<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JGIS</journal-id><journal-title-group><journal-title>Journal of Geographic Information System</journal-title></journal-title-group><issn pub-type="epub">2151-1950</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jgis.2020.125031</article-id><article-id pub-id-type="publisher-id">JGIS-103810</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Predicting of Land Surface Temperature Distribution in Freetown City, Sierra Leone by Using Polynomial Curve Fitting Model
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Elhadi</surname><given-names>K. Mustafa</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guoxiang</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abubakr</surname><given-names>Hassan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohamed</surname><given-names>A. Damos</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Musa</surname><given-names>Tarawally</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>School of Resources and Environment, University of Electronic Science and Technology of China, Chengdu, China</addr-line></aff><aff id="aff1"><addr-line>Department of Surveying and Geo-Informatics, Faculty of Geosciences and Environmental Engineering, Southwest Jiaotong University, Chengdu, China</addr-line></aff><pub-date pub-type="epub"><day>10</day><month>09</month><year>2020</year></pub-date><volume>12</volume><issue>05</issue><fpage>531</fpage><lpage>544</lpage><history><date date-type="received"><day>20,</day>	<month>September</month>	<year>2020</year></date><date date-type="rev-recd"><day>27,</day>	<month>October</month>	<year>2020</year>	</date><date date-type="accepted"><day>30,</day>	<month>October</month>	<year>2020</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Global warming has attracted much concern about the worldwide organization, civil society groups, researchers, and so forth because the worldwide surface temperature has been expanding. This investigation intends to assess and compare the ability of a combination of land cover indices to predict the future distribution of land surface temperatures in Freetown using the Polynomial model analysis. Landsat satellite images of 1988, 1998, 2000, 2010, and 2018 of the Freetown Metropolitan zone were utilized for analysis. The investigation had adopted two land covers indices, Modification of normalized difference water index and Urban Index (UI) (e.g., MNDWI and UI) and applied a multi regression equation for forecasting the future LST. The stimulation results propose that the development will be accompanied by surface temperature increases, especially in Freetown’s western urban area. The temperature prevailing in the west of the metropolitan area may increase in the city somewhere in the range 
  from
   1988 to 2018. Additionally, the results of the LST prediction show that the model is perfect. Our discoveries can be represented as a helpful device for policymakers and community awareness by giving a scientific basis for sustainable urban planning and management.
 
</p></abstract><kwd-group><kwd>Global Warming</kwd><kwd> Land Surface Temperature</kwd><kwd> Polynomial Curve Fitting</kwd><kwd> Land Cover Indices</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The urban heat island (UHI) impact shows a higher air and land surface temperature (LST) in urban regions in contrast with the encompassing rural area, generated by high levels of near-surface energy emission, solar radiation absorption of ground objects, and low rates of evapotranspiration [<xref ref-type="bibr" rid="scirp.103810-ref1">1</xref>]. This is as a result of urbanization and overpopulation. These have resulted in most important human activities, creating enormous impacts on the ecosystem at the local, regional, and global scales. It includes converting natural land surfaces into anthropogenic impervious surfaces due to the introduction of low and high albedo materials, which may lead to dramatic climate changes; consequently, an urban climate is warming systematically since the last decades. Such heat rise and warming can be embraced by numerous biophysical well-being intricacies like heat stress, air contamination, and other well-being-related issues [<xref ref-type="bibr" rid="scirp.103810-ref2">2</xref>]. In recent years, studies have proved that the developed area and bare land accelerate UHI’s impact, though green space and water diminish the UHI intensity [<xref ref-type="bibr" rid="scirp.103810-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.103810-ref4">4</xref>]. Therefore, it is essential to study the prediction of land surface distribution [<xref ref-type="bibr" rid="scirp.103810-ref5">5</xref>]. This is a very vital in urban areas of developing countries that are experiencing an increase in land surface temperature, which may result in adverse climate and related factors. Studies have been confined to few cities in Africa, mainly in Ikom city in Nigeria, Harare metropolitan city in Zimbabwe. For example, Muduako et al., 2016 reported that LST in an urban area is one factor associated with urban heat rise and microclimatic warming within a city [<xref ref-type="bibr" rid="scirp.103810-ref6">6</xref>]. Mushore et al., 2017 documented that urban growth will increase warming and result in future high temperatures unless mitigation efforts are strengthened [<xref ref-type="bibr" rid="scirp.103810-ref7">7</xref>]. To the best of our knowledge, little work has been implemented to predict land surface distribution in Freetown, Sierra Leone, and quantify the implication of land surface temperature. Freetown is a coastal city with a rapid growth in urbanization, and such factor is expected to affect the increase in surface temperature. Such a study is vital both given quantifying the effects of expansion on lower tropospheric temperature and in developing knowledge on growth implications on future climate and thermal comfort on urban residents. Space-borne remote sensing has the benefit of simultaneously observing over large areas enabling spatial analysis and direct comparison in space. Remote sensing satellites such as Landsat have many benefits, including large stores of archival data and continuous improvements in data quality over time. For example, Landsat has archival data dating as far back as 1972, making it an important data source for detecting land surface changes over long periods. This paper used space-borne multi-spectral Landsat imagery to predict the future land surface temperature in Freetown city in Sierra Leone from 2018 to 2026.</p></sec><sec id="s2"><title>2. Materials and Method</title><sec id="s2_1"><title>2.1. Study Area</title><p>Study area Freetown is the first capital of Sierra Leone (<xref ref-type="fig" rid="fig1">Figure 1</xref>) that lies between latitude 8˚05'N and 8˚30'N and extends between longitudes 12˚50'W and 13˚20'W. It is the major port city on the Atlantic Ocean. It is located in the</p><p>western area of Sierra Leone. Freetown experiences a tropical climate with a rainy season from May to October and a dry season from November to April. The yearly average minimum temperature for Freetown is around 23.8˚C, while the average maximum temperature is 29.9˚C. annual mean minimum temperature [<xref ref-type="bibr" rid="scirp.103810-ref8">8</xref>]. The topography of Freetown is undulated. Elevation ranges between 100 m and 700 m, with slopes exceeding 50 m above sea level. The prevailing winds are the southwest monsoon during the wet season and the northeastern harmattan, a dust-laden wind from the Sahara Desert during the dry season. The red-bordered areas (study areas) are a rapidly developing area.</p></sec><sec id="s2_2"><title>2.2. Data Used</title><p>This study uses cloud-free and geometrically corrected Landsat imagery from the Earth Resources Observation and Science (EROS) center through the United States Geological Survey (USGS) Global Visualization Viewer, map projection of the collected satellite images is Universal Transverse Mercator (UTM) within Zone 28 N—Datum World Geodetic System (WGS) 84 (<xref ref-type="table" rid="table1">Table 1</xref>). Various software packages were utilized because each one has strength in some operations needed for this study.</p></sec><sec id="s2_3"><title>2.3. Image Preprocessing</title><p>Landsat satellite images (Landsat 5 TM and Landsat 8 OLI/TIRS) with metadata (MTL) file for the study area were utilized for assessing land surface temperature (LST). The satellite images obtained are processed by a set of pre-processing procedures. The pre-processing in clouded radiometric calibration, atmospheric</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Image information will be used in the study</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sensor information</th><th align="center" valign="middle"  colspan="9"  >Image information</th></tr></thead><tr><td align="center" valign="middle" >Date (dd-mm-yy)</td><td align="center" valign="middle" >Resolution</td><td align="center" valign="middle"  colspan="2"  >Path/row</td><td align="center" valign="middle"  colspan="2"  >Bands</td><td align="center" valign="middle"  colspan="2"  >Source</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Landsat4/5 TM</td><td align="center" valign="middle" >26.12.1988</td><td align="center" valign="middle"  colspan="2"  >30,120 m</td><td align="center" valign="middle"  colspan="2"  >202/54</td><td align="center" valign="middle"  colspan="2"  >3, 5, 7, 6</td><td align="center" valign="middle"  colspan="2"  >Usgs.gov</td></tr><tr><td align="center" valign="middle" >Landsat4/5 TM</td><td align="center" valign="middle" >09.3.1998</td><td align="center" valign="middle"  colspan="2"  >30,120 m</td><td align="center" valign="middle"  colspan="2"  >202/54</td><td align="center" valign="middle"  colspan="2"  >3, 5, 7, 6</td><td align="center" valign="middle"  colspan="2"  >Usgs.gov</td></tr><tr><td align="center" valign="middle" >Landsat4/5 TM</td><td align="center" valign="middle" >03.2.2000</td><td align="center" valign="middle"  colspan="2"  >30,120 m</td><td align="center" valign="middle"  colspan="2"  >202/54</td><td align="center" valign="middle"  colspan="2"  >3, 5, 7, 6</td><td align="center" valign="middle"  colspan="2"  >Usgs.gov</td></tr><tr><td align="center" valign="middle" >Landsat4/5 TM</td><td align="center" valign="middle" >22.2.2010</td><td align="center" valign="middle"  colspan="2"  >30,120 m</td><td align="center" valign="middle"  colspan="2"  >202/54</td><td align="center" valign="middle"  colspan="2"  >3, 5, 7, 6</td><td align="center" valign="middle"  colspan="2"  >Usgs.gov</td></tr><tr><td align="center" valign="middle" >Landsat8 OLI_TIRS</td><td align="center" valign="middle" >12.2.2018</td><td align="center" valign="middle"  colspan="2"  >30,100 m</td><td align="center" valign="middle"  colspan="2"  >202/54</td><td align="center" valign="middle"  colspan="2"  >4, 6, 7, 10</td><td align="center" valign="middle"  colspan="2"  >Usgs.gov</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>correction (dark-object subtraction) using the Envi 5.3 and geometrical distortions correction. After the pre-processing procedure, the satellite images are again re-sampled with pixel sizes of 30 &#215; 30 m for all bands which also includes the thermal band. As referenced before 30 m goals resolution reflective bands of Land-sat images obtained from various seasons were piled up into a single multi-band record for the categorization.</p></sec><sec id="s2_4"><title>2.4. LST Recoupment from the Information in Thermal Infrared Data</title><p>In the proposed research, a mean thermal infrared image containing digital numbers was analyzed every year through computing 2 images collected in each month using LST based procedures that were proposed by [<xref ref-type="bibr" rid="scirp.103810-ref9">9</xref>]. The procedure suggested involves 1) transformation of digital number data contained inside Landsat images to radiance, 2) transformation of radiance into temperature of blackbody and 3) blackbody temperature due to brightness into temperature of land surface (emissivity correction). Adopted from [<xref ref-type="bibr" rid="scirp.103810-ref10">10</xref>] emissivity mapping of land surface was calculated using NDVI.</p><sec id="s2_4_1"><title>2.4.1. Transformation of the Digital Number (DN) to Spectral Radiance</title><p>As shown in equation no. 1 which is considered by [<xref ref-type="bibr" rid="scirp.103810-ref11">11</xref>], data gathered from digital numbers are transformed to spectral radiance. Data from digital numbers are of the TIR bands of ETM+ and TM5 images for individual years. Then the use of Equation no. (2) thermal infrared images of Landsat 8were transformed considering the standard of USGS.</p><p>L λ = L min + L max − L min Q C A L max − Q C A L min ( D N − Q C A L min ) (1)</p><p>= M L &#215; Q c a l + A L (2)</p><p>In Equations (1) and (2), L<sub>λ</sub> denotes spectral radiance in W/(m<sup>2</sup>srμm) gained by the sensor found from each pixel from the Landsat imagery. Band specific multiplicative is denoted by ML and rescaling factors which are gathered from MTL image file are found to be additive and is denoted using the term by AL. DN of each image and maximum DN is represented by Q<sub>cal</sub> and QCAL<sub>max</sub>. The value of Qcal and QCAL<sub>max</sub> for the 16-bit Landsat 8 is 65535 and for other Landsat missions is 255 respectively. QCAL<sub>min</sub> is the least DN (0). Radiances from top of the atmosphere (TOA) are denoted as L<sub>max</sub> and L<sub>min</sub> that are scaled to QCAL<sub>max</sub> and QCAL<sub>min</sub> in W/(m<sup>2</sup>srμm), respectively.</p></sec><sec id="s2_4_2"><title>2.4.2. Calculation Brightness Temperature of Blackbody Using Spectral Radiance</title><p>With the use of Equation (3) the radiant images were transformed into temperature detected in blackbody [<xref ref-type="bibr" rid="scirp.103810-ref12">12</xref>].</p><p>T b = K 2 ln { ( K 1 L λ ) + 1 } (3)</p><p>In the above Equation brightness temperature in Kelvin unit is measured using sensor which is denoted with T<sub>b</sub>, spectral radiance in W/(m<sup>2</sup> srμm) is denoted with L<sub>λ</sub> and through image MTL file prelaunch calibration constants in Kelvin unit is obtained. These are represented as K<sub>1</sub> and K<sub>2</sub>. Error in measurement of surface temperature can arise during the execution process due to detection of earth as a blackbody because of its brightness [<xref ref-type="bibr" rid="scirp.103810-ref12">12</xref>]. To minimize these error values, emissivity correction is performed to attain land surface temperature (LST) from Tb using Equation (4), [<xref ref-type="bibr" rid="scirp.103810-ref13">13</xref>].</p></sec><sec id="s2_4_3"><title>2.4.3. Retrieval of Surface Emissivity (ε)</title><p>A threshold method was suggested by [<xref ref-type="bibr" rid="scirp.103810-ref14">14</xref>] to achieve land surface emissivity from Normalized Difference Vegetation Index (NDVI) threshold method. If NDVI &lt; 0.2 then pixels are acknowledged as barren land. The emissivity of these barren lands was derived from red spectral region. If NDVI &gt; 0.5 then pixels are acknowledged as lands thoroughly covered with plants or agricultural fields and its emissivity value was estimated to be 0.99 [<xref ref-type="bibr" rid="scirp.103810-ref10">10</xref>]. When NDVI value lies between the range of 0.2 to 0.5 then pixels are acknowledged as partially covered with vegetation. Using Equation (4) the emissivity is obtained.</p><p>ε = ε v P v + ε s ( 1 − P v ) + Δ ε (4)</p><p>where ε v the emissivity of vegetation coverage, ε s is the soil surface emissivity and, P v is computed to obtain the proportion of vegetation using Equation (5).</p><p>[ NDVI − NDVI s NDVI v − NDVI s ] 2 (5)</p><p>where NDVI s is the NDVI value of pure soil and NDVI v is the NDVI values of pure vegetation derived from NDVI image. Δ ε in Equation (7) indicates distribution of the land surfaces according to its geometry in addition to its the internal reflection. The value of internal reflection is very low for the ordinary and uniform surfaces [<xref ref-type="bibr" rid="scirp.103810-ref10">10</xref>]. The value of internal reflection is however found to be 2% for rough and heterogeneous surface. Δ ε is calculated using Equation (6)</p><p>( 1 − ε s ) ( 1 − P v ) F ε v (6)</p><p>where shape factor is denoted by F. The mean value for different land surfaces according to its distributions based on its geometry is assumed as 0.5.</p><p>Summarizing Equation (5) and Equation (6), the final equation to calculate emissivity estimation is given as Equation (7).</p><p>ε = m P v + n (7)</p><p>where m and n co-efficient are calculated as below in Equation (8):</p><p>m = ε v − ε s − ( 1 − ε s ) F ε v and n = ε s + ( 1 − ε s ) F ε v (8)</p></sec><sec id="s2_4_4"><title>2.4.4. Brightness Temperature to LST</title><p>LST = T b 1 + { λ T b ( K ρ ) &#215; ln ε } (9)</p><p>In the above Equation (9), wavelength of emitted radiance (11.5 μm) [<xref ref-type="bibr" rid="scirp.103810-ref11">11</xref>] is represented by λ, ρ = hc/σ [<xref ref-type="bibr" rid="scirp.103810-ref15">15</xref>], K is the Stefan–Boltzmann’s constant, h is the Planck’s constant, velocity of light (2.998 &#215; 10<sup>8</sup> ms<sup>−1</sup>) by c and surface emissivity by ε. Finally, the derived LST values were converted to the conventional Degree Celsius (˚C) unit by adding the absolute zero which is approximately minus 273.15˚C. Finally retrieve the (LST) as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec></sec><sec id="s2_5"><title>2.5. Simulation of LST Distribution in Freetown Using Land Cover Indices</title><sec id="s2_5_1"><title>2.5.1. Computation Indices for Land Surfaces of Urban and Vegetation Areas</title><p><xref ref-type="table" rid="table2">Table 2</xref> involves urban indices and indices of vegetation. These were estimated through a digital number of measured bands. As recently referenced, the ultimate objective is to investigate the superiority in a relationship's characteristics with the surface temperature. In addition to this to perceive indices with highest grounded capacity for assessing temperature of surfaces of urban areas, a couple of indices were tried. Simulating LST using polynomial curve fitting was shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Derivation of urban and vegetation indices from Landsat data</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Derivation of Indices</th><th align="center" valign="middle"  colspan="3"  >Urban and Vegetation Indices</th></tr></thead><tr><td align="center" valign="middle" >Index</td><td align="center" valign="middle" >Computation</td><td align="center" valign="middle" >Ref</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Normalized Difference Built-up Index (NDBI)</td><td align="center" valign="middle" >NDBI = WIR 1 + NIR / WIR 1 + NIR</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.103810-ref16">16</xref>]</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >Urban Index (UI)</td><td align="center" valign="middle" >UI = WIR 2 + NIR / WIR 2 + NIR</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.103810-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >Normalized Difference Vegetation Index (NDVI)</td><td align="center" valign="middle" >NDVI = NIR − RED / NIR + RED</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.103810-ref18">18</xref>]</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >Modified Normalized Difference Water Index (MNDWI)</td><td align="center" valign="middle" >NDWI = GREEN − NIR / GREENNIR</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.103810-ref19">19</xref>]</td></tr></tbody></table></table-wrap></sec><sec id="s2_5_2"><title>2.5.2. Correlation Analyses between LST and Indices</title><p>Evaluating temperatures of land surfaces with the use of various factors requires high value of correlation between the predictor variables and temperature measured at land surfaces, with no inter-factor show evaluation of indices for quality assessment of correlation with LST. The indices that exceptionally correlate with LST were chosen and applied to develop a linear regression model in order to analyze future temperatures of land surfaces. To analyze the relation between land cover indices (e.g., UI, MNDWI, NDVI and NDBI) and the LST for each of the periods multiple linear regression models are designed. The investigation outputs demonstrate statistically significant correlations which are valid for an entire year [<xref ref-type="bibr" rid="scirp.103810-ref5">5</xref>]. Land cover indices and LST values were mined from each pixel in the designated area of study for individual point data type in order to achieve this objective. These points were utilized to calibrate the linear regression model [<xref ref-type="bibr" rid="scirp.103810-ref20">20</xref>]. The model offers a general idea about the correlation between LST and LULC indices. This realization is relatively coherent with those narrated by other earlier researches [<xref ref-type="bibr" rid="scirp.103810-ref21">21</xref>].</p></sec><sec id="s2_5_3"><title>2.5.3. Polynomial Curve Fitting for Land Use Land Cover Indices Prediction</title><p>The Land Use Land Cover Indices for 26.12.1988, 9.3.1998, 3.2.2000, 22.2.2010, and 12.2.2018 for the same seasons were the input variable in the polynomial curve fitting [<xref ref-type="bibr" rid="scirp.103810-ref13">13</xref>] to map future state of the indices for 2010 and 2018, Similarly, the Land Use Land Cover Indices 22.2.2010 and 12.2.2018 was used in polynomial curve fitting analysis to predict the state of the Land Use Land Cover Indices in 2026, as shown below:</p><p>[ m ∑ x i ∑ x i 2 ⋯ ∑ x i n ∑ x i ∑ x i 2 ∑ x i 3 ⋯ ∑ x i n + 1 ∑ x i 2 ∑ x i 3 ∑ x i 4 ⋯ ∑ x i n + 2 ⋮ ⋮ ⋮ ⋱ ⋮ ∑ x i n ∑ x i n + 1 ∑ x i n + 2 ⋯ L ∑ x i 2 n ] [ p 1 p 2 p 3 ⋮ p n + 1 ] = [ ∑ y i ∑ x i y i ∑ x i 2 y i ⋮ ∑ x i n y i ]</p><p>Curve fitting over m pairs of data ( x 1 , y 1 ) , ( x 2 , y 2 ) , ⋯ , ( x m , y m ) is a process of obtaining a polynomial regression between the two pairs as follows: p ( x ) = P 1 x n + P 2 x n − 1 + ⋯ + P n x + P n + 1 ; where, p ( x ) is a curve fitting of data pairs; p 1 , p 2 , ⋯ , p n + 1 are the model variables, and the x 1 , ⋯ , x n are the n inputs variables. These input variables have a dependency on the possible data available across. Through the current study, the unknown parameters are found using the least square method. At last Land Use Land Cover Indices predictions were converted into land surface temperature distributions for 2010, 2018 and 2026 in the same seasons through multiple linear regression analysis functions.</p></sec><sec id="s2_5_4"><title>2.5.4. Prediction Accuracy Assessment for LST</title><p>The proposed method is applied to forecast temperature of land surfaces for the year 2016 and its rate of accuracy in predicting was measured through Mean Absolute Percentage error. [MAPE]—Equation (10)—(Owen, Carlson et al. 1998).</p><p>MAPE % = 1 N ∑ i = 1 N | ( T predicted − T observed ) / T observed | ∗ 100 (10)</p><p>where: the modeled surface temperature and the actual land surface temperature recorded from Landsat data for the ith pixel is denoted by T<sub>predictedand</sub> T<sub>observed</sub>. Root Mean Square Error and ration RMSE/std can also be regarded as the measure for calculating accuracy of the prediction model in forecasting temperature. Land surface temperature distribution for the period from 2026 is then found using the prediction model after the accuracy assessment.</p></sec></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Monitoring and Assessing LST Changes</title><p>The LST maps of Free Town in 1988, 1998, 2000, 2010 and 2018 are illustrated in <xref ref-type="fig" rid="fig3">Figure 3</xref> and the descriptive statistics of the retrieved LST values are summarized in <xref ref-type="table" rid="table3">Table 3</xref>. In 12/12/1988, the LST ranged from 17.11˚C to 30.83˚C with an average 21.23˚C, in 09.3.1998, the LST ranged from 17.93˚C to 31.72˚C with a mean 23.94˚C. in 03.2.2000, the LST ranged from 18.38˚C to 32.05˚C with an average 23.28˚C. in 2010, the LST ranged from 20.6˚C 2 to 33.5˚C 6 with a mean 25.25˚C. in 2018, the LST ranged from 20.61˚C to 34.51˚C with a mean 26.72˚C. From these data, the highest LST was in 2018 and the lowest LST in 1988. The LST was increased from one year to another due to development of human activities and climatic change. The high levels of LST were concentrated in the northern parts</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Descriptive statistics of LST for different times</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Statistics Information</th><th align="center" valign="middle"  colspan="4"  >Descriptive statistics of LST</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >YEAR</td><td align="center" valign="middle" >Mean</td><td align="center" valign="middle" >Min</td><td align="center" valign="middle" >Max</td><td align="center" valign="middle" >St</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >26.12.1988</td><td align="center" valign="middle" >21.23</td><td align="center" valign="middle" >17.11</td><td align="center" valign="middle" >30.83</td><td align="center" valign="middle" >1.97</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >09.3.1998</td><td align="center" valign="middle" >23.94</td><td align="center" valign="middle" >17.93</td><td align="center" valign="middle" >31.72</td><td align="center" valign="middle" >2.41</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >03.2.2000</td><td align="center" valign="middle" >23.28</td><td align="center" valign="middle" >18.38</td><td align="center" valign="middle" >32.05</td><td align="center" valign="middle" >1.92</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >22.2.2010</td><td align="center" valign="middle" >25.25</td><td align="center" valign="middle" >20.62</td><td align="center" valign="middle" >33.56</td><td align="center" valign="middle" >2.39</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >12.2.2018</td><td align="center" valign="middle" >26.72</td><td align="center" valign="middle" >20.61</td><td align="center" valign="middle" >34.51</td><td align="center" valign="middle" >2.94</td></tr></tbody></table></table-wrap><p>of the study area. When surface temperature increases, the amount of NDVI value decreases. This is the most common behavior found in grassland and sparse vegetation areas.</p></sec><sec id="s3_2"><title>3.2. Retrieval of Surface Temperature from the Land Use Land Cover Indices</title><p>This technique of using temperature forecast to estimate LST pattern to model and estimate UHI is one such contribution of this study. As presented in <xref ref-type="table" rid="table4">Table 4</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref>, For the Polynomial curve fitting analysis of land surface temperature distribution the Urban Index (UI) and Modification of normalized difference water index (MNDWI) were chosen as the predictors [<xref ref-type="bibr" rid="scirp.103810-ref5">5</xref>]. The regression model was tested on an independent Landsat information acquired in February 2010 and February 2018 and the model nearly resembled like the temperature patterns (<xref ref-type="fig" rid="fig5">Figure 5</xref>, <xref ref-type="fig" rid="fig6">Figure 6</xref>). Based on the Information acquired from independent Landsat in 2018 Regression model was tested. Temperature redeemed from UI and MNDWI based on their direct relation to thermal infrared information (Band 10) of Landsat 8. Based on 161 points samples over the inspected region, the UI and MNDWI forecasted surface temperature with advanced correctness (mean relative rate percentage 5.88%, and 4.41% with root mean square error 1.61˚C, 1.31˚C and ration RMSE/std are 0.5 and 0.44 for 2010 and 2018 respectively.</p></sec><sec id="s3_3"><title>3.3. Predicted Temperature Distribution in Freetown up to the Year 2026</title><p>The rising temperature patterns observed between 2000 and 2018 may proceed through 2026 (<xref ref-type="table" rid="table5">Table 5</xref>) and <xref ref-type="fig" rid="fig7">Figure 7</xref>. The scope of high-temperature classification (greater than 35˚C) was predicted to increase to the detriment of low-temperature classes. According to LST’s values, the predicted values in 2026 were more than the simulated value in 2018. However, in the predictions for South-eastern regions where low-density residential areas are found were moderately cooler than Northern-eastern regions where high-density residential areas are found. Predictions demonstrate that land surface temperatures underneath 32˚C will possibly stay common in the northern half, where low and medium density residential is found. Besides, expecting that development patterns observed between 2000 and 2018 endure, the extension would high-density built-up areas would bring about high surface temperatures (over 35˚C) in eastern regions, such as in high-density residential areas. It is worth noting that the LST expanded for all land cover types.</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Correlation analysis of LST vs. Difference Indies 1988, 1998, 2000, 2010 and 2018</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Correlation analysis</th><th align="center" valign="middle"  colspan="5"  >LST vs. Difference Indies</th></tr></thead><tr><td align="center" valign="middle" >Year</td><td align="center" valign="middle" >Indices</td><td align="center" valign="middle" >Multi Linear regression</td><td align="center" valign="middle" >R</td><td align="center" valign="middle" >R<sup>2</sup></td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1988</td><td align="center" valign="middle" >MNDWI UI</td><td align="center" valign="middle" >LST = 7.65*UI + 3.13*MNDWI + 25.1</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >0.80</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1998</td><td align="center" valign="middle" >MNDWI UI</td><td align="center" valign="middle" >LST = 16.7*UI − 6.56*MNDWI + 28.12</td><td align="center" valign="middle" >0.91</td><td align="center" valign="middle" >0.83</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2000</td><td align="center" valign="middle" >MNDWI UI</td><td align="center" valign="middle" >LST = 14.9*UI − 5.68*MNDWI + 27.01</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >0.78</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >2010</td><td align="center" valign="middle" >MNDWI UI</td><td align="center" valign="middle" >LST = 12.4*UI − 4.84*MNDWI + 28.32</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.81</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2018</td><td align="center" valign="middle" >MNDWI UI</td><td align="center" valign="middle" >LST = 24.9*UI − 44.7*MNDWI + 29.11</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.84</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Descriptive statistics of LST for different times</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Statistics Information</th><th align="center" valign="middle"  colspan="4"  >Descriptive statistics of LST</th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" >YEAR</td><td align="center" valign="middle" >Mean</td><td align="center" valign="middle" >Min</td><td align="center" valign="middle" >Max</td><td align="center" valign="middle" >St</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >26.12.1988</td><td align="center" valign="middle" >21.23</td><td align="center" valign="middle" >17.11</td><td align="center" valign="middle" >30.83</td><td align="center" valign="middle" >1.97</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >09.3.1998</td><td align="center" valign="middle" >23.94</td><td align="center" valign="middle" >17.93</td><td align="center" valign="middle" >31.72</td><td align="center" valign="middle" >2.41</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >03.2.2000</td><td align="center" valign="middle" >23.28</td><td align="center" valign="middle" >18.38</td><td align="center" valign="middle" >32.05</td><td align="center" valign="middle" >1.92</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >22.2.2010</td><td align="center" valign="middle" >25.25</td><td align="center" valign="middle" >20.62</td><td align="center" valign="middle" >33.56</td><td align="center" valign="middle" >2.39</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >12.2.2018</td><td align="center" valign="middle" >26.72</td><td align="center" valign="middle" >20.61</td><td align="center" valign="middle" >34.51</td><td align="center" valign="middle" >2.94</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >2026</td><td align="center" valign="middle" >27.5</td><td align="center" valign="middle" >23.1</td><td align="center" valign="middle" >35.6</td><td align="center" valign="middle" >3.2</td></tr></tbody></table></table-wrap></sec></sec><sec id="s4"><title>4. Conclusions and Outlook</title><p>The investigation aims to forecast future distribution of land surface temperatures in Freetown utilizing the Polynomial curve fitting analysis. The research used two land cover indices (e.g., MNDWI and UI) and implemented a multi-regression equation to predict future LST. We declare that the Urban Index (UI) and (MNDWI) predicted surface temperature with high accuracy (mean relative rate percentage 5.88%, 4.41%, and root mean square error 1.63˚C, 1.31˚C, and ration RMSE/std are 0.5 and 0.44 for 2010 and 2018 respectively). Urban expansion development will be accompanied by surface temperature increments, especially in Freetown’s western metropolitan area. The temperature that dominates the west urban region may increase in the city between 2000 and 2018 may proceed through 2026. For example, different factors, such as effective mitigation procedures and changes in city development policies, can impact surface temperature patterns. By and large, this study’s discoveries underscore the significance of medium resolution satellite information in foreseeing future surface temperatures in urban settings. However, there is a need for future studies to explore the feasibility of these methods and techniques at national or regional spatial levels.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Mustafa, E.K., Liu, G.X., Hassan, A., Damos, M.A. and Tarawally, M. (2020) Predicting of Land Surface Temperature Distribution in Freetown City, Sierra Leone by Using Polynomial Curve Fitting Model. Journal of Geographic Information System, 12, 531-544. https://doi.org/10.4236/jgis.2020.125031</p></sec></body><back><ref-list><title>References</title><ref id="scirp.103810-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Buyantuyev, A. and Wu, J. 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