Optical and Geometrical Properties of Cirrus Clouds over the Tibetan Plateau Measured by LiDAR and Radiosonde Sounding during the Summertime in 2014

Optical and geometrical characteristics of the cirrus clouds over Naqu (4508 m a.s.l., 31.48◦ N, 92.06◦ E), in the Tibetan Plateau were determined from LiDAR and radiosonde measurements performed during the third TIbetan Plateau EXperiment of atmospheric sciences (TIPEX III) campaign from July to August 2014. For the analysis of the temperature dependence, the simultaneous observations with LiDAR and radiosonde were conducted. Cirrus clouds were generally observed ranging from 5.2 km to 12 km above ground level (AGL) (i.e., 9.7 km to 16.5 km a.s.l.), with the midcloud temperatures ranging from −79.7 to −26.0 ◦C. The cloud thickness generally differed from 0.12 to 2.55 km with a mean thickness of 1.22 ± 0.70 km, and 85.7% of the measurement cases had thickness smaller than 1.5 km. The retrievals of linear particle depolarization ratio, extinction coefficient, and optical depth of cirrus clouds were provided. Moreover, the multiple scattering effect inside of cirrus clouds was corrected. The linear particle depolarization ratio of the cirrus clouds varied from 0.36 to 0.52, with a mean value of 0.44 ± 0.04. The optical depth of the cirrus clouds was between 0.01 and 3 following the scheme of Fernald-Klett method. Sub-visual, thin, and opaque cirrus clouds were observed at 4.76%, 61.90% and 33.34% of the measured cases, respectively. The temperature and thickness dependencies of the optical properties were studied in detail. A maximum cirrus thickness of around 2 km was found at temperatures between −60 and −50 ◦C. This study shows that the mean extinction coefficient of the cirrus clouds increases with the increase of temperature. Conversely, the measurements indicate that the linear particle depolarization ratio decreases with the increasing temperature. The relationships between the existence of cirrus clouds and the temperature anomaly (temperature difference from the mean value of the temperature during July and August 2014 over Naqu) and deep convective activity are also discussed. The formation of cirrus clouds is investigated and also its apparent relationship with the South Asia High Pressure, the dynamic processes of Rossby wave, and deep convective activity over the Tibetan Plateau. The outgoing longwave radiation of cirrus clouds is calculated with the Fu-Liou model and is shown to increases monotonously with the increase of optical depth.

[1]  A. Ansmann,et al.  Independent measurement of extinction and backscatter profiles in cirrus clouds by using a combined Raman elastic-backscatter lidar. , 1992, Applied optics.

[2]  David M. Winker,et al.  Vertical distribution of clouds over Hampton, Virginia observed by lidar under the ECLIPS and FIRE ETO programs , 1994 .

[3]  Guoxiong Wu,et al.  The effect of mechanical forcing on the formation of a mesoscale vortex , 2007 .

[4]  Holger Baars,et al.  Optical and geometrical properties of cirrus clouds in Amazonia derived from 1 year of ground-based lidar measurements , 2016 .

[5]  J. Nee,et al.  Lidar ratio and depolarization ratio for cirrus clouds. , 2002, Applied optics.

[6]  LI Chengcai,et al.  The Properties and Formation of Cirrus Clouds over the Tibetan Plateau Based on Summertime Lidar Measurements , 2013 .

[7]  Andrew J. Heymsfield,et al.  A Balloon-Borne Continuous Cloud Particle Replicator for Measuring Vertical Profiles of Cloud Microphysical Properties: Instrument Design, Performance, and Collection Efficiency Analysis , 1997 .

[8]  F. G. Fernald Analysis of atmospheric lidar observations: some comments. , 1984, Applied optics.

[9]  Dimitris Balis,et al.  Optical and geometrical characteristics of cirrus clouds over a Southern European lidar station , 2007 .

[10]  Songhua Wu,et al.  Lidar and Ceilometer Observations and Comparisons of Atmospheric Cloud Structure at Nagqu of Tibetan Plateau in 2014 Summer , 2017 .

[11]  Dengxin Hua,et al.  Mobile multi-wavelength polarization Raman lidar for water vapor, cloud and aerosol measurement. , 2015, Optics express.

[12]  Allan I. Carswell,et al.  Automated method for lidar determination of cloud-base height and vertical extent. , 1992, Applied optics.

[13]  Xiaoquan Song,et al.  Depolarization Ratio Profiles Calibration and Observations of Aerosol and Cloud in the Tibetan Plateau Based on Polarization Raman Lidar , 2018, Remote. Sens..

[14]  G. Tselioudis,et al.  Evidence of impact of aviation on cirrus cloud formation , 2003 .

[15]  A. C. Dilley,et al.  Remote Sounding of High Clouds. Part VI: Optical Properties of Midlatitude and Tropical Cirrus , 1987 .

[16]  Xiaoquan Song,et al.  Observations of water vapor mixing ratio profile and flux in the Tibetan Plateau based on the lidar technique , 2016 .

[17]  Optical and geometrical properties of northern midlatitude cirrus clouds observed with a UV Raman lidar , 1999 .

[18]  K. Sassen,et al.  Cirrus Cloud Microphysical Property Retrieval Using Lidar and Radar Measurements. Part II: Midlatitude Cirrus Microphysical and Radiative Properties , 2002 .

[19]  V. Freudenthaler,et al.  Depolarization ratio profiling at several wavelengths in pure Saharan dust during SAMUM 2006 , 2009 .

[20]  P. Flamant,et al.  Iterative method to determine an averaged backscatter-to-extinction ratio in cirrus clouds. , 1996, Applied optics.

[21]  R. Hogan,et al.  Fast approximate calculation of multiply scattered lidar returns. , 2006, Applied optics.

[22]  M. Kraemer A Microphysics Guide to Cirrus Clouds , 2014 .

[23]  Q. Fu,et al.  Parameterization of the Radiative Properties of Cirrus Clouds , 1993 .

[24]  J. Iaquinta,et al.  Cirrus Crystal Terminal Velocities , 2000 .

[25]  D. Fahey,et al.  Aviation-Produced Aerosols and Cloudiness , 1999 .

[26]  W. Paul Menzel,et al.  Global characterization of cirrus clouds using CALIPSO data , 2008 .

[27]  J. Houghton,et al.  Climate Change 2013 - The Physical Science Basis: Working Group I Contribution to the Fifth Assessment Report of the Intergovernmental Panel on Climate Change , 2014 .

[28]  K. Sassen,et al.  A Midlatitude Cirrus Cloud Climatology from the Facility for Atmospheric Remote Sensing. Part I: Macrophysical and Synoptic Properties , 2001 .

[29]  Albert Ansmann,et al.  Cirrus optical properties observed with lidar, radiosonde, and satellite over the tropical Indian Ocean during the aerosol‐polluted northeast and clean maritime southwest monsoon , 2007 .

[30]  P. Seifert,et al.  Climatological and radiative properties of midlatitude cirrus clouds derived by automatic evaluation of lidar measurements , 2016 .

[31]  Peter J. Webster,et al.  Clouds and Climate: Sensitivity of Simple Systems. , 1981 .

[32]  Peter J. Webster,et al.  The role of hydrological processes in ocean‐atmosphere interactions , 1994 .

[33]  K. Parameswaran,et al.  Temperature dependence of tropical cirrus properties and radiative effects , 2005 .

[34]  Jennifer M. Comstock,et al.  Retrieval of Cirrus Cloud Radiative and Backscattering Properties Using Combined Lidar and Infrared Radiometer (LIRAD) Measurements , 2001 .

[35]  U. Wandinger,et al.  Multiple-Scattering Influence on Extinction-and Backscatter-Coefficient Measurements with Raman and High-Spectral-Resolution Lidars. , 1998, Applied optics.

[36]  Alain Hauchecorne,et al.  Cirrus climatological results from lidar measurements at OHP (44°N, 6°E) , 2001 .

[37]  Atusi Numaguti,et al.  Diurnal Variation of Water Vapor over the Central Tibetan Plateau during Summer. , 2001 .

[38]  Albert Ansmann,et al.  Portable Raman Lidar Polly XT for Automated Profiling of Aerosol Backscatter, Extinction, and Depolarization , 2009 .

[39]  Arnaud Delaval,et al.  Classification of particle effective shape ratios in cirrus clouds based on the lidar depolarization ratio. , 2002, Applied optics.

[40]  V. Freudenthaler,et al.  Characterization of Saharan dust, marine aerosols and mixtures of biomass-burning aerosols and dust by means of multi-wavelength depolarization and Raman lidar measurements during SAMUM 2 , 2011 .

[41]  Kenneth Sassen,et al.  Subvisual-Thin Cirrus Lidar Dataset for Satellite Verification and Climatological Research , 1992 .

[42]  K. Gage,et al.  An Objective Method for the Determination of Tropopause Height from VHF Radar Observations , 1982 .

[43]  K. Sassen The Polarization Lidar Technique for Cloud Research: A Review and Current Assessment , 1991 .

[44]  Kenneth Sassen,et al.  A Midlatitude Cirrus Cloud Climatology from the Facility for Atmospheric Remote Sensing. Part II: Microphysical Properties Derived from Lidar Depolarization , 2001 .

[45]  Harshvardhan,et al.  Temperature dependence of cirrus extinction - Implications for climate feedback , 1988 .

[46]  A. Macke,et al.  Single Scattering Properties of Atmospheric Ice Crystals , 1996 .

[47]  J. Comstock,et al.  Ground‐based lidar and radar remote sensing of tropical cirrus clouds at Nauru Island: Cloud statistics and radiative impacts , 2002 .

[48]  H. Chepfer,et al.  Impact of cirrus cloud ice crystal shape and size on multiple scattering effects: Application to spaceborne and airborne backscatter lidar measurements during LITE Mission and E LITE Campaign , 1999 .