Noise filtering of rotational Raman lidar using threshold amendment for atmospheric temperature measurement

2009 ◽  
Author(s):  
Weiguo Kong ◽  
Siying Chen ◽  
Yinchao Zhang ◽  
Tian Lan ◽  
Zongjia Qiu ◽  
...  
2011 ◽  
Vol 48 (2) ◽  
pp. 022801
Author(s):  
孔卫国 Kong Weiguo ◽  
陈思颖 Chen Siying ◽  
张寅超 Zhang Yinchao ◽  
陈和 Chen He ◽  
邱宗甲 Qiu Zongjia ◽  
...  

2014 ◽  
Vol 14 (21) ◽  
pp. 29019-29055 ◽  
Author(s):  
A. Behrendt ◽  
V. Wulfmeyer ◽  
E. Hammann ◽  
S. K. Muppa ◽  
S. Pal

Abstract. The rotational Raman lidar of the University of Hohenheim (UHOH) measures atmospheric temperature profiles during daytime with high resolution (10 s, 109 m). The data contain low noise errors even in daytime due to the use of strong UV laser light (355 nm, 10 W, 50 Hz) and a very efficient interference-filter-based polychromator. In this paper, we present the first profiling of the second- to forth-order moments of turbulent temperature fluctuations as well as of skewness and kurtosis in the convective boundary layer (CBL) including the interfacial layer (IL). The results demonstrate that the UHOH RRL resolves the vertical structure of these moments. The data set which is used for this case study was collected in western Germany (50°53'50.56′′ N, 6°27'50.39′′ E, 110 m a.s.l.) within one hour around local noon on 24 April 2013 during the Intensive Observations Period (IOP) 6 of the HD(CP)2 Observational Prototype Experiment (HOPE), which is embedded in the German project HD(CP)2 (High-Definition Clouds and Precipitation for advancing Climate Prediction). First, we investigated profiles of the noise variance and compared it with estimates of the statistical temperature measurement uncertainty Δ T based on Poisson statistics. The agreement confirms that photon count numbers obtained from extrapolated analog signal intensities provide a lower estimate of the statistical errors. The total statistical uncertainty of a 20 min temperature measurement is lower than 0.1 K up to 1050 m a.g.l. at noontime; even for single 10 s temperature profiles, it is smaller than 1 K up to 1000 m a.g.l.. Then we confirmed by autocovariance and spectral analyses of the atmospheric temperature fluctuations that a temporal resolution of 10 s was sufficient to resolve the turbulence down to the inertial subrange. This is also indicated by the profile of the integral scale of the temperature fluctuations, which was in the range of 40 to 120 s in the CBL. Analyzing then profiles of the second-, third-, and forth-order moments, we found the largest values of all moments in the IL around the mean top of the CBL which was located at 1230 m a.g.l. The maximum of the variance profile in the IL was 0.40 K2 with 0.06 and 0.08 K2 for the sampling error and noise error, respectively. The third-order moment was not significantly different from zero inside the CBL but showed a negative peak in the IL with a minimum of −0.72 K3 and values of 0.06 and 0.14 K3 for the sampling and noise errors, respectively. The forth-order moment and kurtosis values throughout the CBL were quasi-normal.


2001 ◽  
Author(s):  
Masahiro Funada ◽  
Chikao Nagasawa ◽  
Yasukuni Shibata ◽  
Makoto Abo

2015 ◽  
Vol 58 (4) ◽  
pp. 313-324 ◽  
Author(s):  
LI Ya-Juan ◽  
SONG Sha-Lei ◽  
LI Fa-Quan ◽  
CHENG Xue-Wu ◽  
CHEN Zhen-Wei ◽  
...  

1979 ◽  
Vol 18 (2) ◽  
pp. 225-227 ◽  
Author(s):  
R. Gill ◽  
K. Geller ◽  
J. Farina ◽  
J. Cooney ◽  
A. Cohen

1983 ◽  
Vol 22 (19) ◽  
pp. 2984 ◽  
Author(s):  
Yu. F. Arshinov ◽  
S. M. Bobrovnikov ◽  
V. E. Zuev ◽  
V. M. Mitev

2010 ◽  
Vol 22 (7) ◽  
pp. 1449-1452
Author(s):  
卜令兵 Bu Lingbing ◽  
郭劲秋 Guo Jinqiu ◽  
田力 Tian Li ◽  
黄兴友 Huang Xingyou ◽  
刘博 Liu Bo ◽  
...  

1990 ◽  
Vol 29 (34) ◽  
pp. 5182 ◽  
Author(s):  
Philippe Keckhut ◽  
M. L. Chanin ◽  
A. Hauchecorne

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