Optical Properties and Phase of Some Midlatitude, Midlevel Clouds in ECLIPS

S. A. Young CSIRO Atmospheric Research, Aspendale, Victoria, Australia

Search for other papers by S. A. Young in
Current site
Google Scholar
PubMed
Close
,
C. M. R. Platt CSIRO Atmospheric Research, Aspendale, Victoria, Australia

Search for other papers by C. M. R. Platt in
Current site
Google Scholar
PubMed
Close
,
R. T. Austin CSIRO Atmospheric Research, Aspendale, Victoria, Australia

Search for other papers by R. T. Austin in
Current site
Google Scholar
PubMed
Close
, and
G. R. Patterson CSIRO Atmospheric Research, Aspendale, Victoria, Australia

Search for other papers by G. R. Patterson in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

Several cloud optical quantities were measured for the first time in midlevel, mixed-phase clouds. These included cloud infrared emittance and absorption coefficient (10–12 μm), effective backscatter-to-extinction ratio, and lidar depolarization ratio. Contrary to expectations, the supercooled water clouds were not always optically thick and therefore had measurable infrared absorption coefficients. At times, the water clouds had quite low emittances, whereas ice clouds had emittances that sometimes approached unity. On average, the cloud emittances were greater than those measured previously at lower temperatures in cirrus, but with considerable variability. At higher temperatures, the emittance values were skewed toward unity. The infrared absorption coefficients, for the semitransparent cases, showed a similar trend. The effective isotropic backscatter-to-extinction ratio was also measured. When separated into temperature intervals, the ratio was surprisingly constant, with mean values lying between 0.42 and 0.43, but with considerable variation. These ratios were most variable (0.15–0.8) in the −20° to −10°C temperature range where various ice crystal habits can occur. When multiple scattering effects were allowed for, values of backscatter-to-extinction ratio in the supercooled water clouds agreed well with theory. Multiple scattering factors based on previously obtained theoretical values were used and, thus, validated.

Characteristic and well-known patterns of lidar backscatter coefficient and depolarization ratio were used to separate out the incidence of supercooled water and ice layers and to identify layers of horizontal planar hexagonal crystals. This approach allowed the most detailed examination yet of such incidence by ground-based remote sensing. Water was detected for 92% of the time for the temperature interval of −5° to 0°C. Between −20° and −5°C, percentages varied between 33% and 56%, dropping to 21% between −25° and −20°C and to zero below −25°C. Oriented hexagonal plate crystals were present for 20% of the total time in ice layers between −20° and −10°C, the region of their maximum growth. The depolarization ratio varied significantly among different ice fall streaks, indicating considerable variation in ice crystal habit. Although the dependence of depolarization ratio on optical depth had been predicted theoretically, the first experimental validation in terms of IR emittance was obtained in this study.

* Current affiliation: Department of Atmospheric Science, Colorado State University, Fort Collins, Colorado.

* Corresponding author address: Dr. Stuart A. Young, CSIRO Atmospheric Research, PMB 1, Aspendale, VIC 3195, Australia.

Abstract

Several cloud optical quantities were measured for the first time in midlevel, mixed-phase clouds. These included cloud infrared emittance and absorption coefficient (10–12 μm), effective backscatter-to-extinction ratio, and lidar depolarization ratio. Contrary to expectations, the supercooled water clouds were not always optically thick and therefore had measurable infrared absorption coefficients. At times, the water clouds had quite low emittances, whereas ice clouds had emittances that sometimes approached unity. On average, the cloud emittances were greater than those measured previously at lower temperatures in cirrus, but with considerable variability. At higher temperatures, the emittance values were skewed toward unity. The infrared absorption coefficients, for the semitransparent cases, showed a similar trend. The effective isotropic backscatter-to-extinction ratio was also measured. When separated into temperature intervals, the ratio was surprisingly constant, with mean values lying between 0.42 and 0.43, but with considerable variation. These ratios were most variable (0.15–0.8) in the −20° to −10°C temperature range where various ice crystal habits can occur. When multiple scattering effects were allowed for, values of backscatter-to-extinction ratio in the supercooled water clouds agreed well with theory. Multiple scattering factors based on previously obtained theoretical values were used and, thus, validated.

Characteristic and well-known patterns of lidar backscatter coefficient and depolarization ratio were used to separate out the incidence of supercooled water and ice layers and to identify layers of horizontal planar hexagonal crystals. This approach allowed the most detailed examination yet of such incidence by ground-based remote sensing. Water was detected for 92% of the time for the temperature interval of −5° to 0°C. Between −20° and −5°C, percentages varied between 33% and 56%, dropping to 21% between −25° and −20°C and to zero below −25°C. Oriented hexagonal plate crystals were present for 20% of the total time in ice layers between −20° and −10°C, the region of their maximum growth. The depolarization ratio varied significantly among different ice fall streaks, indicating considerable variation in ice crystal habit. Although the dependence of depolarization ratio on optical depth had been predicted theoretically, the first experimental validation in terms of IR emittance was obtained in this study.

* Current affiliation: Department of Atmospheric Science, Colorado State University, Fort Collins, Colorado.

* Corresponding author address: Dr. Stuart A. Young, CSIRO Atmospheric Research, PMB 1, Aspendale, VIC 3195, Australia.

Save
  • Allen, R. J., and C. M. R. Platt, 1977: Lidar for multiple backscattering and depolarization observations. Appl. Opt.,16, 3193–3199.

  • Browning, K. A., 1994: Survey of perceived priority issues in the parametrizations of cloud-related processes in GCMs. Quart. J. Roy. Meteor. Soc.,120, 483–487.

  • Carswell, A. I., A. Fong, S. R. Pal, and I. Pribluda, 1995: Lidar-derived distribution of cloud vertical location and extent. J. Appl. Meteor.,34, 107–130.

  • Clough, S. A., F. X. Kneizys, and R. W. Davies, 1989: Line shape and the water vapour continuum. Atmos. Res.,23, 229–241.

  • Deirmendjian, D., 1969: Electromagnetic Scattering on Polydispersions. Elsevier, 292 pp.

  • Del Guasta, M., M. Morandi, L. Stefanutti, J. Brechet, and J. Piquad, 1993: One year of cloud lidar data from Dumont d’Urville (Antarctica) 1. General overview of geometric and optical properties. J. Geophys. Res.,98, 18 575–18 587.

  • Derr, V. E., N. L. Abshire, R. E. Cupp, and G. T. McNice, 1976: Depolarization of lidar returns from virga and source cloud. J. Appl. Meteor.,15, 1300–1303.

  • Heymsfield, A. J., and L. M. Miloshevich, 1993: Homogeneous ice nucleation and supercooled water in orographic wave clouds. J. Atmos. Sci.,50, 2335–2353.

  • Heymsfield, A. J., L. M. Miloshevich, A. Slingo, K. Sassen, and D. O’C. Starr, 1991: An observational and theoretical study of highly supercooled altocumulus. J. Atmos. Sci.,48, 923–945.

  • King, W. D., 1982: Location and extent of supercooled water regions in deep stratiform cloud in western Victoria. Aust. Meteor. Mag.,30, 81–88.

  • Le Treut, H., Z. X. Li, and M. Forichon, 1994: Sensitivity of the LMD general circulation model to greenhouse forcing associated with two different cloud water parameterizations. J. Climate,7, 1827–1841.

  • Miller, T. L., and K. C. Young, 1979: A numerical simulation of ice crystal growth from the vapor phase. J. Atmos. Sci.,36, 458–469.

  • Mossop, S. C., A. Ono, and E. R. Wishart, 1970: Ice particles in maritime clouds near Tasmania. Quart. J. Roy. Meteor. Soc.,96, 487–508.

  • Pal, S. R., and A. I. Carswell, 1977: The polarization characteristics of lidar scattering from snow and ice crystals in the atmosphere. J. Appl. Meteor.,16, 70–80.

  • Pal, S. R., A. I. Carswell, I. Gordon, and A. Fong, 1995: Lidar-derived optical properties obtained during the ECLIPS program. J. Appl. Meteor.,34, 107–120.

  • Paltridge, G. W., and C. M. R. Platt, 1981: Aircraft measurements of solar and infrared radiation and the microphysics of cirrus cloud. Quart. J. Roy. Meteor. Soc.,107, 367–380.

  • Paltridge, G. W., W. J. King, and C. M. R. Platt, 1986: A case study of ice particle growth in a mixed-phase altostratus cloud. Aust. Meteor. Mag.,34, 149–154.

  • Platt, C. M. R., 1971: A narrow-beam radiometer for atmospheric radiation studies. J. Appl. Meteor.,10, 1307–1313.

  • Platt, C. M. R., 1977: Lidar observations of a mixed-phase altostratus cloud. J. Appl. Meteor.,16, 339–345.

  • Platt, C. M. R., 1978: Lidar backscatter from horizontal ice crystal plates. J. Appl. Meteor.,17, 482–488.

  • Platt, C. M. R., 1979: Remote sounding of high clouds. I: Calculation of visible and infrared optical properties from lidar and radiometer measurements. J. Appl. Meteor.,18, 1130–1143.

  • Platt, C. M. R., 1981: Remote sounding of high clouds. III: Monte Carlo calculations of multiple-scattered lidar returns. J. Atmos. Sci.,38, 156–167.

  • Platt, C. M. R., and D. J. Gambling, 1971: Emissivity of high layer clouds by combined lidar and radiometric techniques. Quart. J. Roy. Meteor. Soc.,97, 322–325.

  • Platt, C. M. R., and K. Bartusek, 1974: Structure and optical properties of middle-level clouds. J. Atmos. Sci.,31, 1079–1088.

  • Platt, C. M. R., and A. C. Dilley, 1981: Remote sensing of high clouds. IV: Observed temperature variations in cirrus optical properties. J. Atmos. Sci.,38, 1069–1082.

  • Platt, C. M. R., N. L. Abshire, and G. T. McNice, 1978: Some microphysical properties of an ice cloud from lidar observation of horizontally oriented crystals. J. Appl. Meteor.,17, 1320–1324.

  • Platt, C. M. R., J. C. Scott, and A. C. Dilley, 1987: Remote sounding of high clouds. VI: Optical properties of midlatitude and tropical cirrus. J. Atmos. Sci.,44, 729–747.

  • Platt, C. M. R., and Coauthors, 1994: The Experimental Cloud Lidar Pilot Study (ECLIPS) for cloud-radiation research. Bull. Amer. Meteor. Soc.,75, 1635–1654.

  • Platt, C. M. R., S. A. Young, P. J. Manson, G. R. Patterson, S. C. Marsden, R. T. Austin, and J. H. Churnside, 1998: The optical properties of equatorial cirrus from observations in the ARM Pilot Radiation Observation Experiment. J. Atmos. Sci.,55, 1977–1996.

  • Popov, A. A., and O. V. Schefer, 1994: Theoretical and numerical investigations of the intensity of the lidar signal specular reflected from a set of oriented ice plates. Appl. Opt.,75, 7038–7044.

  • Rauber, R. M., and A. Tokay, 1991: An explanation of the existence of supercooled water at the top of cold clouds. J. Atmos. Sci.,48, 1005–1023.

  • Ryan, B. F., E. R. Wishart, and D. E. Shaw, 1976: The growth rates and densities of ice cystals between −3° and −21°C. J. Atmos. Sci.,33, 842–850.

  • Ryan, B. F., W. D. King, and S. C. Mossop, 1985: The frontal transition zone and microphysical properties of associated clouds. Quart. J. Roy. Meteor. Soc.,111, 479–493.

  • Sassen, K., 1976: Polarization diversity lidar returns from virga and precipitation: Anomalies and the bright band analogy. J. Appl. Meteor.,15, 292–300.

  • Sassen, K., 1978: Air-truth polarization studies of orographic clouds. J. Appl. Meteor.,17, 73–91.

  • Sassen, K., 1980: Remote sensing of planar ice crystal fall attitudes. J. Meteor. Soc. Japan,58, 422–429.

  • Sassen, K., 1984: Deep orographic cloud structure and composition derived from comprehensive remote sensing measurements. J. Climate Appl. Meteor.,23, 568–583.

  • Sassen, K., and B. S. Cho, 1992: Subvisual–thin cirrus lidar dataset for satellite verification and climatological research. J. Appl. Meteor.,31, 1275–1286.

  • Sassen, K., H. Zhao, and G. C. Dodd, 1992: Simulated polarization diversity lidar returns from water and precipitating mixed phase clouds. Appl. Opt.,31, 2914–2923.

  • Schotland, R. M., K. Sassen, and R. Stone, 1971: Observations by lidar of linear depolarization ratios for hydrometeors. J. Appl. Meteor.,10, 1011–1017.

  • Stokes, G. M., and S. E. Schwartz, 1994: The Atmospheric Radiation Measurement (ARM) program: Programmatic background and design of the Cloud and Radiation Test bed. Bull. Amer. Meteor. Soc.,75, 1201–1221.

  • Winker, D. M., and M. A. Vaughan, 1994: Vertical distribution of clouds over Hampton, Virginia, observed by lidar under the ECLIPS and FIRE ETO programs. Atmos. Res.,34, 117–133.

  • Young, S. A., 1995: Analysis of lidar backscatter profiles in optically thin clouds. Appl. Opt.,34, 7019–7031.

All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 247 71 6
PDF Downloads 50 13 2