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Tropospheric correction model in support of Precise Point Positioning Jan Douˇ sa, Michal Eliaˇ s and Pavel V´ aclavovic Geodetic Observatory Pecn´ y of the Research Institute of Geodesy, Topography and Cartography, Czech Republic [[email protected]] IGS Workshop 2014 Pasadena, California, USA Abstract New tropospheric correction model was developed at the Geodetic Observatory Pecny (GOP) based on a) numerical weather data field and b) new concept of the zenith wet delay modelling. The model provides parameters for precise calculation of zenih hydrostatic and wet tropospheric delays at the surface and at any altutude up to 10 km. The correction model supports a flexible parametrization including benefit of in situ meteorological observations. First, we demonstrate the performace of new ZWD approximations and analytical calculation when applying a closed loop with a numerical weather field considered as the reference. Additionally, we compared numerical weather field with respect to results from GNSS final tropospheric product provided by IGS. Finally, we study a potential of the model to support GNSS applications like kinematic Precise Point Positioning. Enhanced Zenith Wet Delay (ZWD) model development based on Askne-Nordius model ASKNE-NORDIUS model (1987) for ZWD analytical calculation COLLINS - LANGLEY UNB3 model (1997) for ZWD vertical approximation MODIFIED UNB3 model (2014) for ZWD vertical approximation + + + DOUSA-ELIAS model (2014) for improved ZWD vertical approximation DOUSA-ELIAS model (2014) enhanced ZWD calculation via ASKNE-NORDIUS model + Although developed in 1987, the analytical model of Askne and Nordius remains one of the most precise models for calculating ZWD. New strategy based on improved ZWD vertical approximation is described in Dousa and Elias (2014). Here, we provide several remarks only: Askne-Nordius model is based on the knowledge of the temperature and its lapse rate (beta) and partial water vapour pressure and its exponential decay parameter (lambda). We introduced new ZWD vertical approximation (gamma), which follows the definition of the water vapour decay parameter. Both parameters are fitted via full NWP or radiosonde profile using orig- inal formula and Levenberg-Marquardt algorithm (1963). Optimal combination of both decay parameters was developed for im- proving the ZWD model of Askne-Nordius (1987). Flexibility of the new model includes potential utilization of in situ ob- served meteorological parameters. New ZWD vertical approximation 0 2 4 6 8 10 0 1 2 3 4 5 6 7 height [km] water vapour pressure [hPa] 2005-06-05[00] lat/lon/hgt = +86deg/+10deg/+2m data fit via E fit via ZWD 0 2 4 6 8 10 0 5 10 15 20 25 height [km] water vapour pressure [hPa] 2005-06-05[00] lat/lon/hgt = +42deg/+10deg/+63m data fit via E fit via ZWD 0 2 4 6 8 10 0 20 40 60 80 100 120 140 160 180 height [km] zenith wet delay [mm] 2005-06-05[00] lat/lon/hgt = +42deg/+10deg/+63m data fit via ZWD fit via e Left figure shows water vapour profile (crosses) and approximation (line). Right figures top right display water vapour and ZWD profiles at other location showing a typical unfolding character of both approximations. ZWD vertical approximations using: 1+2) original and modified UNB3 model; 3+4) new model as a function of pressure and height. HEIGHT 0-1 km 1-2 km 2-3 km 3-4 km 4-5 km 5-6 km 6-7 km 7-8 km Original 11.4 20.7 20.2 19.9 15.3 13.2 10.4 7.9 Modified 10.8 19.1 18.6 18.0 13.6 11.4 8.7 6.5 New f(P) 8.2 7.4 5.5 6.5 5.6 5.6 5.0 3.7 New f(H) 8.3 7.4 5.5 6.5 5.7 5.6 5.0 3.7 Improved ZWD calculation (global assessment) -25 -20 -15 -10 -5 0 5 10 15 20 25 ZWD - ref.ZWD [mm] -25 -20 -15 -10 -5 0 5 10 15 20 25 ZWD - ref.ZWD [mm] -25 -20 -15 -10 -5 0 5 10 15 20 25 ZWD - ref.ZWD [mm] -25 -20 -15 -10 -5 0 5 10 15 20 25 ZWD - ref.ZWD [mm] Four figures show global ZWD differences for ZWDs calcu- lated using A-N model with vertical approximations using: a) water vapour pressure decay parameter (lambda), b) ZWD decay parameter (gamma), c) combination of both decay pa- rameters, Tm calculated (A- N), d) combination of both decay parameters, Tm inte- grated. Figure right shows ZWD accuracy in a latitudinal de- pendence when using various vertical approximation variants for the partial water vapour pressure and ZWD: log-fitting, pow-fitintg and new combined approach. 0 10 20 30 40 50 60 -80 -60 -40 -20 0 20 40 60 80 zenith wet delay - rms [mm] latitude [degree] pow-fit via E log-fit via E pow-fit via ZWD log-fit via ZWD pow-fit via E+ZWD Model application - initial study for positioning -0.80 -0.60 -0.40 -0.20 0.00 0.20 0.40 0.60 0.80 00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00 2.28 2.30 2.32 2.34 2.36 2.38 2.40 2.42 N, E, U [m] ztd [m] 09-JAN-2012 ONSA [EST-KIN-NWM] (c) GOP/RIGTC, 14-05-30 12:30 North East Up ZTD -0.80 -0.60 -0.40 -0.20 0.00 0.20 0.40 0.60 0.80 00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00 2.28 2.30 2.32 2.34 2.36 2.38 2.40 2.42 N, E, U [m] ztd [m] 09-JAN-2012 ONSA [EST-KIN-NWM] (c) GOP/RIGTC, 14-05-30 12:30 North East Up ZTD Plots above demonstrate PPP pseudo-kinematic positioning (ONSA) for two scenar- ios: a) with simultaneously estimated coordinates and tropospheric parameters (left); b) with coordinates estimated after introducing tropospheric parameters from the global ERA Interim model (right). Left figure demonstrates a correlation between height and troposphere which time-to-time significantly weakens the solution. 0.000 0.020 0.040 0.060 0.080 0.100 0.120 2012-01-01 2012-01-02 2012-01-03 2012-01-04 2012-01-05 2012-01-06 2012-01-07 2012-01-08 2012-01-09 2012-01-10 2012-01-11 2012-01-12 2012-01-13 2012-01-14 2012-01-15 2012-01-16 2012-01-17 2012-01-18 2012-01-19 2012-01-20 2012-01-21 2012-01-22 2012-01-23 2012-01-24 2012-01-25 2012-01-26 2012-01-27 2012-01-28 2012-01-29 2012-01-30 STD [m] DRES-2012-Jan: (EST-KIN) North East Up 0.000 0.020 0.040 0.060 0.080 0.100 0.120 2012-01-01 2012-01-02 2012-01-03 2012-01-04 2012-01-05 2012-01-06 2012-01-07 2012-01-08 2012-01-09 2012-01-10 2012-01-11 2012-01-12 2012-01-13 2012-01-14 2012-01-15 2012-01-16 2012-01-17 2012-01-18 2012-01-19 2012-01-20 2012-01-21 2012-01-22 2012-01-23 2012-01-24 2012-01-25 2012-01-26 2012-01-27 2012-01-28 2012-01-29 2012-01-30 STD [m] DRES-2012-Jan: (NWM-KIN) North East Up 0.000 0.020 0.040 0.060 0.080 0.100 0.120 2012-01-01 2012-01-02 2012-01-03 2012-01-04 2012-01-05 2012-01-06 2012-01-07 2012-01-08 2012-01-09 2012-01-10 2012-01-11 2012-01-12 2012-01-13 2012-01-14 2012-01-15 2012-01-16 2012-01-17 2012-01-18 2012-01-19 2012-01-20 2012-01-21 2012-01-22 2012-01-23 2012-01-24 2012-01-25 2012-01-26 2012-01-27 2012-01-28 2012-01-29 2012-01-30 STD [m] DRES-2012-Jan: (NWM-KIN) North East Up Figures above show monthly coordinate repeatabilities (DRES) demonstrating the better performance for height with tropospheric delays introduced from the external model and when compare to simultaneously estimated ZTDs and coordinates. 0.002 0.004 0.006 0.008 0.010 0.012 0.014 0.016 0 10 20 30 40 50 RMS ZTD [m] HOUR [#5-minutes ] Comparing of RMS errors:ONSA-Jan-2012 IGS - NWM *smt - *flt 0.002 0.004 0.006 0.008 0.010 0.012 0.014 0.016 0 10 20 30 40 50 RMS ZTD [m] HOUR [#5-minutes ] Comparing of RMS errors:ONSA-Jan-2012 IGS - NWM *smt - *flt 0.000 0.010 0.020 0.030 0.040 0.050 0.060 0.070 0 10 20 30 40 50 RMS ZTD [m] HOUR [#5-minutes ] Comparing of RMS errors:ONSA-2012 IGS-PPP IGS-NWM Last plots compare ZTD accuracies during the PPP initialization (ONSA) and ZTD accuracies from the ERA Interim model. Note the results are from the winter period; ZTD accuracy of ERA Interim can be double worse. ERA Interim ZTD assessment 2 2.1 2.2 01/07/12 01/14/12 01/21/12 01/28/12 -0.04 -0.02 0 0.02 0.04 ZTD [m] Difference [m] EPOCH [#5-minutes ] ANKR-2012-Jan: ZTD (IGS-NWM) Diff IGS NWM 2 2.1 2.2 01/07/12 01/14/12 01/21/12 01/28/12 -0.04 -0.02 0 0.02 0.04 ZTD [m] Difference [m] EPOCH [#5-minutes ] ANKR-2012-Jan: ZTD (IGS-NWM) Diff IGS NWM 2.1 2.2 2.3 07/07/12 07/14/12 07/21/12 07/28/12 -0.04 -0.02 0 0.02 0.04 ZTD [m] Difference [m] EPOCH [#5-minutes ] ANKR-2012-Jul: ZTD (IGS-NWM) Diff IGS NWM 2.1 2.2 2.3 07/07/12 07/14/12 07/21/12 07/28/12 -0.04 -0.02 0 0.02 0.04 ZTD [m] Difference [m] EPOCH [#5-minutes ] ANKR-2012-Jul: ZTD (IGS-NWM) Diff IGS NWM Comparison of ERA Interim global numerical weather data field and IGS final tro- pospheric products. Plots display ZTDs (and ZTD differences) between IGS final product and ZTDs calculated from the ERA Interim numerical weather data field during two months (seasons): January and July, 2013. Reference 1. Askne J, Nordius H (1987) Estimation of tropospheric delay for microwaves from surface weather data, In: Radio Science, 22(3):379–386 2. Collins JP (1997) Assessment and Development of a Tropospheric Delay Model for Aircraft Users of the Global Positioning System, M.Sc.E. thesis, Department of Geodesy and Geomatics Engineering Technical Report No. 203, University of New Brunswick, Fredericton, New Brunswick, Canada, 174 pp. 3. Dousa J, Elias M (2014) An improved model for calculating tropospheric wet delay, Geophysical Research Letters (accepted on 6 June, 2014) 4. Marquardt, D. (1963) An algorithm for least-squares estimation of nonlinear pa- rameters, J Soc Ind Appl Math, 11(2):431–441 Acknowledgement: The model development was supported by the ESA Project Trop4LAS and the Czech Science Foundation (P209/12/2207). We acknowledge the ERA Interim data provided by the European Centre for Medium-Range Weather Forecasts (ECMWF).
Transcript
Page 1: Tropospheric correction model in support of Precise Point ... 2014 - PS12 - Dousa... · Comparing of RMS errors:ONSA-Jan-2012 IGS - NWM *smt - *flt 0.000 0.010 0.020 0.030 0.040 0.050

Tropospheric correction model in support of Precise Point Positioning

Jan Dousa, Michal Elias and Pavel VaclavovicGeodetic Observatory Pecny of the Research Institute of Geodesy, Topography and Cartography, Czech Republic [[email protected]]

IGS Workshop 2014 Pasadena, California, USA

AbstractNew tropospheric correction model was developed at the Geodetic Observatory Pecny (GOP) based on a) numerical weather data field and b) new concept of the zenith wet

delay modelling. The model provides parameters for precise calculation of zenih hydrostatic and wet tropospheric delays at the surface and at any altutude up to 10 km. The

correction model supports a flexible parametrization including benefit of in situ meteorological observations.

First, we demonstrate the performace of new ZWD approximations and analytical calculation when applying a closed loop with a numerical weather field considered as the

reference. Additionally, we compared numerical weather field with respect to results from GNSS final tropospheric product provided by IGS. Finally, we study a potential of

the model to support GNSS applications like kinematic Precise Point Positioning.

Enhanced Zenith Wet Delay (ZWD) model development based on Askne-Nordius modelASKNE-NORDIUS model (1987)

for ZWD analytical calculation

COLLINS - LANGLEY UNB3 model (1997)for ZWD vertical approximation

MODIFIED UNB3 model (2014)for ZWD vertical approximation

+ + +

DOUSA-ELIAS model (2014)for improved ZWD vertical approximation

DOUSA-ELIAS model (2014) enhanced ZWD calculation via ASKNE-NORDIUS model

+

Although developed in 1987, the analytical model of Askne and Nordius

remains one of the most precise models for calculating ZWD. New strategy

based on improved ZWD vertical approximation is described in Dousa and

Elias (2014). Here, we provide several remarks only:

•Askne-Nordius model is based on the knowledge of the temperature and

its lapse rate (beta) and partial water vapour pressure and its exponential

decay parameter (lambda).

•We introduced new ZWD vertical approximation (gamma), which follows

the definition of the water vapour decay parameter.

•Both parameters are fitted via full NWP or radiosonde profile using orig-

inal formula and Levenberg-Marquardt algorithm (1963).

•Optimal combination of both decay parameters was developed for im-

proving the ZWD model of Askne-Nordius (1987).

• Flexibility of the new model includes potential utilization of in situ ob-

served meteorological parameters.

New ZWD vertical approximation

0

2

4

6

8

10

0 1 2 3 4 5 6 7

he

igh

t [k

m]

water vapour pressure [hPa]

2005-06-05[00] lat/lon/hgt = +86deg/+10deg/+2m

datafit via Efit via ZWD

0

2

4

6

8

10

0 5 10 15 20 25

he

igh

t [k

m]

water vapour pressure [hPa]

2005-06-05[00] lat/lon/hgt = +42deg/+10deg/+63m

datafit via Efit via ZWD

0

2

4

6

8

10

0 20 40 60 80 100 120 140 160 180

he

igh

t [k

m]

zenith wet delay [mm]

2005-06-05[00] lat/lon/hgt = +42deg/+10deg/+63m

datafit via ZWDfit via e

Left figure shows water vapour profile (crosses) and approximation (line).

Right figures top right display water vapour and ZWD profiles at other

location showing a typical unfolding character of both approximations.

ZWD vertical approximations using: 1+2) original and modified UNB3

model; 3+4) new model as a function of pressure and height.

HEIGHT 0-1 km 1-2 km 2-3 km 3-4 km 4-5 km 5-6 km 6-7 km 7-8 km

Original 11.4 20.7 20.2 19.9 15.3 13.2 10.4 7.9

Modified 10.8 19.1 18.6 18.0 13.6 11.4 8.7 6.5

New f(P) 8.2 7.4 5.5 6.5 5.6 5.6 5.0 3.7

New f(H) 8.3 7.4 5.5 6.5 5.7 5.6 5.0 3.7

Improved ZWD calculation (global assessment)

−25

−20

−15

−10

−5

0

5

10

15

20

25

ZWD − ref.ZWD [mm]

−25

−20

−15

−10

−5

0

5

10

15

20

25

ZWD − ref.ZWD [mm]

−25

−20

−15

−10

−5

0

5

10

15

20

25

ZWD − ref.ZWD [mm]

−25

−20

−15

−10

−5

0

5

10

15

20

25

ZWD − ref.ZWD [mm]

Four figures show global ZWD

differences for ZWDs calcu-

lated using A-N model with

vertical approximations using:

a) water vapour pressure decay

parameter (lambda), b) ZWD

decay parameter (gamma), c)

combination of both decay pa-

rameters, Tm calculated (A-

N), d) combination of both

decay parameters, Tm inte-

grated.

Figure right shows ZWD accuracy in a latitudinal de-

pendence when using various vertical approximation

variants for the partial water vapour pressure and ZWD:

log-fitting, pow-fitintg and new combined approach. 0

10

20

30

40

50

60

-80 -60 -40 -20 0 20 40 60 80

ze

nith

we

t d

ela

y -

rm

s [

mm

]

latitude [degree]

pow-fit via E

log-fit via E

pow-fit via ZWD

log-fit via ZWD

pow-fit via E+ZWD

Model application - initial study for positioning

-0.80

-0.60

-0.40

-0.20

0.00

0.20

0.40

0.60

0.80

00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00

2.28

2.30

2.32

2.34

2.36

2.38

2.40

2.42

N, E

, U [m

]

ztd

[m]

09-JAN-2012

ONSA [EST-KIN-NWM]

(c) GOP/RIGTC, 14-05-30 12:30

NorthEast

UpZTD

-0.80

-0.60

-0.40

-0.20

0.00

0.20

0.40

0.60

0.80

00:00 02:00 04:00 06:00 08:00 10:00 12:00 14:00 16:00 18:00 20:00 22:00 00:00

2.28

2.30

2.32

2.34

2.36

2.38

2.40

2.42

N, E

, U [m

]

ztd

[m]

09-JAN-2012

ONSA [EST-KIN-NWM]

(c) GOP/RIGTC, 14-05-30 12:30

NorthEast

UpZTD

Plots above demonstrate PPP pseudo-kinematic positioning (ONSA) for two scenar-

ios: a) with simultaneously estimated coordinates and tropospheric parameters (left);

b) with coordinates estimated after introducing tropospheric parameters from the

global ERA Interim model (right). Left figure demonstrates a correlation between

height and troposphere which time-to-time significantly weakens the solution.

0.000

0.020

0.040

0.060

0.080

0.100

0.120

2012-01-01

2012-01-02

2012-01-03

2012-01-04

2012-01-05

2012-01-06

2012-01-07

2012-01-08

2012-01-09

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2012-01-20

2012-01-21

2012-01-22

2012-01-23

2012-01-24

2012-01-25

2012-01-26

2012-01-27

2012-01-28

2012-01-29

2012-01-30

ST

D [

m]

DRES-2012-Jan: (EST-KIN)

NorthEast

Up

0.000

0.020

0.040

0.060

0.080

0.100

0.120

2012-01-01

2012-01-02

2012-01-03

2012-01-04

2012-01-05

2012-01-06

2012-01-07

2012-01-08

2012-01-09

2012-01-10

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2012-01-13

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2012-01-22

2012-01-23

2012-01-24

2012-01-25

2012-01-26

2012-01-27

2012-01-28

2012-01-29

2012-01-30

ST

D [

m]

DRES-2012-Jan: (NWM-KIN)

NorthEast

Up

0.000

0.020

0.040

0.060

0.080

0.100

0.120

2012-01-01

2012-01-02

2012-01-03

2012-01-04

2012-01-05

2012-01-06

2012-01-07

2012-01-08

2012-01-09

2012-01-10

2012-01-11

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2012-01-23

2012-01-24

2012-01-25

2012-01-26

2012-01-27

2012-01-28

2012-01-29

2012-01-30

ST

D [

m]

DRES-2012-Jan: (NWM-KIN)

NorthEast

Up

Figures above show monthly coordinate repeatabilities (DRES) demonstrating the

better performance for height with tropospheric delays introduced from the external

model and when compare to simultaneously estimated ZTDs and coordinates.

0.002

0.004

0.006

0.008

0.010

0.012

0.014

0.016

0 10 20 30 40 50

RM

S Z

TD

[m

]

HOUR [#5-minutes ]

Comparing of RMS errors:ONSA-Jan-2012

IGS - NWM

*smt - *flt

0.002

0.004

0.006

0.008

0.010

0.012

0.014

0.016

0 10 20 30 40 50

RM

S Z

TD

[m

]

HOUR [#5-minutes ]

Comparing of RMS errors:ONSA-Jan-2012

IGS - NWM

*smt - *flt

0.000

0.010

0.020

0.030

0.040

0.050

0.060

0.070

0 10 20 30 40 50

RM

S Z

TD

[m

]

HOUR [#5-minutes ]

Comparing of RMS errors:ONSA-2012

IGS-PPPIGS-NWM

Last plots compare ZTD accuracies during the PPP initialization (ONSA) and ZTD

accuracies from the ERA Interim model. Note the results are from the winter period;

ZTD accuracy of ERA Interim can be double worse.

ERA Interim ZTD assessment

2

2.1

2.2

01/07/12 01/14/12 01/21/12 01/28/12-0.04

-0.02

0

0.02

0.04

ZT

D [m

]

Diffe

rence [m

]

EPOCH [#5-minutes ]

ANKR-2012-Jan: ZTD (IGS-NWM)

Diff IGS NWM

2

2.1

2.2

01/07/12 01/14/12 01/21/12 01/28/12-0.04

-0.02

0

0.02

0.04

ZT

D [m

]

Diffe

rence [m

]

EPOCH [#5-minutes ]

ANKR-2012-Jan: ZTD (IGS-NWM)

Diff IGS NWM

2.1

2.2

2.3

07/07/12 07/14/12 07/21/12 07/28/12-0.04

-0.02

0

0.02

0.04

ZT

D [m

]

Diffe

rence [m

]

EPOCH [#5-minutes ]

ANKR-2012-Jul: ZTD (IGS-NWM)

Diff IGS NWM

2.1

2.2

2.3

07/07/12 07/14/12 07/21/12 07/28/12-0.04

-0.02

0

0.02

0.04

ZT

D [m

]

Diffe

rence [m

]

EPOCH [#5-minutes ]

ANKR-2012-Jul: ZTD (IGS-NWM)

Diff IGS NWM

Comparison of ERA Interim global numerical weather data field and IGS final tro-

pospheric products. Plots display ZTDs (and ZTD differences) between IGS final

product and ZTDs calculated from the ERA Interim numerical weather data field

during two months (seasons): January and July, 2013.

Reference

1. Askne J, Nordius H (1987) Estimation of tropospheric delay for microwaves from

surface weather data, In: Radio Science, 22(3):379–386

2. Collins JP (1997) Assessment and Development of a Tropospheric Delay Model

for Aircraft Users of the Global Positioning System, M.Sc.E. thesis, Department

of Geodesy and Geomatics Engineering Technical Report No. 203, University of

New Brunswick, Fredericton, New Brunswick, Canada, 174 pp.

3. Dousa J, Elias M (2014) An improved model for calculating tropospheric wet

delay, Geophysical Research Letters (accepted on 6 June, 2014)

4. Marquardt, D. (1963) An algorithm for least-squares estimation of nonlinear pa-

rameters, J Soc Ind Appl Math, 11(2):431–441

Acknowledgement: The model development was supported by the ESA ProjectTrop4LAS and the Czech Science Foundation (P209/12/2207). We acknowledge

the ERA Interim data provided by the European Centre for Medium-Range Weather

Forecasts (ECMWF).

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