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6 期                     张  翔等:黄土高原典型塬区边界层高度反演方法对比研究                                        1641
               演效果最好, 与位温廓线反演结果的相关性为                                tion of atmospheric boundary layer height using ceilometer back‐
               0. 56, 平均绝对偏差约为406 m。                                scatter  data  assisted  by  a  boundary  layer  model[J]. Quarterly
                                                                    Journal  of  the  Royal  Meteorological  Society,  138(664):  649-
                  (3)  混合算法反演结果与云高仪内部算法得
                                                                    663. DOI: 10. 1002/qj. 964.
               到的小时平均边界层高度以及位温廓线反演结果
                                                                 Emeis S, Münkel C, Vogt S, et al, 2004. Atmospheric boundary-lay‐
               均有良好的一致性, 能够较为准确地反映边界层高                              er  structure  from  simultaneous  SODAR,  RASS,  and  ceilometer
               度的日变化特征。总体上, 基于后向散射反演的边                              measurements[J]. Atmospheric Environment, 38(2): 273-286.
               界层高度高于基于位温廓线的结果, 即物质边界层                              DOI: 10. 1016/j. atmosenv. 2003. 09. 054.
                                                                 Emeis  S,  Schäfer  K,  2006. Remote  sensing  methods  to  investigate
               高于热力边界层。
                                                                    boundary-layer  structures  relevant  to  air  pollution  in  cities[J].
                   本研究分析了使用云高仪后向散射廓线, 结合
                                                                    Boundary-Layer  Meteorology,  121(2):  377-385. DOI:  10.
               混合算法反演平凉地区大气边界层高度的有效性,                               1007/s10546-006-9068-2.
               可为我国黄土塬区天气、 气候和大气物质与能量传                           Emeis S, Schäfer K, Münkel C, 2008. Surface-based remote sensing
               输过程等的研究提供边界层高度等基础数据的补                                of  the  mixing-layer  height  a  review [J]. Meteorologische
                                                                    Zeitschrift,  17(5):  621-630. DOI:  10. 1127/0941-2948/2008/
               充方案。当对边界层高度序列的连性及时间分辨
                                                                    0312.
               率要求较高时, 可采用本研究给出的混合算法反演
                                                                 Eresmaa N, Karppinen A, Joffre S M, et al, 2006. Mixing height de‐
               结果进行补充, 但使用中需对雨后晴天或连续晴天                              termination by ceilometer[J]. Atmospheric Chemistry and Phys‐
               大气较为干净时(即气溶胶含量低), 以及夜间或早                             ics, 6: 1485-1493. DOI: 10. 5194/acp-6-1485-2006.
               晨存在高空气溶胶层时的反演结果进行订正。由                             Flamant C, Pelon J, Flamant P H, et al, 1997. Lidar determination of
                                                                    the entrainment zone thickness at the top of the unstable marine at‐
               于探空数据时间分辨率的限制, 未对混合算法在早
                                                                    mospheric boundary layer[J]. Boundary-Layer Meteorology, 83
               晚过渡期和正午快速增长期的反演性能进行验证。
                                                                    (2): 247-284. DOI: 10. 1023/A: 1000258318944.
               未来研究中还需结合其他观测手段, 如激光测风雷                           Flentje H, Claude H, Elste T, et al, 2010. The Eyjafjallajökull erup‐
               达、 微波辐射计等, 联合反演大气边界层高度, 提                            tion in April 2010-detection of volcanic plume using in-situ mea‐
               供更为完善准确的边界层高度数据。                                     surements, ozone sondes and Lidar-ceilometer profiles[J]. Atmo‐
                                                                    spheric  Chemistry  and  Physics,  10(20):  10085-10092. DOI:
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