A simple model for estimation of snow/ice surface temperature of Antarctic ice sheet using remotely sensed thermal band data

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Indian Journal of Radio & Space Physics Vol 44, March 2015, pp 51-55 A simple model for estimation of snow/ice surface temperature of Antarctic ice sheet using remotely sensed thermal band data H S Gusain 1,$,*, V D Mishra 1, Gursewak Singh Brar 2 & Ashwagosha Ganju 1 1 Snow and Avalanche Study Establishment, Research and Development Centre, Sector 37A, Chandigarh 160 036, India 2 Department of Geography, Punjab University, Sector 15, Chandigarh 160 015, India $ E-mail: gusain_hs@yahoo.co.in Received 18 August 2014; revised received and accepted 22 January 2015 In this paper, a model has been developed to estimate surface temperature of Antarctic ice sheet using thermal bands of Moderate Resolution Imaging Spectroradiometer (MODIS) sensor images and in situ surface temperature measurements. The brightness temperature of snow/ice surface of Antarctica has been estimated for MODIS bands 31 and 32 using Planck s spectral radiation equation. Split window technique has been used to develop the model from brightness temperature and Automatic Weather Station recorded surface temperature. The model has been validated using in situ measurements of surface temperature of the ice sheet near Indian Antarctic Research Station Maitri. High coefficient of determination (R2 in the range 0.952-0.99) and low root mean square error (0.8-1.2 C) has been obtained between modeled and in situ recorded surface temperature. The model is easy to use and can generate the surface temperature maps at spatial resolution of 1.0 km. These maps can be useful in various glaciological, hydrological, climatological and ecological studies of the ice sheet. Keywords: Snow, Ice, Surface temperature, Antarctic ice sheet, Thermal bands, Satellite sensor images, Brightness temperature PACS Nos: 92.40.vv; 92.40.vw; 92.60.hv; 93.30.Ca 1 Introduction Surface temperature is an important parameter for controlling various physical, biological and chemical processes on earth. It has been estimated for different land covers using various satellite sensors data by various researchers 1-8. Generally, two types of methods are in vogue to estimate surface temperature using remote sensing data: (i) single infrared channel method and (ii) the split-window method. Single channel method requires radiative transfer model and vertical profiles of atmospheric data. The splitwindow method corrects for atmospheric effects based on differential absorption in adjacent infrared bands 2,9,10. Studies have been devoted to establish the methodology for retrieval of land surface temperature (LST) from thermal bands of Moderate Resolution Imaging Spectroradiometer (MODIS), Advanced Very High Resolution Radiometer (AVHRR), Advanced Spaceborne Thermal Emission and Reflection Radiometer (ASTER) and many other satellites sensor data. LST can be retrieved using thermal infrared remote sensing only in clear sky conditions while microwave techniques have all weather capabilities 2. Surface temperature estimated from thermal bands data of different multi-spectral satellite sensors has advantage of higher spatial resolution as compared to that estimated from passive microwave data. Thus, the intensity of emissions captured by thermal bands of multi-spectral images is stronger as compared to the intensity of emissions captured by passive microwave images. Passive microwave and thermal bands of multi-spectral images have been used to estimate surface temperature of various land covers. Key et al. 3 estimated clear sky surface temperature of polar regions using thermal bands data of AVHRR and Along Track Scanning Radiometer (ATSR) and obtained accuracies in the range of 0.3-2.1 K. Basist et al. 11 demonstrated the capability of Special Sensor Microwave Imager (SSM/I) to observe the land surface temperature in United States and the globe and reported an absolute error of about 2.0 C with in situ measurements. Hall et al. 6 produced daily surface temperature (IST) of sea ice at spatial resolution of 1 km and 4 km using Terra and Aqua MODIS images with root mean square error (RMSE) of 1.2-3.7 K. Brogioni et al. 7 estimated surface temperature of east Antarctic ice sheet using passive

52 INDIAN J RADIO & SPACE PHYS, MARCH 2015 microwave remote sensing data of Advanced Microwave Scanning Radiometer-Earth (AMSR-E) with RMSE in the range 2-7 K. Negi et al. 12 derived a regression relation for estimation of snow surface temperature of snow cover in Western Himalayas using MODIS thermal bands data and ground data. The equation has been validated from in situ recorded data in lower, middle and upper Himalaya and an RMSE of 2.5 C was reported. In this paper, a simple model is presented to estimate surface temperature of the Antarctic ice sheet using only thermal bands data of the MODIS. The model generates surface temperature maps at spatial resolution of 1 km. 2 Study area and Data The study area lies in the eastern Dronning Maud Land of East Antarctica. Indian research station Maitri is located in Schirmacher Oasis in the coastal margin of the Dronning Maud Land, East Antarctica at 70 45.94'S and 11 44.13'E (Refs 13,14). The study area considered in the present work extends from 70.2 S to 72 S and 8.6 E to 14 E (Fig. 1). It comprises ice shelves of Princess Astrid Coast, ice-free area of Schirmacher Oasis, continental ice sheet and Wohlthat Mountain from north to south. North of the Shirmacher Oasis is ice shelf spreading about 70 km up to Antarctic sea and south of the Oasis is continental ice sheet which increases in thickness towards south. Wohlthat Mountain is about 70 km south of the Shirmacher Oasis. The elevation ranges from 22 m near Antarctic sea to 3003 m on high Antarctic plateau in the study area. Most part of the study area is flat ice sheet having slope less than 5. A small terrain with slope angle between 20 and 30 also exists near Schirmacher Oasis and Wohlthat Mountain. In the present work, in situ recorded snow/ice surface temperature data and remotely acquired MODIS sensor data have been used. Snow and Avalanche Study Establishment (SASE) has installed two automatic weather stations (AWS) on Antarctic ice sheet at a distance of approximately 1 km and Fig. 1 Study area in Antarctica 8 km from Maitri research station. Infrared (IR) sensor mounted on these AWSs record hourly snow/ice surface temperature. Images from MODIS sensor on-board Terra and Aqua satellite (downloaded from http://ladsweb.nascom.nasa.gov) have been used for estimation of surface temperature. Channel 31 and 32 of MODIS sensor image are thermal bands and have been used to estimate brightness temperature. Salient specifications of MODIS data 15 is given in Table 1. MODIS sensor data on clear sky days for the period 2007-2012 have been collected for the study. 3 Methodology The following form of equation within the framework of the split window algorithm 1,2,4,9 has been used for estimation of surface temperature in Antarctica. T s = a + b.t 31 + c.(t 31 T 32 ) (1) where, T s, is surface temperature; T 31, brightness temperature of MODIS band 31; T 32, brightness temperature of MODIS band 32; and a, b, c, regression coefficients. Emissivity of the snow/ice surface has been assumed to be unity in the present study 16. Hori et al. 17 examined the dependence of the directional emissivity on various types of snow surfaces. They observed that emissivity at 10.5 and 12.5 µm for different snow types is different for nadir angle and off-nadir angle and vary from 0.949 to 0.997. They demonstrated that directional emissivity of snow in the thermal infrared vary depending upon the surface snow type. Emissivity of snow and ice also vary with melting of the snow/ice surface. Present study area has different types of snow/ice surfaces. As field observations are not available on different emissivity values of snow/ice surfaces and change in emissivity values Table 1 Salient specifications of MODIS sensor Total number of bands 36 Wavelength range 0.4 14.4 µm Swath 2330 km Radiometric resolution 12 bit Repeat cycle 1-2 days Orbit elevation 705 km Band Spatial resolution, m Spectral resolution, µm Radiance_scale, mw cm -2 sr -1 µm -1 Band 31 1000 x 1000 10.780 11.280 0.0000840022 Band 32 1000 x 1000 11.770 12.270 0.0000729698

GUSAIN et al.: ESTIMATION OF SNOW/ICE SURFACE TEMPERATURE OF ANTARCTIC ICE SHEET 53 due to melting of the snow/ice in the study area, it may have some inherent error in the model. MODIS thermal bands 31 (10.780-11.280 µm) and 32 (11.770-12.270 µm) have been used to estimate brightness temperature in the study area. According to the black body radiation principle, the spectral radiance emitted from surface as a black body can be described by Planck s spectral radiation equation 18 given as: L λ (T) = 2 h c 2 λ -5 (e hc/λkt -1) -1 (2) where, L λ, is spectral radiance of black body; h, Planck s constant (6.626 x 10-34 J s); c, velocity of light (3 x 10 8 m s -1 ); λ, wavelength; k, Boltzmann s constant (1.381 x 10-23 J K -1 ); and T, brightness temperature. Using Eq. (2), the brightness temperature can be estimated as 4 : T = hcλ -1 k -1 [log (1+2 h c 2 λ -5 L λ -1 )] -1 (3) In Eq. (3), mean wavelength 11.03 and 12.02 µm for the MODIS bands 31 and 32 have been used, respectively for the estimation of brightness temperature. Spectral radiance (L λ ) values for MODIS bands 31 and 32 have been estimated using following equation 19 : L λ = radiance_scale λ (DN radiance_offset λ ) (4) where, radiance_scale λ and radiance_offset λ are the scale and offset parameters, respectively for MODIS spectral bands, radiance_scale λ for MODIS bands 31 and 32 are given in Table 1; radiance_offset λ for MODIS bands 31 and 32 are 1577.34 and 1658.22, respectively. Spectral radiance for MODIS bands 31 and 32 have been estimated for different days of the years 2007, 2008 and 2009. Brightness temperature has been estimated for these days using Eq. (3). AWS recorded in situ surface temperature at the time of MODIS satellite pass and estimated brightness temperature have been used to obtain the values of constants a, b and c in Eq. (1). The coefficients obtained are given as: a = -260.0967412, b = 0.959826974, and c = -1.034104696 These values of the coefficients a, b, and c have been used in Eq. (1) to estimate surface temperature at spatial scale and the model is given as: T s = -260.0967412 + 0.959826974T 31-1.034104696 (T 31 T 32 ) (5) Using this model, surface temperature has been estimated at each pixel of the MODIS image in the study area. The algorithm was developed using the data of the years 2007, 2008, 2009 and the algorithm was validated at the AWS locations using data of different days of the years 2010-2012. 4 Results and Discussion Figures 2 and 3 show the MODIS derived surface temperature map of the study area on 12 January 2010 and 7 February 2012, respectively at 0900 hours. The surface temperature on 12 January 2010 varies from -19 to 6.9 C in the study area with mean value of -7.8+4.7 C. The surface temperature on 7 February 2012 varies from -25 to 4 C in the study area with mean value of -13.7+4.9 C. Surface temperature has been observed decreasing with time from January to February, which is obvious as the season changes from summer season towards winter season in the continent. Surface temperature has also been estimated for different days of the years 2007-2012 and surface temperature maps have been Fig. 2 Surface temperature map of the study area for 12 January 2010 at 0900 hrs UT Fig. 3 Surface temperature map of the study area for 7 February 2012 at 0900 hrs UT

54 INDIAN J RADIO & SPACE PHYS, MARCH 2015 Fig. 4 Observed vs estimated surface temperature for different clear sky days of the year 2010 generated. These maps have been validated at the AWS locations using in situ recorded surface temperature values. The regression plot between estimated and observed surface temperature during different days of the year 2010 and 2011-12 are shown in Figs 4 and 5, respectively. High coefficient of determination (R 2 = 0.99 for 2010 and R 2 = 0.952 for summer season 2011-12) has been obtained between model estimated and in situ recorded values. Absolute error between observed and estimated surface temperature varied from 0.1 C to 1.5 C during different days of the year 2010, mean absolute error (MAE) obtained was 0.6 C and root mean square error (RMSE) obtained was 0.8 C. For the years 2011 and 2012, absolute error between observed and estimated surface temperature varied from 0 C to 2.2 C with MAE of 1.0 C and RMSE of 1.2 C, respectively. The surface temperature maps, thus generated, may be used in various glaciological, ecological and environmental studies. 5 Conclusion In the present study a simple algorithm has been developed to estimate snow/ice surface temperature of the Antarctic ice sheet using MODIS thermal bands data and in situ recorded data. Algorithm has potential to generate surface temperature maps from thermal bands images at spatial resolution of 1.0 km. These maps have been validated with ground observed values. A high coefficient of determination (R 2 = 0.952 to 0.99) and low root mean square error (RMSE = 0.8-1.2 C) has been obtained between model estimated and ground observed values. The maps may be potentially used for estimation of Fig. 5 Observed vs estimated surface temperature for different clear sky days of the year 2011 and 2012 energy fluxes, hydrological, glaciological and other studies in Antarctica. Acknowledgement The authors are thankful to all the scientists/technical officers/technical staff of Snow and Avalanche Study Establishment (SASE), who participated in Indian Scientific Expedition to Antarctica and collected valuable data for the study. They acknowledge the logistic support provided by National Centre of Antarctic and Ocean Research (NCAOR), Goa, during field campaigns in Antarctica. NASA s LAADS web (http://ladsweb.nascom.nasa. gov) is duly acknowledged for providing MODIS data. References 1. Price J C, Land surface temperature measurements from the split window channels of the NOAA-7 AVHRR, J Geophys Res (USA), 79 (1984) pp 5039-5044. 2. Wan Z & Dozier J, A generalized split-window algorithm for retrieving land surface temperature measurement from space, IEEE Trans Geosci Remote Sens (USA), 34 (1996) pp 892 905. 3. Key J R, Collins J B, Fowler C & Stone R S, High-latitude surface temperature estimates from thermal satellite data, Remote Sens Environ (USA), 61 (1997) pp 302-309. 4. Qin Z & Karnieli A, Progress in the remote sensing of land surface temperature and ground emissivity using NOAA-AVHRR data, Int J Remote Sens (UK), 20 (1999) pp 2367-2393. 5. Wan Z, MODIS Land-Surface temperature algorithm theoretical basis document (LST ATBD), version 3.3 (Institute for Computational Earth System Science, University of California, Santa Barbara, USA), 1999, pp 1-77. 6. Hall D K, Key J R, Casey K A, Riggs G A & Cavalieri D J, Sea ice surface temperature product from MODIS, IEEE Trans Geosci Remote Sens (USA), 42 (2004) pp 1076-1087. 7. Brogioni M, Macelloni G, Pettinato S & Montomoli F, Estimation of air and surface temperature evolution of the

GUSAIN et al.: ESTIMATION OF SNOW/ICE SURFACE TEMPERATURE OF ANTARCTIC ICE SHEET 55 east Antarctic sheet by means of passive microwave remote sensing, Proc of IEEE International Geoscience and Remote Sensing Symposium (IGARSS) (IEEE, Vancouver, Canada, BC), 2011, pp 3859-3862. 8. Hall D K, Surface temperature of snow and ice, in Encyclopaedia of snow, ice and glaciers, edited by Vijay P Singh, Pratap Singh and Umesh K Haritashya (Springer, USA), 2011, pp 1123-1125. 9. Becker F & Li Z -L, Towards a local split window method over land surface, Int J Remote Sens (UK), 3 (1990) pp 369-393. 10. Price J C, Estimating surface temperature from satellite thermal infrared data: A simple formulation for the atmospheric effect, Remote Sens Environ (USA), 13 (1983) pp 353-361. 11. Basist A, Grody N C, Peterson T C & Williams C N, Using the special sensor microwave/imager to monitor land surface temperatures, wetness and snow cover, J Appl Meteorol (USA), 37 (1998) pp 888-911. 12. Negi H S, Thakur N K & Mishra V D, Estimation and validation of snow surface temperature using MODIS data for NW-Himalaya, J Indian Soc Remote Sens, 35 (2007) pp 287 299. 13. Gusain H S, Mishra V D & Arora M K, A four-year record of the meteorological parameters, radiative and turbulent energy fluxes at the edge of the East Antarctic ice sheet, close to Schirmacher Oasis, Antarctic Sci (UK), 26 (1) (2014) pp 93-103. 14. Gusain H S, Singh K K, Mishra V D, Srivastava P K & Ganju A, Study of surface energy and mass balance at the edge of the Antarctic ice sheet during summer in Dronning Maudland, East Antarctica, Antarctic Sci (UK), 21 (4) (2009) pp 401-409. 15. Salomonson V V, Barnes W L, Maymon P W, Montgomery H E & Ostrow H, MODIS: Advanced Facility Instrument for Studies of the Earth as a System, IEEE Trans Geosci Remote Sens (USA), 27 (1989) pp 145 153. 16. Bintanja R & Van Den Broeke M R, Local climate, circulation and surface-energy balance of an Antarctic blueice area, Ann Glaciol (UK), 20 (1994) pp 160-168. 17. Hori M, Aoki T, Tanikawa T, Motoyoshi H, Hachikubo A, Sugiura K, Yasunari T J, Eide H, Storvold R, Nakajima Y & Takahashi F, In-situ measured spectral directional emissivity of snow and ice in the 8-14 µm atmospheric window, Remote Sens Environ (USA),100 (2006) pp 486-502. 18. Ulaby F T, Moore R K & Fung A K, Microwave remote sensing fundamentals and radiometry, vol I (Book-Mart Press, North Bergen NJ, USA), 1990, 365 p. 19. Qu J J, Gao W, Kafatos M, Murphy R E & Salomonson V V, Earth Science Satellite Remote Sensing vol 1: Science and Instruments (Tsinghua University Press, Springer, USA), 2006, 414 p.