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Aeronautics and Aerospace Open Access Journal

Technical Paper Volume 3 Issue 3

Adjustment of the dual frequency altimeter low subsection backscatter coefficient statistical model 

Zhuhui Jiang,1,2,3 Wei Zhang4

1State Key Laboratory of Geo-information Engineering, China
2International Space University, France
3Institute of Atmospheric Physics, Chinese Academy of Sciences, LAGEO, China
4Chinese satellite maritime tracking and control department, China

Correspondence: Zhuhui Jiang, State Key Laboratory of Geo-information Engineering, Xi’an 710054, China, Tel 0033766146906

Received: July 05, 2019 | Published: July 19, 2019

Citation: Jiang Z, Zhang E. Adjustment of the dual frequency altimeter low subsection backscatter coefficient statistical model. Aeron Aero Open Access J. 2019;3(3):115-118. DOI: 10.15406/aaoaj.2019.03.00087

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Abstract

The Ku band and C band backscatter coefficient statistical relationship plays an important role in dual frequency altimeter wind speed retrieval when it is rain. In order to improve the precision of wind speed retrieval, it is very important to put forward a proper statistical relationship. Jiang’s relationship has higher precision than Quartly’s and Yang’s relationship between 12dB and 26dB. But if C band backscatter coefficient is 12dB, the wind speed is 27.3683m/s, so if the wind speed is larger than 27.3683m/s, Jiang’s relationship can’t work. High wind speed condition is one of the most important sea phenomena, so we eagerly need to build a new relationship that can apply to the entire sea phenomenon. This paper is based on the specular scattering theory, analyses the low backscatter coefficient subsection’s relationship, put forward a method that if C band backscatter coefficient is between 12dB and 26dB, Jiang’s relationship is used, if C band backscatter coefficient is smaller than 12dB, Yang’s relationship is used. This relationship redounds to improve wind speed retrieval when it is rain.

Keywords: dual frequency altimeter, statistical model, backscatter coefficient, low subsection

Chinese classification code:

84. 40. Xb, 92. 60. Gn

Introduction

NASA and French space agency launched Topex/Poseidon in 1992, and Topex is the first dual-frequency radar altimeter (Ku band 13.6GHz and C band 5.3GHz). The initial thought of the equipment of C band payload is to retrieve the total electron content. There is substantial progress for the altimeter sea surface wind speed error reduction caused by rain because the dual-frequency altimeter is available. Quartly et al.,1 point out that the main influence of rain to radar altimeter echo is attenuating the signal; it is different between the attenuation of C band backscatter coefficient σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ and that of Ku band backscatter coefficient   σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca GGGcGaeq4Wdm3damaaDaaaleaapeGaam4saiaadwhaa8aabaWdbiaa d+gaaaaaaa@3D9C@ in the rain. They established a statistical relationship model between σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ and   σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca GGGcGaeq4Wdm3damaaDaaaleaapeGaam4saiaadwhaa8aabaWdbiaa d+gaaaaaaa@3D9C@ under the assumption of no rain, open sea, no sea ice and small signal deviation angle. The literature2-5 also established a statistical model and carried out relevant research of decrease rain influence. The precipitation capacity of 10 mm/h causes the signal attenuation of about 4.5dB for Ku band and about 0.26 for C band. If the backscatter error is 0.1dB, the retrieved wind speed error is about 0.3m/s in moderate wind, so the backscatter coefficient statistical model is very important for rain influence reduction. The amount of trial data is too small for the backscatter coefficient statistical model of the literature.1 The statistical relationship model established in the literature5 is a piecewise linear function, which is disconnected at the link points. Jiang et al.,6 presented a new backscatter coefficient statistical model with 7 and a half years Jason-1 data by a polynomial fitting method to solve above problems, but the available range of C band backscatter coefficient is only 12 dB to 26 dB. C band backscatter coefficient of 12 dB corresponds to the sea surface wind speed of about 27m/s by calculation, which means that if the sea surface wind speed is higher than 27m/s, the model of literature5 lose effectiveness. However, high wind speed and severe sea situation often cause tremendous disasters, so it is necessary to research low subsection backscatter coefficient statistical relationship.

In this paper, the low subsection backscatter coefficient statistical relationship of C band and Ku band is analyzed basing on the specular scattering theory in section 2, the accuracies of different methods are evaluated in section 3, and an adjusted method is put forward that if C band backscatter coefficient is in the range of 12 dB to 26 dB, the method of literature6 is available, and if C band backscatter coefficient is below 12 dB, the method of literature5 is available. The adjusted method can improve sea surface wind speed accuracy under rainfall conditions.

The basic theory of wind speed inversion of dual-frequency altimeter under rainfall condition

The influence of rainfall on the radar signal can be obtained by the function proposed by Marshall Palmer

k=a R b MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGRbGaeyypa0JaamyyaiaadkfapaWaaWbaaSqabeaapeGaamOyaaaa aaa@3C72@

where k refers to the absorption coefficient, R is the precipitation capacity, a and b are coefficients determined by radar frequency.

The total attenuation of radar signal emission and reception follows the following relation,

A=2kh=2ha R b MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGbbGaeyypa0JaaGOmaiaadUgacaWGObGaeyypa0JaaGOmaiaadIga caWGHbGaamOua8aadaahaaWcbeqaa8qacaWGIbaaaaaa@4190@

where h is the height of rainfall.

Therefore, there is the following relationship between rainfall and the attenuation intensity caused by rainfall

R= ( A 2ha ) 1 b MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGsbGaeyypa0ZaaeWaa8aabaWdbmaalaaapaqaa8qacaWGbbaapaqa a8qacaaIYaGaamiAaiaadggaaaaacaGLOaGaayzkaaWdamaaCaaale qabaWdbmaaliaapaqaa8qacaaIXaaapaqaa8qacaWGIbaaaaaaaaa@40F2@ (1)

for a=34.6× 10 3 , b=1.109 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca qGHbGaeyypa0JaaG4maiaaisdacaGGUaGaaGOnaiabgEna0kaaigda caaIWaWdamaaCaaaleqabaWdbiabgkHiTiaaiodaaaGccaGGSaGaai iOaiaadkgacqGH9aqpcaaIXaGaaiOlaiaaigdacaaIWaGaaGyoaaaa @4955@ Ku band, a=1.06× 10 3 , b=1.393 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca qGHbGaeyypa0JaaGymaiaac6cacaaIWaGaaGOnaiabgEna0kaaigda caaIWaWdamaaCaaaleqabaWdbiabgkHiTiaaiodaaaGccaGGSaGaai iOaiaadkgacqGH9aqpcaaIXaGaaiOlaiaaiodacaaI5aGaaG4maaaa @4954@ for C band.

The basic iterative method2,7-10 for the inversion of wind speed by dual-frequency altimeter under rainfall condition is

First, estimate whether it is rain according to the backscatter coefficient statistical model of between σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ and   σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca GGGcGaeq4Wdm3damaaDaaaleaapeGaam4saiaadwhaa8aabaWdbiaa d+gaaaaaaa@3D9C@ . If it is not rain, jump out of iteration;

If it is rain, σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ is substituted into the statistical model to obtain the ideal backscatter coefficient of Ku band σ Ku o' MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baiaa cEcaaaaaaa@3D23@ , and then the signal attenuation of Ku band is obtained by comparing with it, A Ku = σ Ku o' σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGbbWdamaaBaaaleaapeGaam4saiaadwhaa8aabeaak8qacqGH9aqp cqaHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Bai aacEcaaaGccqGHsislcqaHdpWCpaWaa0baaSqaa8qacaWGlbGaamyD aaWdaeaapeGaam4Baaaaaaa@4710@ ;

Precipitation capacity R can be calculated by equation (1). R is independent of the radar signal, so the corresponding C band signal attenuation A C MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGbbWdamaaBaaaleaapeGaam4qaaWdaeqaaaaa@3974@ can be calculated by equation (1). The signal attenuation of C band is σ C o' = σ C o + A C MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbGaai4jaaaa kiabg2da9iabeo8aZ9aadaqhaaWcbaWdbiaadoeaa8aabaWdbiaad+ gaaaGccqGHRaWkcaWGbbWdamaaBaaaleaapeGaam4qaaWdaeqaaaaa @43EF@ ;

The new signal attenuation of Ku band A Ku ' MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGbbWdamaaDaaaleaapeGaam4saiaadwhaa8aabaWdbiaacEcaaaaa aa@3B32@ can be obtained by substituting σ C o' MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbGaai4jaaaa aaa@3C21@ and σ Ku o' MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baiaa cEcaaaaaaa@3D23@ into the statistical relationship;

Judge whether A Ku ' MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGbbWdamaaDaaaleaapeGaam4saiaadwhaa8aabaWdbiaacEcaaaaa aa@3B32@ is less than a certain threshold, if it is true, jump out of the iteration, and retrieve the sea surface wind speed by the corrected σ Ku o' MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baiaa cEcaaaaaaa@3D23@ . If it is false, go to ‘c’ and continue the iteration.

The precipitation capacity of 10 mm/h causes the signal attenuation of about 4.5dB for Ku band and about 0.26 for C band by equation (1). If the backscatter error is 0.1dB, the retrieved wind speed error is about 0.3m/s in the moderate wind from the Modified Chelton and Wentz Wind Speed Model Function (MCW), so the statistical model has important effects on wind speed retrieval.

Backscatter coefficient statistical model

There is a certain correlation between σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ and   σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca GGGcGaeq4Wdm3damaaDaaaleaapeGaam4saiaadwhaa8aabaWdbiaa d+gaaaaaaa@3D9C@ physically, but this correlation cannot be deduced theoretically2 which is usually based on empirical fitting.

Quartly et al.,1 analyzed the influence of precipitation ideally on altimeter wind speed retrieval using Topex data. They suggested that the C band backscatter coefficient could be used to distinguish rain or not from the different influence on a different frequency. Forwardly, a piecewise statistical model fitting from Topex data from December 1992 to October 1993 (Cycle 11, 12, 21, 22, 29, 30, 39 and 40) is put forward ignoring conditions that the liquid water content is less than 0.2mm.

  σ Ku o =8.99+1.19( σ C o 13.0), σ C o <13.0dB; σ Ku o =8.99+1.52( σ C o 13.0), σ C o [13.0dB,14.0dB); σ Ku o =10.51+1.21( σ C o 14.0), σ C o [14.0dB,14.7dB); σ Ku o =11.36+0.89( σ C o 14.7), σ C o [14.7dB,15.7dB); σ Ku o =12.25+0.72( σ C o 15.7), σ C o [15.7dB,16.2dB); σ Ku o =12.61+0.86( σ C o 16.2), σ C o [16.2dB,19.4dB); σ Ku o =15.36+0.96( σ C o 19.4), σ C o [19.4dB,21.0dB); σ Ku o =16.90+1.07( σ C o 21.0), σ C o [21.0dB,24.2dB); σ Ku o =20.31+1.11( σ C o 24.2), σ C o [24.2dB,26.0dB); σ Ku o =undefined, σ C o 26.2dB. } MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca qGGcWdamaaciaaeaqabeaacqaHdpWCdaqhaaWcbaGaam4saiaadwha aeaacaWGVbaaaOGaeyypa0JaaGjbVlaaiIdacaGGUaGaaGyoaiaaiM dacqGHRaWkcaaIXaGaaiOlaiaaigdacaaI5aGaaiikaiabeo8aZnaa DaaaleaacaWGdbaabaGaam4BaaaakiabgkHiTiaaigdacaaIZaGaai OlaiaaicdacaGGPaGaaiilaiaaysW7caaMe8UaaGjbVlabeo8aZnaa DaaaleaacaWGdbaabaGaam4BaaaakiabgYda8iaaigdacaaIZaGaai OlaiaaicdacaWGKbGaamOqaiaacUdaaeaacqaHdpWCdaqhaaWcbaGa am4saiaadwhaaeaacaWGVbaaaOGaeyypa0JaaGioaiaac6cacaaI5a GaaGyoaiabgUcaRiaaigdacaGGUaGaaGynaiaaikdacaGGOaGaeq4W dm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaeyOeI0IaaGymaiaaio dacaGGUaGaaGimaiaacMcacaGGSaGaaGjbVlaaysW7caaMe8Uaeq4W dm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaeyicI4Saai4waiaaig dacaaIZaGaaiOlaiaaicdacaWGKbGaamOqaiaacYcacaaIXaGaaGin aiaac6cacaaIWaGaamizaiaadkeacaGGPaGaai4oaaqaaiabeo8aZn aaDaaaleaacaWGlbGaamyDaaqaaiaad+gaaaGccqGH9aqpcaaIXaGa aGimaiaac6cacaaI1aGaaGymaiabgUcaRiaaigdacaGGUaGaaGOmai aaigdacaGGOaGaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGa eyOeI0IaaGymaiaaisdacaGGUaGaaGimaiaacMcacaGGSaGaaGjbVl aaysW7cqaHdpWCdaqhaaWcbaGaam4qaaqaaiaad+gaaaGccqGHiiIZ caGGBbGaaGymaiaaisdacaGGUaGaaGimaiaadsgacaWGcbGaaiilai aaigdacaaI0aGaaiOlaiaaiEdacaWGKbGaamOqaiaacMcacaGG7aaa baGaeq4Wdm3aa0baaSqaaiaadUeacaWG1baabaGaam4Baaaakiabg2 da9iaaigdacaaIXaGaaiOlaiaaiodacaaI2aGaey4kaSIaaGimaiaa c6cacaaI4aGaaGyoaiaacIcacqaHdpWCdaqhaaWcbaGaam4qaaqaai aad+gaaaGccqGHsislcaaIXaGaaGinaiaac6cacaaI3aGaaiykaiaa cYcacaaMe8Uaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaey icI4Saai4waiaaigdacaaI0aGaaiOlaiaaiEdacaWGKbGaamOqaiaa cYcacaaIXaGaaGynaiaac6cacaaI3aGaamizaiaadkeacaGGPaGaai 4oaaqaaiabeo8aZnaaDaaaleaacaWGlbGaamyDaaqaaiaad+gaaaGc cqGH9aqpcaaIXaGaaGOmaiaac6cacaaIYaGaaGynaiabgUcaRiaaic dacaGGUaGaaG4naiaaikdacaGGOaGaeq4Wdm3aa0baaSqaaiaadoea aeaacaWGVbaaaOGaeyOeI0IaaGymaiaaiwdacaGGUaGaaG4naiaacM cacaGGSaGaaGjbVlabeo8aZnaaDaaaleaacaWGdbaabaGaam4Baaaa kiabgIGiolaacUfacaaIXaGaaGynaiaac6cacaaI3aGaamizaiaadk eacaGGSaGaaGymaiaaiAdacaGGUaGaaGOmaiaadsgacaWGcbGaaiyk aiaacUdaaeaacqaHdpWCdaqhaaWcbaGaam4saiaadwhaaeaacaWGVb aaaOGaeyypa0JaaGjbVlaaigdacaaIYaGaaiOlaiaaiAdacaaIXaGa ey4kaSIaaGimaiaac6cacaaI4aGaaGOnaiaacIcacqaHdpWCdaqhaa WcbaGaam4qaaqaaiaad+gaaaGccqGHsislcaaIXaGaaGOnaiaac6ca caaIYaGaaiykaiaacYcacaaMe8Uaeq4Wdm3aa0baaSqaaiaadoeaae aacaWGVbaaaOGaeyicI4Saai4waiaaigdacaaI2aGaaiOlaiaaikda caWGKbGaamOqaiaacYcacaaIXaGaaGyoaiaac6cacaaI0aGaamizai aadkeacaGGPaGaai4oaaqaaiabeo8aZnaaDaaaleaacaWGlbGaamyD aaqaaiaad+gaaaGccqGH9aqpcaaMe8UaaGymaiaaiwdacaGGUaGaaG 4maiaaiAdacqGHRaWkcaaIWaGaaiOlaiaaiMdacaaI2aGaaiikaiab eo8aZnaaDaaaleaacaWGdbaabaGaam4BaaaakiabgkHiTiaaigdaca aI5aGaaiOlaiaaisdacaGGPaGaaiilaiaaysW7cqaHdpWCdaqhaaWc baGaam4qaaqaaiaad+gaaaGccqGHiiIZcaGGBbGaaGymaiaaiMdaca GGUaGaaGinaiaadsgacaWGcbGaaiilaiaaikdacaaIXaGaaiOlaiaa icdacaWGKbGaamOqaiaacMcacaGG7aaabaGaeq4Wdm3aa0baaSqaai aadUeacaWG1baabaGaam4Baaaakiabg2da9iaaysW7caaIXaGaaGOn aiaac6cacaaI5aGaaGimaiabgUcaRiaaigdacaGGUaGaaGimaiaaiE dacaGGOaGaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaeyOe I0IaaGOmaiaaigdacaGGUaGaaGimaiaacMcacaGGSaGaaGjbVlabeo 8aZnaaDaaaleaacaWGdbaabaGaam4BaaaakiabgIGiolaacUfacaaI YaGaaGymaiaac6cacaaIWaGaamizaiaadkeacaGGSaGaaGOmaiaais dacaGGUaGaaGOmaiaadsgacaWGcbGaaiykaiaacUdaaeaacqaHdpWC daqhaaWcbaGaam4saiaadwhaaeaacaWGVbaaaOGaeyypa0JaaGjbVl aaikdacaaIWaGaaiOlaiaaiodacaaIXaGaey4kaSIaaGymaiaac6ca caaIXaGaaGymaiaacIcacqaHdpWCdaqhaaWcbaGaam4qaaqaaiaad+ gaaaGccqGHsislcaaIYaGaaGinaiaac6cacaaIYaGaaiykaiaacYca caaMe8Uaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaeyicI4 Saai4waiaaikdacaaI0aGaaiOlaiaaikdacaWGKbGaamOqaiaacYca caaIYaGaaGOnaiaac6cacaaIWaGaamizaiaadkeacaGGPaGaai4oaa qaaiabeo8aZnaaDaaaleaacaWGlbGaamyDaaqaaiaad+gaaaGccqGH 9aqpcaWG1bGaamOBaiaadsgacaWGLbGaamOzaiaadMgacaWGUbGaam yzaiaadsgacaGGSaGaaGjbVlaaysW7caaMe8UaaGjbVlaaysW7caaM e8UaaGjbVlaaysW7caaMe8UaaGjbVlaaysW7caaMe8UaaGjbVlaays W7caaMe8UaaGjbVlaaysW7caaMe8UaaGjbVlabeo8aZnaaDaaaleaa caWGdbaabaGaam4BaaaakiabgwMiZkaaikdacaaI2aGaaiOlaiaaik dacaWGKbGaamOqaiaac6caaaGaayzFaaaaaa@EF30@ (2)

Yang5 suggested a piecewise statistical model using piecewise linear fitting by Jason-1 data from March 2006 to February 2007 (Cycle 155, 157, 159, 163, 167, 169, 172, 174, 176, 180, 184 and 188) (Table 1). Its expression is

σ Ku o =f[ σ C o ]= c 1 × σ C o + c 2 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadUeacaWG1baabaGaam4Baaaakiabg2da9iaadAgacaGGBbGa eq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaaiyxaiabg2da9i aadogadaWgaaWcbaGaaGymaaqabaGccqGHxdaTcqaHdpWCdaqhaaWc baGaam4qaaqaaiaad+gaaaGccqGHRaWkcaWGJbWaaSbaaSqaaiaaik daaeqaaaaa@4EE9@ (3)

Quartly et al.,1 and Yang5 fitted the statistical model by 80 days and 120 days data respectively, the amount of data is small and unrepresentative. The piecewise linear function link points of Yang5 are disconnected.

Jiang et al.,6 presented a new backscatter coefficient statistical model with 7 and a half years no rain, open sea, no sea ice and small signal deviation angle Jason-1 data by polynomial fitting method to solve above problems, but the available range of C band backscatter coefficient is only 12 dB to 26 dB (Equation 4). The fitting coefficients are listed in Table 2.

σ Ku o =f( σ C o )=a ( σ C o ) 6 +b ( σ C o ) 5 +c ( σ C o ) 4 +d ( σ C o ) 3 +e ( σ C o ) 2 +f( σ C o )+g MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadUeacaWG1baabaGaam4Baaaakiabg2da9iaadAgacaGGOaGa eq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaaiykaiabg2da9i aadggacaGGOaGaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGa aiykamaaCaaaleqabaGaaGOnaaaakiabgUcaRiaadkgacaGGOaGaeq 4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaaiykamaaCaaaleqa baGaaGynaaaakiabgUcaRiaadogacaGGOaGaeq4Wdm3aa0baaSqaai aadoeaaeaacaWGVbaaaOGaaiykamaaCaaaleqabaGaaGinaaaakiab gUcaRiaadsgacaGGOaGaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVb aaaOGaaiykamaaCaaaleqabaGaaG4maaaakiabgUcaRiaadwgacaGG OaGaeq4Wdm3aa0baaSqaaiaadoeaaeaacaWGVbaaaOGaaiykamaaCa aaleqabaGaaGOmaaaakiabgUcaRiaadAgacaGGOaGaeq4Wdm3aa0ba aSqaaiaadoeaaeaacaWGVbaaaOGaaiykaiabgUcaRiaadEgaaaa@72F8@ (4)

The above three statistical model standard deviations are listed in Table 3. Jiang et al.,6 standard deviations are significantly better between 12 dB to 26 dB than the standard deviation of Quartly et al.,1 and Yang.5 Only in the range of 12 dB to 15 dB, the accuracy of Yang5 is higher than Jiang et al.6, the accuracy of Jiang et al.,6 are very high in the rest of the range.

σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacqaHdp WCkmaaDaaaleaajugWaiaadoeaaSqaaKqzadGaam4Baaaaaaa@3CA2@ range/dB

c 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGJbWaaSbaaSqaaiaaigdaaeqaaaaa@395C@ c 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGJbWaaSbaaSqaaiaaikdaaeqaaaaa@395D@

σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsacqaHdp WCkmaaDaaaleaajugWaiaadoeaaSqaaKqzadGaam4Baaaaaaa@3CA2@ range /dB

c 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGJbWaaSbaaSqaaiaaigdaaeqaaaaa@395C@ c 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca WGJbWaaSbaaSqaaiaaikdaaeqaaaaa@395D@
σ C o <13.0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadoeaaeaacaWGVbaaaOGaeyipaWJaaGymaiaaiodacaGGUaGa aGimaaaa@3F0B@

1.202

-7.086

16.2 σ C o <19.4 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGymaiaaiAdaca GGUaGaaGOmaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaigdacaaI5aGaaiOlaiaaisdaaaa@43B2@

0.894

-1.829

13.0 σ C o <14.0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGymaiaaiodaca GGUaGaaGimaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaigdacaaI0aGaaiOlaiaaicdaaaa@43A5@

1.471

-10.602

19.4 σ C o <21.0 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGymaiaaiMdaca GGUaGaaGinaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaikdacaaIXaGaaiOlaiaaicdaaaa@43AC@

0.916

-2.23

14.0 σ C o <14.7 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGymaiaaisdaca GGUaGaaGimaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaigdacaaI0aGaaiOlaiaaiEdaaaa@43AD@

1.527

-11.357

21.0 σ C o <24.2 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGOmaiaaigdaca GGUaGaaGimaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaikdacaaI0aGaaiOlaiaaikdaaaa@43A6@

1.026

-4.498

14.7 σ C o <15.7 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGymaiaaisdaca GGUaGaaG4naiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaigdacaaI1aGaaiOlaiaaiEdaaaa@43B5@

1.099

-5.023

24.2 σ C o <26.0 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGOmaiaaisdaca GGUaGaaGOmaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaikdacaaI2aGaaiOlaiaaicdaaaa@43AB@

0.849

-0.203

15.7 σ C o <16.2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGymaiaaiwdaca GGUaGaaG4naiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaakiabgYda8iaaigdacaaI2aGaaiOlaiaaikdaaaa@43B2@

0.914

-2.146

26.2 σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGOmaiaaiAdaca GGUaGaaGOmaiabgsMiJkabeo8aZnaaDaaaleaacaWGdbaabaGaam4B aaaaaaa@3FB7@

0.099

19.334

Table 1 Yang5 subsection coefficient of her standard relationship

coefficients

value

a

23.7591600170160e-006

b

-2.76710569836364e-003

c

132.238924476659e-003

d

-3.31438816243354

e

45.8713603676501

f

-330.723722504547

g

975.195895449145

Table 2 Jiang et al.,6 coefficients

standard deviation

σ C o [12,26] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadoeaaeaacaWGVbaaaOGaeyicI4Saai4waiaaigdacaaIYaGa aiilaiaaikdacaaI2aGaaiyxaaaa@4209@ /dB

σ C o [12,15) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadoeaaeaacaWGVbaaaOGaeyicI4Saai4waiaaigdacaaIYaGa aiilaiaaigdacaaI1aGaaiykaaaa@41D3@ /dB

σ C o [15,20) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadoeaaeaacaWGVbaaaOGaeyicI4Saai4waiaaigdacaaI1aGa aiilaiaaikdacaaIWaGaaiykaaaa@41D2@ /dB

σ C o [20,23] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadoeaaeaacaWGVbaaaOGaeyicI4Saai4waiaaikdacaaIWaGa aiilaiaaikdacaaIZaGaaiyxaaaa@4205@ /dB

Jiang et al.,6

0.0543

0.0606

0.0602

0.0384

Yang5

0.1896

0.0273

0.086

0.2634

Quartly et al.,1

0.3124

0.439

0.1827

0.3843

Table 3 Standard deviation of the three standard relationships

Adjustment of the backscatter coefficient statistical model

This section will discuss the shortcomings of the statistical relationship in Jiang et al.,6 and advance the adjusted methods.

The statistical scatter diagram of Jason-1 radar altimeter from cycle 1 to cycle 279 is shown in Figure 1. The samples selected criterion is no rain, open sea, no sea ice and small signal deviation angle. Because the accuracy of backscatter coefficient values of Jason-1's GDR (Geophysical Data Records) is 0.01dB, the scatter points are drawn every 0.01dB during statistics.

Figure 1 The σ C o MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcLbsaqaaaaaaaaa Wdbiabeo8aZPWdamaaDaaaleaajugWa8qacaWGdbaal8aabaqcLbma peGaam4Baaaaaaa@3E77@ and σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baaaa aaa@3C79@ statistical scatter diagram of Jason-1 radar altimeter from cycle 1 to cycle 279.

The scatter points are relatively concentrated when, σ C o [ 12,26) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaigdacaaIYaGaaiilaiaaikdacaaI2aGaai ykaaGaay5waaaaaa@426E@ and the correlation of Ku band and C band backscatter coefficient is obvious. But the scatter points are relatively divergent when σ C o <12 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyip aWJaaGymaiaaikdaaaa@3DFB@ dB and σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ > 26 dB, this is the reason that Jiang et al.,6 adopted the range of σ C o [ 12,26) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaigdacaaIYaGaaiilaiaaikdacaaI2aGaai ykaaGaay5waaaaaa@426E@ .

Some samples of sea surface wind speed value corresponding to Ku band backscatter coefficients using the method of Jiang et al.,11 are listed in Table 4.

When the significant wave height is 1m and σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baaaa aaa@3C78@ =23.3dB, the calculated wind speed value is 0.0084 m/s. Since the higher the backscatter coefficient of radar altimeter is, the smaller the corresponding wind speed value is, so the condition of σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ > 26 dB will not be considered. According to equation (4), when σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ =12dB,  σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baaaa aaa@3C78@ =9.0800dB, the corresponding wind speed value is 27.3683m/s, that is to say, when the wind speed calculated by radar altimeter is greater than 27.3683m/s, σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ should be less than 12dB. High wind speed and severe sea situation often cause tremendous disasters, so it is necessary to research the statistical model when σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ <12 dB. The Ku band and C band statistical model of equation (4) in the range of σ C o [ 8,32] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaiIdacaGGSaGaaG4maiaaikdacaGGDbaaca GLBbaaaaa@41EA@ is shown in Figure 2. When σ C o [ 8,12] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaiIdacaGGSaGaaGymaiaaikdacaGGDbaaca GLBbaaaaa@41E8@ , it means that σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baaaa aaa@3C78@ decreases if σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ increases which violates the specular scattering theory of radar altimeter. This paper adopts the statistical model of Yang5 in the range of σ C o [ 8,12) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaiIdacaGGSaGaaGymaiaaikdacaGGPaaaca GLBbaaaaa@41B4@ (The dotted line in figure 2).  The reason is that the accuracy of Yang5 is the highest when σ C o [ 8,12) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaiIdacaGGSaGaaGymaiaaikdacaGGPaaaca GLBbaaaaa@41B4@ in Table 3 which meets the specular scattering theory.

That is, Yang5 is adopted when σ C o [ 8,12) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaiIdacaGGSaGaaGymaiaaikdacaGGPaaaca GLBbaaaaa@41B4@ , while Jiang et al.,6 is adopted when   σ C o [ 12,26) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca qGGcGaeq4Wdm3damaaDaaaleaapeGaam4qaaWdaeaapeGaam4Baaaa kiabgIGiopaadeaapaqaa8qacaaIXaGaaGOmaiaacYcacaaIYaGaaG OnaiaacMcaaiaawUfaaaaa@4391@ .

σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0baaS qaaiaadUeacaWG1baabaGaam4Baaaaaaa@3C1A@ /dB

Wind speed/ m s -1 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeyBaiabgwSixl aabohadaahaaWcbeqaaiaab2cacaqGXaaaaaaa@3D2D@

Significant wave height /m

23.300

0.0084

1

10.2313

20

——

9.0800

27.3683

——

8.6688

30

——

7.1063

40

——

5.5438

50

——

Table 4 The correspondence of sea surface wind speed and significant wave height with σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baaaa aaa@3C78@

Figure 2 The backscatter coefficient statistical model in the range of σ C o [ 8,32) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qaca qGdpWdamaaDaaaleaapeGaae4qaaWdaeaapeGaae4BaaaakiabgIGi opaadeaapaqaa8qacaaI4aGaaiilaiaaiodacaaIYaGaaiykaaGaay 5waaaaaa@4139@ .

Conclusions

The backscatter coefficient statistical model plays an important role in the sea surface wind speed retrieval using dual frequency altimeter. This paper suggests an adjustment of low subsection backscatter coefficient statistical relationship, that is, Yang5 is adopted when σ C o [ 8,15) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaiIdacaGGSaGaaGymaiaaiwdacaGGPaaaca GLBbaaaaa@41B7@ , while Jiang et al.,6 is adopted when σ C o [ 15,26) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaOGaeyic I48aamqaa8aabaWdbiaaigdacaaI1aGaaiilaiaaikdacaaI2aGaai ykaaGaay5waaaaaa@4271@ . The adjustment will improve the accuracy of the statistical model, and have a positive affect for high wind speed retrieval. Work in this paper and Jiang et al.,6 only consider the statistical relationship between σ C o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGdbaapaqaa8qacaWGVbaaaaaa@3B76@ and σ Ku o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqkY=MjY=Pj0xh9v8qiW7rqqrFfpeea0xe9Lq=Jc9vqaq pepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=x b9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaaeaaaaaaaaa8qacq aHdpWCpaWaa0baaSqaa8qacaWGlbGaamyDaaWdaeaapeGaam4Baaaa aaa@3C78@ without any physical mechanism research, and is short of in situ data verification. Further work will consider these aspects.

Funding details

Project Supported by Foundation of State Key Laboratory of Geo-information Engineering (SKLGIE2018-ZZ-8), the Postdoctoral Science Foundation of China(2017M610971).

Acknowledgments

None.

Conflicts of interest

Authors declare that there is no conflict of interest.

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