Interpretation of ATSR-2 measurements of cirrus clouds using phase functions of imperfect hexagonal ice crystals

1998 ◽  
Author(s):  
Wouter H. Knap ◽  
M. Hess ◽  
Piet Stammes ◽  
Robert B. A. Koelemeijer ◽  
Philip D. Watts
2014 ◽  
Vol 39 (19) ◽  
pp. 5788 ◽  
Author(s):  
Anatoli Borovoi ◽  
Alexander Konoshonkin ◽  
Natalia Kustova

Author(s):  
Natalia V. Kustova ◽  
Anatoli G. Borovoi ◽  
Alexander V. Konoshonkin ◽  
Andrey P. Lyulyakin ◽  
Tatiana B. Zhuravleva ◽  
...  

1995 ◽  
Vol 34 (25) ◽  
pp. 5867 ◽  
Author(s):  
Jianyun Zhang ◽  
Lisheng Xu

1999 ◽  
Vol 104 (D24) ◽  
pp. 31721-31730 ◽  
Author(s):  
Wouter H. Knap ◽  
Michael Hess ◽  
Piet Stammes ◽  
Robert B. A. Koelemeijer ◽  
Phil D. Watts

2006 ◽  
Vol 100 (1-3) ◽  
pp. 91-102 ◽  
Author(s):  
Guang Chen ◽  
Ping Yang ◽  
George W. Kattawar ◽  
Michael I. Mishchenko

2013 ◽  
Vol 38 (15) ◽  
pp. 2881 ◽  
Author(s):  
Anatoli Borovoi ◽  
Alexander Konoshonkin ◽  
Natalia Kustova

1995 ◽  
Vol 34 (2) ◽  
pp. 447-459 ◽  
Author(s):  
E. O. Schmidt ◽  
R. F. Arduini ◽  
B. A. Wielicki ◽  
R. S. Stone ◽  
S-C. Tsay

Abstract Brightness temperature difference (BTD) values are calculated for selected Geostationary Operational Environmental Satellite (GOES-6) channels (3.9, 12.7 µm) and Advanced Very High Resolution Radiometer channels (3.7, 12.0 µm). Daytime and nighttime discrimination of particle size information is possible given the infrared cloud extinction optical depth and the BTD value. BTD values are presented and compared for cirrus clouds composed of equivalent ice spheres (volume, surface area) versus randomly oriented hexagonal ice crystals. The effect of the hexagonal ice crystals is to increase the magnitude of the BTD values calculated relative to equivalent ice sphere (volume, surface area) BTDs. Equivalent spheres (volume or surface area) do not do a very good job of modeling hexagonal ice crystal effects on BTDs; however, the use of composite spheres improves the simulation and offers interesting prospects. Careful consideration of the number of Legendre polynomial coefficients used to fit the scattering phase functions is crucial to realistic modeling of cirrus BTDs. Surface and view-angle effects are incorporated to provide more realistic simulation.


1996 ◽  
Vol 14 (5) ◽  
pp. 566-573
Author(s):  
B. Strauss

Abstract. The scattering behaviour of bullet-rosette and bullet-shaped ice particles is investigated using model calculations (ray tracing method) with special emphasis on the asymmetry factor g. Because the variability of the geometrical features of these particles is very large, some representative shapes are used in the calculations. The model is based on geometrical optics, and particles are assumed to be oriented randomly; a wavelength of 0.56 μm is considered; absorption is neglected. The scattering behaviour of bullet rosettes is compared to that of single branches out of the bullet rosette. It turns out that there are slight differences in the asymmetry factor values, depending on the lengths of the branches (∆g~0.02) and on the angles between the branches (∆g~0.01). Bullets show some special features in their phase functions due to the pyramid. The length of the particle influences the asymmetry factor (∆g~0.10), as does the shape of the pyramid (∆g~0.07). The influence of the pyramidal shape decreases with increasing particle length. Bullets were compared to hexagonally shaped columns. This was done for two columns, one as long as the columnar part of the bullet (length without pyramid), and one for a column as long as the bullet including the pyramid. Asymmetry factor values of bullets with a pyramidal angle of 28° deviate less than ∆g~0.01 from the range given by the two values of the columns.


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