Ma Xiumei, Lee Wenchau, Zhao Kun, et al. Optimization of nonlinear VAD method in the low-level wind retrieval. J Appl Meteor Sci, 2014, 25(3): 321-329.
Citation: Ma Xiumei, Lee Wenchau, Zhao Kun, et al. Optimization of nonlinear VAD method in the low-level wind retrieval. J Appl Meteor Sci, 2014, 25(3): 321-329.

Optimization of Nonlinear VAD Method in the Low-level Wind Retrieval

  • Received Date: 2013-07-04
  • Rev Recd Date: 2014-01-10
  • Publish Date: 2014-05-31
  • The performance of nonlinear velocity azimuth display method in the vertical wind profile retrieval at low levels (below 2 km) is quantitatively examined by combing the theoretical analysis and cases observed by SoWMEX S-Pol radar and Yangjiang radar in Guangdong Province. Results show that the general structure and evolution of the low-level wind profile can be reasonably deduced by traditional nonlinear VAD method. The root mean square error can be used to evaluate orders of velocity azimuth display (VAD) fitting, but small error does not always mean the better performance especially with big continuous data absence, and a specific example is given. When setting the VAD fitting order to 3 instead of 2, coefficients which represent the horizontal wind u and v are closer to the wind derived from radial velocity image. However, when the fitting order comes to 4, coefficients lost their physical meaning. The wind direction differs a lot and the speed is much smaller than the value before. At the same time, the root mean square error decreases compared with the order of 3. Besides, data used in nonlinear VAD fitting come from the whole volume, which decreases quite a lot and leads to nonlinear VAD fitting error when the volume coverage pattern (VCP) only has some lower elevations (e.g., two elevations). Therefore, the retrieved wind could contain large error in certain situations, such as for a region with large continuous data absence or a volume scan with fewer elevations.After carefully evaluating the impact of the corresponding parameters on the nonlinear VAD retrievals by analyzing radar measurements, a modified nonlinear VAD method is proposed which takes account of the maximum fitting order in horizontal (VAD) and vertical adaptively according to the size of continuous data absence and the number of sweeps in a volume scan. VAD fitting is abandoned when the data absence is larger than 90°; the order is set to 3 when the data absence is between 60° and 90°; and the order is set to 4 when the data absence is smaller than 60°. The order of nonlinear VAD fitting is reduced when the VCP only has low elevations. Apply the method in two cases: One is a front case passing through Taiwan, China, the other is a typhoon case landfall in Guangdong Province, with both of them having nonlinearity in the low level wind profile. The wind profile after adjusted can significantly improve the wind retrieval, as compared with the traditional nonlinear VAD. Both wind speed and direction from modified nonlinear VAD agree with those from sounding observations, with the root mean square of the wind less than 2 m·s-1, which is obviously better than nonlinear VAD before adjusted.
  • Fig. 1  The distribution of radar and sounding stations in this study

    (the maximum Doppler range of 150 km, the shaded shows the terrain height)

    Fig. 2  The vertical wind profile retrieved by nonlinear VAD of S-Pol radar from 0000 UTC to 2352 UTC on 2 June 2008(a) without considering data absence, the order in z is 3, (b) considering data absence, the order in z is 3, (c) considering data absence, the order in z is 2

    (* indicates the VCP1 scan mode, the others are VCP2 scan mode)

    Fig. 3  The low-level wind profile retrived from VAD and nonliner VAD at 1500 UTC 2 June 2008 as compared with the GPS observeraion of Pingdong Station

    Fig. 4  Nonlinear VAD wind profile of Yangjiang radar from 0100 UTC to 2400 UTC on 23 July 2012 (a) without considering data absence, order in z is 3, (b) considering data absence, order in z is 3

    Fig. 5  The low-level wind profile retrived from VAD and nonliner VAD at 1100 UTC 23 July 2012 as compared with the GTS observeraion of Yangjiang

    Table  1  The Fourier coefficients and the aprroximation error for the VAD with the different numer of harmonics

    谐波系数 a0 a1 b1 a2 b2 a3 b3 a4 b4 均方根误差/(m·s-1)
    二阶 -0.8 8.3 2.3 -0.3 0.0 2.19
    三阶 -1.6 7.2 0.9 -2.0 0.6 -0.3 2.2 1.92
    四阶 -5.2* 0.6* 0.3* -3.1 5.6* 2.7* 3.1 0.5 -1.5 1.87
    注:*表示拟合系数明显与实际联系的物理量大小不符。
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    Table  2  Nonlinear VAD coefficients for u and v with elevation of 0.5° and 1.5° at 0000 UTC 2 June 2008

    系数 1 z z2 z3 r2 r2z 均方根误差/(m·s-1)
    二阶u -2.2 11.6 -11.5 -0.001 0.004 1.32
    二阶v 0.4 -1.5 3.3 0.0006 -0.001 1.12
    三阶u -2.6 13.4 -24.2 44.0 0.006 -0.024 1.31
    三阶v 0.09 0.09 -7.7 38.1 0.007 -0.026 1.11
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    • Received : 2013-07-04
    • Accepted : 2014-01-10
    • Published : 2014-05-31

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