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1 Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore Institute of Engineering Surveying and Space Geodesy The University of Nottingham

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Page 1: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

1

Ionospheric Scintillation Effects on GPS Measurements

Professor Terry Moore

Institute of Engineering Surveying and Space Geodesy

The University of Nottingham

Page 2: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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hEPSRC funded project qStudy effects of ionospheric scintillation and of North/South TEC

gradients in Northern Europe and mid-latitudes (UK)by

qInvestigating impact on GPS applications

qAssessing impact on GPS accuracy, integrity and availability

h3 years duration

hIESSG with collaborators:

hThales Geosolutions Group Ltd

hTrinity House Lighthouse Service

hUniversity of Calgary

Ionospheric Scintillation Effects on GPS Measurements

Page 3: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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WP1 Establishment of a scintillation observing GPS network

Using an array of GPS scintillation monitorsCo-located with dual-frequency receivers

WP2 Develop data processing and archiving strategies

WP3 Assess impact on EGNOS

WP4 Assess impact on Maritime DGPS

WP5 Assess impact on different receiver technologies

WP6 Application to other satellite systems

Also: Form data base for future (next solar maximum)

Develop warning & mitigation mechanisms ?

Work Packages

Page 4: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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ID Task Name

1 WP1 - Establish Network

2 WP2 - Software Development

3 WP3 - EGNOS Performance

4 WP4 - DGPS Performance

5 WP5 - Impact on Receivers

6 WP6 - Other Applications

7

8 Progress Report #1

9 Progress Report #2

10 Progress Report #3

11 Progress Report #4

12 Final Report

13

14 Progress Meeting #1

15 Progress Meeting #2

16 Progress Meeting #3

17 Progress Meeting #4

30/08

28/02

27/02

27/11

25/03

06/09

07/03

06/03

04/12

Qtr 1 Qtr 2 Qtr 3 Qtr 4 Qtr 1 Qtr 2 Qtr 3 Qtr 4 Qtr 1 Qtr 2 Qtr 3 Qtr 4 Qtr 1 Qtr 2 Qtr 32001 2002 2003 2004

01 March 2001

Time Scale

Page 5: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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hThales SkyFix Europe Network

hNorth South Distribution (red ellipses)

hGPS Iono Scintillation Monitors

hCo-located with 2-freq receiversNOTTINGHAM

The MonitoringNetwork

Page 6: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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hGPS Silicon Valley GSV 4004

hDual Frequency 12 channel NovAtel OEM4 card

hStable ovenized crystal oscillator

hWide bandwidth to insure that all spectral componentsof amplitude and phase scintillation are measured (50 Hz raw data)

hLogs and Outputs Statistics of Phase and AmplitudeScintillation (60 seconds data)

Ionospheric Scintillation Monitor

hAlso outputs TEC and dTEC

The monitor can also track one SBAS satellite (e.g. EGNOS or WAAS)

Page 7: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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Experimental IESSG Interactive Scintillation Plots Web Interface

Page 8: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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Experimental IESSG Interactive Scintillation Plots Web Interface

Page 9: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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Station with Scintillation Data(current monitoring network, part of Thales SkyFix Network)

Station with dual frequency Data

Stations with Dual-frequency/Scintillation Data

Ny Alesund

Tromso

BergenLerwick

Hammerfest

Nottingham

Bronnoysund

79N 12E 71N 23E

70N 19E

65N 12E

60N 01W 60N 05E

53N 01W

Page 10: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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Dual-Frequency Model Residuals24 Hrs, 30 sec dual-freq data from Nottingham

02 Apr 2001Peak of the Solar Cycle(major GeomagneticStorm)

08 Jun 1997Low of the Solar Cycle

All Satellites

Bernese software

Page 11: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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Phase Scintillation Data for PRN 10, starting at 22:00 UT on 01 Apr 2001

Correlation of TEC residuals with Phase Scintillation (Iono Storm Apr 2001)

R e s id u a l s in T E C U

- 2

- 1 .5

- 1

- 0 .5

0

0 .5

1

S V 1 0 N o t t i n g h a m 0 1 - 0 2 A p r i l 2 0 0 1

0

0 . 0 5

0 . 1

0 . 1 5

0 . 2

0 . 2 5

0 . 3

2 2 2 3 0

T i m e o f D a y ( h o u r s )

Ph

ase

Sig

ma

(Rad

ian

s)

0

1 0

2 0

3 0

4 0

5 0

6 0

7 0

8 0

Ele

vatio

n A

ng

le (

Deg

rees

)

P h a s e S i g m a

E le v a t i o n a n g le

Page 12: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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L e r w i c k K i n d e x H o u r l y S t a n d a r d D e v i a t i o n 3 1 M a r c h 2 0 0 1

0 . 0

5 0 . 0

1 0 0 . 0

1 5 0 . 0

2 0 0 . 0

2 5 0 . 0

3 0 0 . 0

3 5 0 . 0

4 0 0 . 0

Correlation of TEC Variations, GPS Positioning Errors and

Hourly Standard Deviation of Geomagnetic Field

Lerwick 31 March 2001

HourlyStdev of GeomagField from Lerwick

TEC Variationsat Lerwick

40

-120

L e r w i c k - 3 D P o s i t i o n E r r o r - 3 1 M a r c h 2 0 0 1

0 . 0

2 0 . 0

4 0 . 0

6 0 . 0

8 0 . 0

1 0 0 . 0

1 2 0 . 0

GPS 3D PositioningErrors at Lerwick

120

0

Page 13: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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Spatial Analysis ofPhase Scintillation07 September 2002

Page 14: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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North-South Gradient in TEC ChangeIono Storm Nov 2001

Lat 70o NLong 19o E

Lat 60o NLong 01o W

Lat 53o NLong 01o W

Lerwick

Nottingham

Ny Alesund

Lat 79o NLong 12o E

Tromso

04 Nov 05 Nov 06 Nov 07 Nov 08 Nov

Page 15: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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TEC Change Observed at Tromso and Hammerfest on 7 November 2001

Tromso -IGS 2-freq dataprocessed with Bernese

Hammerfest -output data from GSV4004

TROMHAMM

Page 16: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

16 05 Nov 06 Nov 07 Nov

TEC change per 30 seconds

Dual Frequencyresiduals

HourlyStandard Deviationof geomagnetic field (Lerwick Observatory) 0

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

3 5 0

4 0 0

4 5 0

All satellites plotted

Lerwick Nov 01 - Correlation of TEC Variations, GPS Residuals, Phase Scintillation (Bergen) and Hourly Standard Deviation of Geomagnetic Field

GPS 3D positionResiduals

- 1 0 0

- 8 0

- 6 0

- 4 0

- 2 0

0

2 0

4 0

6 0

8 0

1 0 0

Res

idua

ls (m

eter

s)

100

Phase Scintillation(at Bergen)

Page 17: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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4th - 8th November 2001 - Sumburgh Head (TRIMBLE SSI) LERWICK (ASHTECH ZX11)

0.00

10.00

20.00

30.00

40.00

50.00

60.00

0:3004/11/2001

06:3004/11/2001

12:3004/11/2001

18:3004/11/2001

00:3005/11/2001

06:3005/11/2001

12:3005/11/2001

18:3005/11/2001

0:3006/11/2001

06:3006/11/2001

12:3006/11/2001

18:3006/11/2001

00:3007/11/2001

06:3007/11/2001

12:3007/11/2001

18:3007/11/2001

0:3008/11/2001

06:3008/11/2001

12:3008/11/2001

18:3008/11/2001

Time of Observation

% o

f obs

erva

tions

with

No

L2

0

1

2

3

4

5

6

7

8

9

10

1.504/11/2001

10.504/11/2001

19.504/11/2001

4.505/11/2001

13.505/11/2001

22.505/11/2001

7.506/11/2001

16.506/11/2001

1.507/11/2001

10.507/11/2001

19.507/11/2001

4.508/11/2001

13.508/11/2001

22.508/11/2001

Lerwick K Index- Time

Lerw

ick

K In

dex

SUM1

LERW

K Index

K i n d e x T o t a l S i g m a f o r 0 4 t o 0 8 N o v 2 0 0 1

0

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

3 5 0

4 0 0

4 5 0

1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2

t i m e ( 5 d a y s )

L2 Data Loss for Different Receivers at Lerwickand Sumburgh, 4 to 8 Nov 01

Hourly Standard Deviationof Geomagnetic Field

LERW

SUMB

Page 18: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

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DGPS Solution at Lynas from Flamborough - Hourly 2drms (m)

0.0

5.0

10.0

15.0

20.0

25.0

0:00 04/11/01

12:00 04/11/01

0:00 05/11/01

12:00 05/11/01

0:00 06/11/01

12:00 06/11/01

0:00 07/11/01

12:00 07/11/01

0:00 08/11/01

12:00 08/11/01

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

10

HD

OP

GIRD

FLAM

DGPS Solution at Girdleness from Flamborough - Hourly 2drms (m)

0.0

5.0

10.0

15.0

20.0

25.0

0:00 04/11/01

12:00 04/11/01

0:00 05/11/01

12:00 05/11/01

0:00 06/11/01

12:00 06/11/01

0:00 07/11/01

12:00 07/11/01

0:00 08/11/01

12:00 08/11/01

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

10

HD

OPNorth-South

East-West

North-South vs East-West Baseline DGPS (4 to 8 Nov 01)

2drms error (whole period) = 2.66m

2drms error (whole period) = 3.5m

FLAM

LYN

Page 19: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

19

DGPS Solution at Girdleness from Flamborough - Hourly 2drms (m)

0.0

5.0

10.0

15.0

20.0

25.0

0:00 04/11/01

12:00 04/11/01

0:00 05/11/01

12:00 05/11/01

0:00 06/11/01

12:00 06/11/01

0:00 07/11/01

12:00 07/11/01

0:00 08/11/01

12:00 08/11/01

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

10

HD

OP

DGPS Solution at Girdleness from Flamborough - Hourly 2drms (m)EGNOS Corrections applied at both ends

(SVs without correction in solution, min 4 SVs)

0.0

5.0

10.0

15.0

20.0

25.0

0:01 04/11/01

12:01 04/11/01

0:01 05/11/01

12:01 05/11/01

0:01 06/11/01

12:01 06/11/01

0:01 07/11/01

12:01 07/11/01

0:01 08/11/01

12:01 08/11/01

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

10

HD

OP

2drms error (whole period) = 2.57m

North-South

Improvement with the EGNOS Corrections on a North/South Baseline (4 to 8 Nov 01)

GIRD

FLAM

Page 20: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

20

0.0

5.0

10.0

15.0

20.0

25.0

0:01 04/11/01

12:01 04/11/01

0:01 05/11/01

12:01 05/11/01

0:01 06/11/01

12:01 06/11/01

0:01 07/11/01

12:01 07/11/01

0:01 08/11/01

12:01 08/11/01

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

10

HD

OP

2drms error (w h o le period) = 2.85m

Only 4 SVs with corrections coveredby EGNOS grid

0.0

5.0

10.0

15.0

20.0

25.0

0:01 04/11/01

12:01 04/11/01

0:01 05/11/01

12:01 05/11/01

0:01 06/11/01

12:01 06/11/01

0:01 07/11/01

12:01 07/11/01

0:01 08/11/01

12:01 08/11/01

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

10

HD

OP

2drms error (w h o le period) = 2.57m

Additional 3 SVs, even without EGNOS correction,improve solution

GIRD

FLAM

0

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

3 5 0

4 0 0

4 5 0

(SVs without correction in solution, min 4 SVs)

(SVs without correction NOT in solution, min 4 SVs)

Hourly Standard Deviation of Geomagnetic Field

However . . . .

Page 21: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

21

Possible Development of Warning Mechanisms

Prediction of Scintillation Levels with WBMOD (Wide Band Model)

hBased on climatological models of global distribution of ionospheric irregularities + propagation theory

hDeveloped by NorthWest Research Associates Inc.

hInputs: location, day of the year, local time, SSN, Kp

hRelevant outputs: S4 and Phase RMS (SPHI)

hPredictions based on the L1 GPS frequency

Page 22: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

22

Hourly Standard Deviationof Geomagnetic Field

K i n d e x T o t a l S i g m a f o r 0 4 t o 0 8 N o v 2 0 0 1

0

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

3 5 0

4 0 0

4 5 0

1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2 1 4 7 1 0 1 3 1 6 1 9 2 2

t i m e ( 5 d a y s )

0 . 0 0

2 . 0 0

4 . 0 0

6 . 0 0

8 . 0 0

1 0 . 0 0

1 2 . 0 0

0 : 3 0 0 6 : 3 0 1 2 : 3 0 1 8 : 3 0 0 0 : 3 0 0 6 : 3 0 1 2 : 3 0 1 8 : 3 0 0 : 3 0 0 6 : 3 0 1 2 : 3 0 1 8 : 3 0 0 0 : 3 0 0 6 : 3 0 1 2 : 3 0 1 8 : 3 0 0 : 3 0 0 6 : 3 0 1 2 : 3 0 1 8 : 3 0

T i m e o f O b s e r v a t i o n

% o

f o

bse

rvat

ion

s w

ith

no

L2

TEC changes

W B M O D P r e d i c t e d L 1 S P H I - L e r w i c k , 0 4 t o 0 8 N o v 0 1

0

0 . 2

0 . 4

0 . 6

0 . 8

1

1 . 2

1 . 4

1:30

7:30

13:3

0

19:3

0

1:30

07:3

0

13:3

0

19:3

0

1:30

07:3

0

13:3

0

19:3

0

1:30

07:3

0

13:3

0

19:3

0

01:3

0

07:3

0

13:3

0

19:3

0

t i m e - s t a r t i n g a t 0 : 0 0 o n 4 N o v 0 1

Pre

dic

ted

SP

HI i

n r

adia

ns

9 9 % p e r c e n t i l e l e w r _ 5 d a y s 9 9

Predicted Phase Sigma(99% percentile)

Percentage ofL2 loss on a semicodelssGPS receiver

Correlation of TEC Changes with hourly standard deviationof Geomagnetic Field, WBMOD prediction and Data Loss,

Lerwick, 4 to 8 November 2001

Page 23: Ionospheric Scintillation Effects on GPS Measurements · Ionospheric Scintillation Effects on GPS Measurements Professor Terry Moore ... Ionospheric Scintillation Effects on GPS Measurements

23

D G P S S o lu t io n a t T r o n d h e im f r o m O s lo - H o u r l y 2 d r m s (m )

0 .0

5 .0

1 0 .0

1 5 .0

2 0 .0

2 5 .0

0 : 0 0 0 4 / 1 1 / 0 1

1 2 : 0 0 0 4 / 1 1 / 0 1

0 : 0 0 0 5 / 1 1 / 0 1

1 2 : 0 0 0 5 / 1 1 / 0 1

0 : 0 0 0 6 / 1 1 / 0 1

1 2 : 0 0 0 6 / 1 1 / 0 1

0 : 0 0 0 7 / 1 1 / 0 1

1 2 : 0 0 0 7 / 1 1 / 0 1

0 : 0 0 0 8 / 1 1 / 0 1

1 2 : 0 0 0 8 / 1 1 / 0 1

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

1 0

HD

OP

2 d r m s e r r o r (w h o le p e r io d ) = 4 . 3 0 m

Correlation of WBMOD phase and amplitude scintillation predictions with DGPS and EGNOS user 2drms - Trondheim, 4 to 8

Nov 2001

0

0 . 1

0 . 2

0 . 3

0 . 4

0 . 5

0 . 6

0 . 7

1:30

4:30

7:30

10:3

0

13:3

0

16:3

0

19:3

0

22:3

0

1:30

04:3

0

07:3

0

10:3

0

13:3

0

16:3

0

19:3

0

22:3

0

1:30

04:3

0

07:3

0

10:3

0

13:3

0

16:3

0

19:3

0

22:3

0

1:30

04:3

0

07:3

0

10:3

0

13:3

0

16:3

0

19:3

0

22:3

0

01:3

0

04:3

0

07:3

0

10:3

0

13:3

0

16:3

0

19:3

0

22:3

0

0

0 . 0 5

0 . 1

0 . 1 5

0 . 2

0 . 2 5

1:30

7:30

13:30

19:30 1:3

007:

3013:

3019:

30 1:30

07:30

13:30

19:30 1:3

007:

3013:

3019:

3001:

3007:

3013:

3019:

30

Mean Predicted Phase Scintillation

Mean Predicted AmplitudeScintillation

D G P S S o lu t io n a t T r o n d h e im f r o m O s lo - H o u r l y 2 d r m s (m )E G N O S C o r r e c t io n a p p lie d a t b o th e n d s

(S V s w ith o u t c o r r e c t io n in s o lu t io n , m in 4 S V s )

0 .0

5 .0

1 0 .0

1 5 .0

2 0 .0

2 5 .0

0 : 0 1 0 4 / 1 1 / 0 1

1 2 : 0 1 0 4 / 1 1 / 0 1

0 : 0 1 0 5 / 1 1 / 0 1

1 2 : 0 1 0 5 / 1 1 / 0 1

0 : 0 1 0 6 / 1 1 / 0 1

1 2 : 0 1 0 6 / 1 1 / 0 1

0 : 0 1 0 7 / 1 1 / 0 1

1 2 : 0 1 0 7 / 1 1 / 0 1

0 : 0 1 0 8 / 1 1 / 0 1

1 2 : 0 1 0 8 / 1 1 / 0 1

2drm

s (m

)

0

1

2

3

4

5

6

7

8

9

1 0

HD

OP

2 d r m s e r r o r (w h o le p e r io d ) = 3 .6 9 m TRDS

OSLO