TY - JOUR
T1 - In-situ measured spectral directional emissivity of snow and ice in the 8-14 μm atmospheric window
AU - Hori, Masahiro
AU - Aoki, Teruo
AU - Tanikawa, Tomonori
AU - Motoyoshi, Hiroki
AU - Hachikubo, Akihiro
AU - Sugiura, Konosuke
AU - Yasunari, Teppei J.
AU - Eide, Hans
AU - Storvold, Rune
AU - Nakajima, Yukinori
AU - Takahashi, Fumihiro
N1 - Funding Information:
This work was conducted as part of the ADEOS-II/GLI Cal/Val experiment supported by Japan Aerospace Exploration Agency (JAXA). The authors would like to thank the cooperation of the U.S. Department of Energy as part of the Atmospheric Radiation Measurement Program for the use of the atmospheric radiation data and the ARM facilities at the North Slope of Alaska site. Atmospheric profiles (JMAOA) data were provided by Japan Meteorological Agency. We thank Yasuko Iizuka for obtaining some of snow pit work results used in this paper and many helpful comments. We are also grateful to the three anonymous reviewers, and their useful comments and suggestions on the original manuscript. M.H. conceived and designed the experiment, and together with R.S. and F.T. carried out the measurements and data analysis of snow TIR emissivity; T.A. and T.T. together with H.M. and H.E. carried out the measurements and data analysis of snow SWIR reflectance; A.H., K.S., and T.J.Y. together with Y.N. designed and carried out the snow pit work; M.H. wrote the paper.
PY - 2006/2/28
Y1 - 2006/2/28
N2 - The directional emissivity of snow and ice surfaces in the 8-14 μm thermal infrared (TIR) atmospheric window was determined from spectral radiances obtained by field measurements using a portable Fourier transform infrared spectrometer in conjunction with snow pit work. The dependence of the directional emissivity on the surface snow type (grain size and shape) was examined. We obtained emissivity spectra for five different surface types, i.e., fine dendrite snow, medium granular snow, coarse grain snow, welded sun crust snow, and smooth bare ice. The derived emissivities show a distinct spectral contrast at wavelengths λ = 10.5-12.5 μm which is enhanced with increasing the snow grain size. For example, emissivities at both 10.5 μm and 12.5 μm for the nadir angle were 0.997 and 0.984 for the fine dendrite snow, 0.996 and 0.974 for the medium granular snow, 0.995 and 0.971 for the coarse grain snow, 0.992 and 0.968 for the sun crust, and 0.993 and 0.949 for the bare ice, respectively. In addition, the spectral contrast exhibits a strong angular dependence, particularly for the coarser snow and bare ice, e.g., the emissivity at λ = 12.5 μm for the off-nadir angle of 75° reaches down to 0.927, 0.896, and 0.709 for the coarse grain snow, sun crust, and bare ice cases, respectively. The angular dependent emissivity spectra of the bare ice were quite consistent with the spectra predicted by the Fresnel reflectance theory. The observed results firmly demonstrate that the directional emissivity of snow in the TIR can vary depending upon the surface snow type. The high variability of the spectral emissivity of snow also suggests the possibility to discriminate between snow and ice types from space using the brightness temperature difference in the atmospheric window.
AB - The directional emissivity of snow and ice surfaces in the 8-14 μm thermal infrared (TIR) atmospheric window was determined from spectral radiances obtained by field measurements using a portable Fourier transform infrared spectrometer in conjunction with snow pit work. The dependence of the directional emissivity on the surface snow type (grain size and shape) was examined. We obtained emissivity spectra for five different surface types, i.e., fine dendrite snow, medium granular snow, coarse grain snow, welded sun crust snow, and smooth bare ice. The derived emissivities show a distinct spectral contrast at wavelengths λ = 10.5-12.5 μm which is enhanced with increasing the snow grain size. For example, emissivities at both 10.5 μm and 12.5 μm for the nadir angle were 0.997 and 0.984 for the fine dendrite snow, 0.996 and 0.974 for the medium granular snow, 0.995 and 0.971 for the coarse grain snow, 0.992 and 0.968 for the sun crust, and 0.993 and 0.949 for the bare ice, respectively. In addition, the spectral contrast exhibits a strong angular dependence, particularly for the coarser snow and bare ice, e.g., the emissivity at λ = 12.5 μm for the off-nadir angle of 75° reaches down to 0.927, 0.896, and 0.709 for the coarse grain snow, sun crust, and bare ice cases, respectively. The angular dependent emissivity spectra of the bare ice were quite consistent with the spectra predicted by the Fresnel reflectance theory. The observed results firmly demonstrate that the directional emissivity of snow in the TIR can vary depending upon the surface snow type. The high variability of the spectral emissivity of snow also suggests the possibility to discriminate between snow and ice types from space using the brightness temperature difference in the atmospheric window.
KW - Directional emissivity
KW - Remote sensing
KW - Snow and ice
KW - Snow grain size
KW - Surface temperature
UR - http://www.scopus.com/inward/record.url?scp=32244433128&partnerID=8YFLogxK
U2 - 10.1016/j.rse.2005.11.001
DO - 10.1016/j.rse.2005.11.001
M3 - 学術論文
AN - SCOPUS:32244433128
SN - 0034-4257
VL - 100
SP - 486
EP - 502
JO - Remote Sensing of Environment
JF - Remote Sensing of Environment
IS - 4
ER -