Impact of second-order ionospheric delays on troposphere ZWD … · 2019-01-31 ·...

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Impact of second-order ionospheric delays on troposphere ZWD estimation with GPS and BeiDou measurements Shaocheng ZHANG 1 , Lei FANG 1 , Guangxing WANG 1 , Xinzhe WANG 2 1.China University of Geosciences, Wuhan 2. Wuhan University Email[email protected] Oct. 29~Nov. 2, 2018 IGS Workshop 2018

Transcript of Impact of second-order ionospheric delays on troposphere ZWD … · 2019-01-31 ·...

Page 1: Impact of second-order ionospheric delays on troposphere ZWD … · 2019-01-31 · 测量学教研室 Impact of second-order ionospheric delays on troposphere ZWD estimation with

测量学教研室

Impact of second-order ionospheric delays on troposphere ZWD estimation with GPS

and BeiDou measurements

Shaocheng ZHANG1, Lei FANG1, Guangxing WANG1, Xinzhe WANG2

1.China University of Geosciences, Wuhan 2. Wuhan University

Email:[email protected]

Oct. 29~Nov. 2, 2018 IGS Workshop 2018

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Contents

• Introduction − Ionosphere delays on GNSS signals

− Characteristic of second-order ionosphere delays

− Impact on PPP results

• Troposphere zenith wet delay (ZWD) Estimation − Coordinate-fixed PPP estimation

− Block-wised least square for receiver clock & ISB errors

• Analysis results − Real observation results

− Simulation demonstration

• Summary & Conclusions

2 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

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Introduction

• High-order ionosphere delays on GNSS signals − Ionosphere delays on carrier phase (L) & code (P) measurements

here

after ionosphere-free linear combination

3 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

𝐼𝐼𝐼𝐿,𝑓 = −𝐼1,𝑓 − 𝐼2,𝑓 −𝐼3,𝑓…

𝐼𝐼𝐼𝑃,𝑓 = 𝐼1,𝑓 + 2𝐼2,𝑓 +𝐼3,𝑓…

𝐼1,𝑓 = 40.309∙𝑆𝑆𝑆𝑆𝑓2

𝐼2,𝑓 = 1.1284×1012∙𝐵∙cos 𝜃∙STEC𝑓3

𝐿IF =𝑓12

𝑓12 − 𝑓22𝐿1 −

𝑓12

𝑓12 − 𝑓22𝐿2

𝐼1,IF = 0

𝐼2,IF ≠ 0

𝐼3,𝑓 =812.42·∫ 𝑁𝑒2𝑑𝑑+1.5793·1022·𝐵2·(1+𝑐𝑐𝑐2𝜃)·𝑆𝑆𝑆𝑆

𝑓4

𝐼3,IF ≠ 0

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Introduction

• Characteristic of second-order ionosphere delays − Our research focus on high-order ionosphere residuals, and I2 delays

were taken for instance.

here B is the geomagnetic field value; θ is the angle between geomagnetic field and GNSS signals;

STEC is the total electronic content on the slant signal path; f is the signal frequency.

4 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

𝐼2,𝑓 = 1.1284×1012∙𝐵∙cos 𝜃∙STEC𝑓3

I2 delay on each GNSS signal was calculated with IGS final TEC map and

IGRF-12th model (International Geomagnetic Reference Field).

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Introduction

• I2 delays on GNSS ionosphere-free observations during days of high TEC level (DOY 79~85, 2016) – Three stations located in northern hemisphere, equator area and

southern hemisphere

5 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

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Introduction

• I2 delays on GNSS ionosphere-free observations during days of low TEC level (DOY 79~85, 2018) – Three stations located in northern hemisphere, equator area and

southern hemisphere

6 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

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• Impact on kinematic PPP when TEC is high – 21 IGS stations

• GPS-only solutions

• Jan 1st, 2014 (high TEC year)

• 24 hours with 30 seconds interval

7 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

Introduction

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• Coordinate-fixed PPP estimation − Stations with precise position information

− Troposphere delays on slant path were modeled with three components: the hydrostatic, wet and horizontal gradient [Davis et al, 1993]

𝐿𝐼𝐼𝐺 = 𝜌𝐺 + 𝑡𝑟 − 𝑡𝑐𝐺 + 𝑇𝐺 + 𝑁𝐼𝐼𝐺 + 𝜀𝐿𝐺 𝐿𝐼𝐼𝑆 = 𝜌𝑆 + 𝑡𝑟 − 𝑡𝑐𝑆 + 𝐼𝐼𝐼𝐺,𝑆 + 𝑇𝑆 + 𝑁𝐼𝐼𝑆 + 𝜀𝐿𝑆 𝑃𝐼𝐼𝐺 = 𝜌𝐺 + 𝑡𝑟 − 𝑡𝑐𝐺 + 𝑇𝐺 + 𝜀𝑃𝐺 𝑃𝐼𝐼𝑆 = 𝜌𝑆 + 𝑡𝑟 − 𝑡𝑐𝑆 + 𝐼𝐼𝐼𝐺,𝑆 + 𝑇𝑆 + 𝜀𝑃𝑆

Troposphere ZWD Estimation

8 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

𝑇𝑆 = 𝑚ℎ · 𝑍𝑍𝑍 + 𝑚𝑤 · 𝑍𝑍𝑍 + 𝑚𝑤 · cot (𝑒𝑒𝑒𝑒) · (𝐺𝑁 · cos (𝑎𝑎𝑎𝑚) + 𝐺𝑆 · sin (𝑎𝑎𝑎𝑚))

−𝐼2𝐺 −𝐼2𝑆 +2 · 𝐼2𝐺 +2 · 𝐼2𝑆

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Troposphere ZWD Estimation

• Coordinate-fixed PPP estimation − The function could be summarized as least square model as following:

− Least square solution for the un-known parameters X will be:

Impact of second-order ionospheric delays

9 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

𝑋 = 𝑡𝑟 , 𝐼𝐼𝐼𝐺,𝑆 ,𝑍𝑍𝑍,𝐺𝑁,𝐺𝑆 𝑆

L= 𝐼𝑋

𝐿 =

𝐿𝐼𝐼𝐺 − 𝜌𝐺 + 𝑡𝑐𝐺 − 𝑁𝐼𝐼𝐺 𝐿𝐼𝐼𝑆 − 𝜌𝑆 + 𝑡𝑐𝑆 − 𝑁𝐼𝐼𝑆

𝑃𝐼𝐼𝐺 − 𝜌𝐺 + 𝑡𝑐𝐺

𝑃𝐼𝐼𝑆 − 𝜌𝑆 + 𝑡𝑐𝑆

∆𝐿 =

−𝐼2𝐺 −𝐼2𝑆

2 · 𝐼2𝐺 2 · 𝐼2𝑆

+∆𝐿

X= (𝐼𝑆𝑃𝐼)−1𝐼𝑆𝑃L X= (𝐼𝑆𝑃𝐼)−1𝐼𝑆𝑃L − (𝐼𝑆𝑃𝐼)−1𝐼𝑆𝑃∆L

∆𝑋=− (𝐼𝑆𝑃𝐼)−1𝐼𝑆𝑃∆L

𝑄 = 𝑑𝑎𝑎𝑑 𝜀𝐿𝐺2, 𝜀𝐿𝑆

2, 𝜀𝑃𝐺2, 𝜀𝑃𝑆

2

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Troposphere ZWD Estimation

• Block-wise least square (Xu G. 2003) − Receiver clocks & ISB errors were considered as dynamic parameters

− ZWD, GN and GE were estimated with previous 30min observation.

10 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

𝑋 = 𝑡𝑟 , 𝐼𝐼𝐼𝐺,𝑆 | 𝑍𝑍𝑍,𝐺𝑁 ,𝐺𝑆 𝑆

𝑋 = 𝑋1 𝑋2 𝑆

𝐿 = 𝐼1𝐼2

𝑋1𝑋2

𝑋2 = 𝑀2−1𝑅2

𝑀2 = 𝐼2𝑆𝑃𝐼2 − 𝐼2𝑆𝑃𝐼1 𝐼1𝑆𝑃𝐼1−1𝐼1𝑆𝑃𝐼2

𝑅2 = 𝐼2𝑆𝑃 − 𝐼2𝑆𝑃𝐼1 𝐼1𝑆𝑃𝐼1−1𝐼1𝑆𝑃 𝐿

𝑋2 = � 𝑀2,𝑖

𝑡

𝑡−30𝑚𝑖𝑚

−1

∙� 𝑅2,𝑖

𝑡

𝑡−30𝑚𝑖𝑚

∆𝑅2= 𝐼2𝑆𝑃 − 𝐼2𝑆𝑃𝐼1 𝐼1𝑆𝑃𝐼1−1𝐼1𝑆𝑃 ∆𝐿

∆𝑋2= � 𝑀2,𝑖

𝑡

𝑡−30𝑚𝑖𝑚

−1

∙� ∆𝑅2,𝑖

𝑡

𝑡−30𝑚𝑖𝑚

• Sequential solution

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Analysis results

• Real observation results – ZWD difference with & without I2 correction

– Both GPS-only and GPS/BeiDou analysis.

– Satellite number & dilution of precision on ZWD estimation.

11 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

2016.060, HKWS 2018.060, HKWS

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Analysis results

12 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

2016.060, GMSD 2018.060, GMSD

2016.060, XMIS 2018.060, XMIS

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Analysis results

• Real observation results – 10 IGS stations with real observation in

Asia-Pacific area

• GPS only vs. GPS+BeiDou

– ZWDs were calculated with previous 30min observation

• Normally used in real-time estimation

• 30 seconds interval

– Maximum ZWD difference comparison

• Four equinox & solstice days on 3 years

– The Spring & Autumnal equinox

– The Summer & Winter solstice

13 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

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Analysis results

14 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

Max

imum

ZW

D d

iffer

ence

(mm

)

Spring equinox Autumnal equinox

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Analysis results

15 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

Max

imum

ZW

D d

iffer

ence

(mm

)

Summer solstice Winter solstice

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• Simulation demonstration (Left: GPS+BeiDou; Right:GPS only) – Since only B , P and I2 are needed for the calculation, simulation is

possible without real observation L.

– 5°×5° grid range from (55°𝐼, 70°𝐸) to (55°𝑁, 160°𝐸) simulation is based on broadcast ephemeris, IGS TEC grid and IGRF 12th model

Analysis results

16 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

DOY 080, 2015 DOY 172, 2015 DOY 356, 2015

DOY 080, 2017 DOY 172, 2017 DOY 356, 2017

5:00 UTC, on high TEC epoch

Inst

anta

neou

s ZW

D d

iffer

ence

(mm

)

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Analysis results

• Maximum ZWD difference statistic from 1:00-11:00 UTC – Left:GPS+BeiDou, Right: GPS only

17 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

DOY 080, 2015 DOY 356, 2015

DOY 080, 2017 DOY 356, 2017

DOY 172, 2015

DOY 172, 2017

Max

imum

ZW

D d

iffer

ence

(mm

)

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Summary & Conclusions

• The second-order ionosphere (I2) delays on GNSS signals are several millimeters, and can reach over 1 centimeter on high TEC signal paths. They lead to south direction bias on positioning applications

• Both real data and simulated 30min estimation results shown that the I2 delays have remarkable impacts on ZWD estimation – Maximum value could reach up to 3 millimeters. – GPS+BeiDou can help decreasing the I2 impacts compared to GPS only

estimation. However, the improvement is relatively limited and not always positive.

• Considering 5~10 millimeters accuracy on ZWD estimation, the I2 delays impact should not be ignored.

• On the next solar maximum year, the expected I2 impacts on ZWD estimation may be more obvious.

18 Oct. 29~Nov. 2, 2018 IGS Workshop 2018

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Shaocheng Zhang (张绍成) China University of Geosciences, Wuhan Email:[email protected]