A Remote Sensing Analysis of the Temporal and Spatial Changes of Land Surface Temperature in Calabar Metropolis, Nigeria ()
1. Introduction
Land surface temperature (LST) which is controlled by the surface energy balance, atmospheric state and thermal properties of the surface/subsurface rocks is one of the important parameters in several environmental models [1] . As suggested by [2] , LST provides an accurate measure for indicating energy exchange balance between the Earth and the atmosphere. Studies on LST are important to environmental studies and management of the Earth’s resources due to its ability to determine the effective radiating temperature of the Earth’s surface. Also, LST is a major factor of determining the partition of the available energy into sensible and latent heat flux. For example, the rate of change of LST is sensitive to the characteristics of the land surface such as soil moisture, land use and vegetation [3] .
With the advent of thermal remote sensing technology, observation of LST has become possible using Satellite and Aircraft platforms [4] , which has provided the new direction for the observations of thermal reflectance and the study of their effects through the combination of thermal remote sensing and urban micrometeorology [5] . Various satellites, and methods such as Landsat TM Bands are available that can be used to examine the LST [6] [7] [8] [9] . Landsat TM Bands are the data which is most widely used for these studies [6] [7] [8] [9] . Previous studies have demonstrated that the LST product retrieved from thermal infrared (TIR) sensors can be used to monitor the distribution of temperature over an area [5] [10] [11] [12] [13] [14] . Several researchers have estimated air temperatures using Landsat TM Imageries [7] [15] - [20] . This paper assesses the temporal and spatial changes of LST over Calabar Metropolis, Nigeria.
2. Materials and Method
2.1. Study Area
Calabar Metropolis, the study area, is the capital of Cross River State, Nigeria, located at the Southern part of the State. It encompasses of Calabar Municipality and Calabar South Local Government Areas and lies between latitudes 4˚50'N and 5˚10'N and longitudes 8˚17'E and 8˚20'E; bounded to the north by Odukpani Local Government Area (LGA) and to the East by Akpabuyo LGA. Calabar Metropolis is sandwiched between the Great Kwa River to the East and the Calabar River to the West. The present of urban area is on the eastern bank of the Calabar River, its growth of the southern part is hindered by the mangrove swamps. It covers an estimated land area of about 274.593 km2 (Figure 1).
Calabar falls within tropical equatorial (Af) climate of high temperature, high relative humidity and abundant annual rainfall [21] . The annual rainfall is 2750 mm and the mean annual average temperature is 26.1˚C. The study area has witnessed a tremendous increase in the population of 10,000 estimated at the pre-colonial, to 99,352 in 1993; 328,876, in 1991. The last census in 2006 put the population to 371,022 [22] . The population growth of Calabar has been followed by the expansion of its physical boundaries. This increase in the physical boundaries implies a corresponding loss of vegetation and land in the area thereby a direct impact on the micro-climate [22] .
2.2. Image and Pre-Processing
Landsat cloud-free imageries were acquired from the NASA web site which
comprised of the Thematic Mapper (TM), Enhance Thematic Mapper plus (ETM+) image and the operational land Imager (OLI) to determine LST within Calabar Metropolis between “2002 and 2016”. The imageries downloaded covered a period of 15 years at an interval of 2 years. The software employed for desktop analysis was ArcGIS. Identifying the study area was the first step of this research which was achieved with the use of an administrative map of Calabar, showing Calabar Municipality and Calabar South LGA.
2.3. Retrieving of Land Surface Temperature
Land surface temperature was estimated using various procedures which range from radiometric calibration, conversion of DN to radiance, correction for atmospheric absorption, re-emission and surface emissivity which has been used in [23] as described below:
Conversion of Digital Numbers (DN) of the bands to Spectral Radiance
(1)
where,
LMAX = the spectral radiance that is scaled to QCALMAX in W/(m2 * sr * μm) LMIN = the spectral radiance that is scaled to QCALMIN in W/(m2 * sr * μm) QCALMAX = the maximum quantized calibrated pixel value (corresponding to LMAX) in DN = 255 QCALMIN = the minimum quantized calibrated pixel value (corresponding to LMIN) in DN = 1.
Conversion from Spectral Radiance to At-Satellite Brightness Temperature [23]
(2)
where, T = At-satellite brightness temperature, Ll = Spectral radiance (gotten from equations - and -), K1 = Band specific thermal conversion constant from the metadata, x is the thermal band number), K2 = Band specific thermal conversion constant from the metadata, −273.15 = Constant for conversion from Kelvin to Degrees Celsius as shown in [23] .
Correcting for Land Surface Emissivity (LSE) [23]
The temperature values obtained using Equation (2) are reference to a blackbody. Therefore, corrections for spectral emissivity (ε) became necessary according to the nature of land cover (Equation (3))
(3)
where, e = Land Surface Emissivity, 0.004 & 0.986 = Constants for emissivity estimation, PV = Proportion of vegetation [23] given by the equation
(4)
where, NDVI = Normalized Differential Vegetation Index as computed with Equation (1) for each of the years, NDVImin = Minimum value of NDVI for that year, NDVImax = Maximum value of NDVI for that year [23] .
Estimation of the Land Surface Temperature [23]
(5)
where, LST= Land Surface Temperature, BT = At-satellite brightness temperature, W = Wavelength of emitted radiance (µm) [23] given as:
(6)
h = Planck’s constant (
), S = Boltzmann constant (
), C = Velocity of light (
), e = LSE.
3 Result Presentation and Discussion
Land Surface Temperature (LST) Analysis
Based on the LST retrieval algorithm mentioned earlier, seven LST maps at an interval of two years (2002 to 2016) were generated to measure the magnitude and to quantify LST spatially explicit over the whole study area. In order to display the LST map clearly, the density slice function of ArcGIS was used to distinguish the LST zones by different colors. The LST over Calabar metropolis was studied from the analysis of Landsat images of the investigated years (2002, 2006, 2008, 2010, 2012, 2014 and 2016). The results of the LST imagery were classified using standard deviation. LST for the different years was also extracted and presented in degree Celsius (Figure 2 and Table 1).
The result of the LST maps revealed a great variation in the surface radiant temperature for the selected periods (Figure 2 and Table 1). Comparing radiant temperature for the selected periods we observed that, in 2002, the radiant temperature is confined within the range of 14.19˚C to 31.4˚C with mean of 25.32 ˚C; while the radiant temperature of 2006 falls within the range of 18.77˚C to 30.52˚C with a mean of 23.76˚C. Also, in 2008, the radiant temperature falls within the range of 18.92˚C to 32.14˚C with a mean of 24.63˚C while the radiant temperature of 2010 falls within the range of 14.18˚C to 24.77˚C, with 18.72˚C as the mean. The result also revealed a great variation in the mean LST for 2008, 2006 and 2002. Comparing mean LST of 2008 with 2002 and 2006, we observed a slight negative difference of −0.69˚C and a positive difference of 1.26˚C in 2002 and 2006 respectively (Table 1).
Table 1. LST change status of Calabar Metropolis (2002-2016).
Furthermore, the result of the LST map of 2012 reveals the highest mean radiant temperature in 2012 to be 30.25˚C, followed by 21.12˚C with a mean of 25.07˚C, higher than that of 2010. In 2014, radiant temperature falls within the range of 17.64˚C to 30.00˚C with a mean of 23˚C (Table 1). The result of the 2014 LST map further revealed the mean LST of 2014 to be higher than the mean LST of 2010, but lower than the other years understudy. Comparing mean LST of 2014 and 2012, we observed that mean LST in 2012 was higher than 2014 (Table 1).
From the findings of this study, it is evident that, the highest mean radiant of 25.38˚C was observed in 2016, followed by 2002 with mean LST of 25.32˚C, while the least radiant temperature was observed in 2010 (Table 1). The low mean value of the radiant temperature in 2010 compared to the other years can be attributed to the adverse weather condition such as dust haze and fog reported by [24] , during the months of January to March, November to December 2010, dry north easterly winds prevailed over parts of West Africa as a result of surface pressure built up over the Sahara deserts and Sahel region which transported air borne dust particles southward, thus, reducing the horizontal visibility to less than 1000 m.
The findings of this study also demonstrated that, out of the five land use classes identified in the study area (water body, sparse vegetation, dense vegetation, built up area and bare land) [25] , built-up and bare land LULC classes exhibited the highest mean LST values. The mean LST value of 32.14˚C was observed around the bareland class while the lowest radiant temperature of 14.19˚C was observed around the water body classes (Table 1).
4. Conclusion
This study has demonstrated that, Land Surface Temperature (LST) values have grown from the 2002 extent to the 2016 size and their spatial extent is getting larger as urbanization intensifies. The result revealed that the built-up area was the land use category that was significantly linked to high mean and high LST. The study also revealed that the lowest mean LST corresponded to areas covered by water bodies, followed by areas over woodland. The removal of the vegetal cover exposes the land surface to insolation expressed in reflectance that signifies the heating or cool surface systems. The sequence indicates that abundant water is helpful in buffering urban heat islands (UHIS). Vegetation covers should be protected to reduce potential future UHIS around the urban fringe transits through a peri-urban heating system.