Particle Size Estimation in Ice-Phase Clouds Using Multifrequency Radar Reflectivity Measurements at 95, 33, and 2.8 GHz

Stephen M. Sekelsky Microwave Remote Sensing Laboratory, University of Massachusetts—Amherst, Amherst, Massachusetts

Search for other papers by Stephen M. Sekelsky in
Current site
Google Scholar
PubMed
Close
,
Warner L. Ecklund Cooperative Institute for Research in Environmental Sciences, University of Colorado, Boulder, Colorado

Search for other papers by Warner L. Ecklund in
Current site
Google Scholar
PubMed
Close
,
John M. Firda Microwave Remote Sensing Laboratory, University of Massachusetts—Amherst, Amherst, Massachusetts

Search for other papers by John M. Firda in
Current site
Google Scholar
PubMed
Close
,
Kenneth S. Gage NOAA Aeronomy Laboratory, Boulder, Colorado

Search for other papers by Kenneth S. Gage in
Current site
Google Scholar
PubMed
Close
, and
Robert E. McIntosh Microwave Remote Sensing Laboratory, University of Massachusetts—Amherst, Amherst, Massachusetts

Search for other papers by Robert E. McIntosh in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

Multifrequency radar measurements collected at 2.8 (S band), 33.12 (Ka band), and 94.92 GHz (W band) are processed using a neural network to estimate median particle size and peak number concentration in ice-phase clouds composed of dry crystals or aggregates. The model data used to train the neural network assume a gamma particle size distribution function and a size–density relationship having decreasing density with size. Results for the available frequency combinations show sensitivity to particle size for distributions with median volume diameters greater than approximately 0.2 mm.

Measurements are presented from the Maritime Continent Thunderstorm Experiment, which was held near Darwin, Australia, during November and December 1995. The University of Massachusetts—Amherst 33.12/94.92-GHz Cloud Profiling Radar System, the NOAA 2.8-GHz profiler, and other sensors were clustered near the village of Garden Point, Melville Island, where numerous convective storms were observed. Attenuation losses by the NOAA radar signal are small over the pathlengths considered so the cloud-top reflectivity values at 2.8 GHz are used to remove propagation path losses from the higher-frequency measurements. The 2.8-GHz measurements also permit estimation of larger particle diameters than is possible using only 33.12 and 94.92 GHz. The results suggest that the median particle size tends to decrease with height for stratiform cloud cases. However, this trend is not observed for convective cloud cases where measurements indicate that large particles can exist even near the cloud top.

Corresponding author address: Stephen M. Sekelsky, Dept. of Electrical and Computer Engineering, Knowles 209 C, University of Massachusetts, Amherst, MA 01003.

Abstract

Multifrequency radar measurements collected at 2.8 (S band), 33.12 (Ka band), and 94.92 GHz (W band) are processed using a neural network to estimate median particle size and peak number concentration in ice-phase clouds composed of dry crystals or aggregates. The model data used to train the neural network assume a gamma particle size distribution function and a size–density relationship having decreasing density with size. Results for the available frequency combinations show sensitivity to particle size for distributions with median volume diameters greater than approximately 0.2 mm.

Measurements are presented from the Maritime Continent Thunderstorm Experiment, which was held near Darwin, Australia, during November and December 1995. The University of Massachusetts—Amherst 33.12/94.92-GHz Cloud Profiling Radar System, the NOAA 2.8-GHz profiler, and other sensors were clustered near the village of Garden Point, Melville Island, where numerous convective storms were observed. Attenuation losses by the NOAA radar signal are small over the pathlengths considered so the cloud-top reflectivity values at 2.8 GHz are used to remove propagation path losses from the higher-frequency measurements. The 2.8-GHz measurements also permit estimation of larger particle diameters than is possible using only 33.12 and 94.92 GHz. The results suggest that the median particle size tends to decrease with height for stratiform cloud cases. However, this trend is not observed for convective cloud cases where measurements indicate that large particles can exist even near the cloud top.

Corresponding author address: Stephen M. Sekelsky, Dept. of Electrical and Computer Engineering, Knowles 209 C, University of Massachusetts, Amherst, MA 01003.

Save
  • Ackerman, T., E. Clothiaux, R. Austin, M. Platt, S. Young, W. Ecklund, S. Sekelsky, and R. McIntosh, 1996: The Maritime Continent Thunderstorm Experiment: Cirrus anvil outflow, the Garden Point MCTEX research group. Preprints, 1996 Atmospheric Radiation Measurement (ARM) Program Science Team Meeting, San Antonio, TX, U.S. Department of Energy, 13.

  • Atlas, D., S. Matrosov, A. Heymsfield, M. Chou, and D. Wolff, 1995:Radar and radiation properties of ice clouds. J. Appl. Meteor.,34, 2329–2345.

  • Auer, A., and D. Veal, 1970: The dimensions of ice crystals in natural clouds. J. Atmos. Sci.,27, 919–926.

  • Aydin, K., and T. Walsh, 1996: Computational study of millimeter wave scattering from bullet rosette type ice crystals. Proc. 1996 Int. Geoscience and Remote Sensing Symp., Lincoln, NE, IEEE, 563–565.

  • ——, and C. Tang, 1997: Millimeter wave radar scattering from model ice crystal distributions. IEEE Trans. Geosci. Remote Sens.,35, 140–146.

  • Bankert, R. L., 1994: Cloud classification of AVHRR imagery in maritime regions using a probabilistic neural network. J. Appl. Meteor.,33, 909–918.

  • Battan, L. J., 1973: Radar Observation of the Atmosphere. University of Chicago, 324 pp.

  • Bohren, C. F., and S. B. Singham, 1991: Backscattering by nonspherical particles: A review of methods and suggested new approaches. J. Geophys. Res.,96 (D3), 5269–5277.

  • Brown, P., and P. Francis, 1995: Improved measurements of ice water content in cirrus using a total water probe. J. Atmos. Oceanic Technol.12, 410–414.

  • Carter, D., K. Gage, W. Ecklund, W. Angevine, P. Johnston, A. Riddle, J. Wilson, and C. Williams, 1995: Developments in UHF lower tropospheric wind profiling at NOAA’s aeronomy laboratory. Radio Sci.,30, 977–1001.

  • Deirmendjian, D., 1969: Electromagnetic Scattering on Spherical Polydispersions. American Elsevier, 290 pp.

  • Draine, B., and P. Flatau, 1994: Discrete-dipole approximation for scattering calculations. J. Opt. Soc. Amer.,11A, 1491–1499.

  • ——, and ——, 1996: User Guide to the discrete dipole approximation code DDSCAT Version 5a. Princeton Observatory Preprint POPe-695, Princeton University Observatory, Princeton University, Princeton, NJ, 39 pp. [Available from Princeton University Observatory, Princeton University, Princeton, NJ 08544-1001; available via anonymous ftp from astro.princeton.edu/draine/scat/ddscat/ver5a.].

  • Eccles, P. J., and D. Atlas, 1973: A dual-wavelength radar hail detector. J. Appl. Meteor.12, 847–856.

  • Ecklund, W., C. Williams, P. Johnston, and K. Gage, 1999: A 3-GHz profiler for precipitating cloud studies. J. Atmos. Oceanic Technol., in press.

  • Evans, K. F., and J. Vivekanandan, 1990: Multiparameter radar and microwave radiative transfer modeling on nonspherical atmospheric ice particles. IEEE Trans. Geosci. Remote Sens.,28, 423–437.

  • Galloway, J., A. Pazmany, J. Mead, R. E. McIntosh, D. Leon, J. French, R. Kelly, and G. Vali, 1997: Detection of ice hydrometeor alignment using an airborne W-band polarimetric radar. J. Atmos. Oceanic Technol.,14, 3–12.

  • Gossard, E. E., 1994: Measurement of cloud droplet size spectra by Doppler radar. J. Atmos. Oceanic Technol.,11, 712–726.

  • Gunn, K., and J. S. Marshall, 1958: The distribution with size of aggregate snowflakes. J. Meteor.,15, 452–461.

  • Haykin, S., 1994: Neural Networks: A Comprehensive Foundation. MacMillan College Publishing, 696 pp.

  • Hendry, A., G. C. McCormick, and B. Barge, 1976: The degree of common orientation of hydrometeors observed by polarization diversity radars. J. Appl. Meteor.,15, 633–640.

  • Heymsfield, A., 1972: Ice crystal terminal velocities. J. Atmos. Sci.,29, 1348–1357.

  • Hobbs, P., S. Chang, and J. Locatelli, 1974: The dimensions and aggregation of ice crystals in natural clouds. J. Geophys. Res.79, 2199–2206.

  • Intrieri, J. M., G. L. Stephens, W. L. Eberhard, and T. Uttal, 1993: A method for determining cirrus cloud particle sizes using lidar and radar backscatter technique. J. Appl. Meteor.,32, 1074–1082.

  • Keenan, T., and Coauthors, 1994: Science Plan Maritime Continent Thunderstorm Experiment (MCTEX). BMRC Research Rep. 44, BMRC, Melbourne, Victoria, Australia, 61 pp. [Available from Bureau of Meteorology, BMRC, P.O. Box 1289k, Melbourne, Victoria 3001, Australia.].

  • Kosarev, A., and J. Mazin, 1991: An empirical model of the physical structure of upper layer clouds. Atmos. Res.,26, 213–228.

  • Lhermitte, R. M., 1987: Observations of stratiform rain with 94 GHz and S-band Doppler radar. Tech. Rep. AFGL-TR-0268, Air Force Geophysics Laboratory, Hanscom AFB, MA, 18 pp. [Available from Air Force Geophysics Laboratory, Air Force Systems Command, United States Air Force, Hanscom Air Force Base, MA 01731.].

  • ——, 1988: Cloud and precipitation remote sensing at 94 GHz. IEEE Trans. Geosci. Remote Sens.,26, 207–216.

  • Locatelli, J., and P. Hobbs, 1974: Fall speeds and masses of solid precipitation particles. J. Geophys. Res.,79, 2185–2197.

  • Lohmeier, S. P., S. M. Sekelsky, J. M. Firda, G. A. Sadowy, and R. E. McIntosh, 1997: Classification of particles in stratiform clouds using the 33 and 95 GHz polarimetric cloud profiling radar system. IEEE Trans. Geosci. Remote Sens.,35, 256–270.

  • Magono, C., and T. Nakamura, 1965: Aerodynamic studies of falling snowflakes. J. Meteor. Soc. Japan,43, 139–147.

  • Marshall, J., and W. Palmer, 1948: The distribution of raindrops with size. J. Meteor.,5, 165–166.

  • Matrosov, S. Y., 1992: Radar reflectivity in snowfall. IEEE Trans. Geosci. Remote Sens.,30, 454–461.

  • ——, 1993: Possibilities of cirrus particle sizing from dual-frequency radar measurements. J. Geophys. Res.,98 (D11), 20 675–20 683.

  • ——, J. B. Snider, and R. A. Kropfli, 1992: Estimation of ice cloud parameters from ground-based infrared radiometer and radar measurements. J. Geophys. Res.,97 (D11), 11 567–11 574.

  • McFarquhar, G., and A. Heymsfield, 1996: Microphysical characteristics of three anvils sampled during the central equitorial Pacific experiment. J. Atmos. Sci.,53, 2401–2423.

  • Metcalf, J. I., 1995: Radar observations of changing orientations of hydrometeors in thunderstorms. J. Appl. Meteor.,34, 757–772.

  • Mitchell, D., R. Zhang, and R. Pitter, 1990: Mass–dimensional relationships for ice particles and the influence of riming on snowfall rates. J. Appl. Meteor.,29, 153–163.

  • Nemarich, J., R. J. Wellman, B. E. Gordon, D. R. Hutchins, G. A. Turner, and J. Lacombe, 1984: Attenuation and backscatter for snow and sleet at 96, 140 and 225 GHz. Proc. Snow Symp. IV, Hanover, NH, U.S. Army Cold Regions Research and Engineering Laboratory, 41–52.

  • O’Brien, S. G., and G. H. Goedecke, 1988: Scattering of millimeter waves by snow crystals and equivalent homogeneous symmetric particles. Appl. Opt.,27, 2439–2444.

  • Oguchi, T., 1983: Electromagnetic wave propagation and scattering in rain and other hydrometeors. Proc. IEEE,71, 1836–1844.

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

  • Ray, P., 1972: Broadband complex refractive indices of ice and water. Appl. Opt.,11, 1836–1844.

  • Sassen, K., 1987a: Ice cloud content from radar reflectivity. J. Climate Appl. Meteor.,26, 1050–1053.

  • ——, 1987b: Polarization and Brewster angle properties of light pillars. J. Opt. Soc. Amer.,4A, 570–580.

  • Sekelsky, S. M., and R. E. McIntosh, 1996: Cloud observations with a polarimetric 33 GHz and 95 GHz radar. Meteor. Atmos. Phys.,58, 123–140.

  • Sekhon, R. S., and R. C. Srivastava, 1970: Snow size spectra and radar reflectivity. J. Atmos. Sci.,27, 299–307.

  • Smith, P. L., 1984: Equivalent radar reflectivity factors for snow and ice particles. J. Climate Appl. Meteor.,23, 1258–1260.

  • Tang, C., and K. Aydin, 1995: Scattering from ice crystals at 94 and 220 GHz millimeter wave frequencies. IEEE Trans. Geosci. Remote Sens.,33, 93–99.

  • Thomason, J., A. Illingworth, and V. Marecal, 1995: Density and size distribution of aggregating snow particles inferred from coincident aircraft and radar observations. Preprints, 27th Conf. on Radar Meteorology, Vail, CO, Amer. Meteor. Soc., 127–129.

  • Ulbrich, C. W., 1983: Natural variations in the analytical form of the raindrop size distribution. J. Climate Appl. Meteor.,22, 1764–1775.

  • Xiao, R., and V. Chandrasekar, 1997: Development of a neural network based algorithm for rainfall estimation from radar observables. IEEE Trans. Geosci. Remote Sens.,35, 160–171.

  • Zell, A., G. Mamier, and M. Vogt, 1995: Stuttgart Neural Network Simulator, Version 4.1: User manual. University of Stuttgart, Stuttgart, Germany, 312 pp. [Available from University of Stuttgart, SNNS Group Breitwiesenstrasse 20-22 Stuttgart, Germany 70565; available via anonymous ftp from ftp.informatik.uni-stuttgart.de/pub/SNNS.].

All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 554 96 5
PDF Downloads 257 63 5