.1
-0.05
0
0.05
0.1
0.15
0.2
dN_TG dN_PM
Geoid height differences
Monday Tuesday Wednesday Thursday Friday(m)
ΔN = SSH – ADT – N(FIN2005N00)
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DOY 141-145
Tide Gauges (cm) Physical Model (cm)
FIN2005N00 NKG2015 FIN2005N00 NKG2015
Mean Std. Mean Std. Mean Std. Mean Std.
Monday 5.2 4.1 15.6 4.6 4.6 4.1 15.0 4.6
Tuesday -3.8 5.7 6.3 6.7 -4.9 5.7 5.2 6.8
Wednesday 3.4 3.1 11.6 3.6 2.9 3.1 11.2 3.8
Thursday 7.4 4.3 14.3 4.7 7.5 4.7 14.5 5.2
Friday -5.1 3.7 4.5 4.6 -5.6 3.5 4.1 4.2
All 2.4 6.4 11.2 6.4 2.0 6.7 10.8 6.7
GNSS-Geoid comparison Geomari
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It is possible to recover geoid heights from GNSS
observations at sea and validate existing geoid models
• Agreement between geoid heights derived from GNSS
observations and those from geoid models better than 5 cm
in the Bothnian Sea
• Less good agreement with big vessel and piggyback-mode
over large area
• In Eastern Gulf of Finland results are promising. Here geoid
height differences may reveal differences between geoid
models that are due to differences in input gravity data.
Conclusions I
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Important:
- Positioning of GNSS antenna
- Common processing of base stations
- Coordinate transformation to systems related to geoid model
- Vessel with well determined internal coordinate system
- Knowledge on relative locations of instruments and water line
- Pitch and roll
- Static draft and squat
- Well-controlled area with good monitoring networks and models
- Elsewhere modelling of tides may be needed
Conclusions II
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www.famosproject.eu