<?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">OJG</journal-id><journal-title-group><journal-title>Open Journal of Geology</journal-title></journal-title-group><issn pub-type="epub">2161-7570</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojg.2018.810060</article-id><article-id pub-id-type="publisher-id">OJG-87521</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>
 
 
  AQUA Satellite Data and Imputation of Geopotential Height: A Case Study for Pakistan
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Usman</surname><given-names>Saleem</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>Mian</surname><given-names>Sohail Akram</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muhammad</surname><given-names>Fahad Ullah</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Faisal</surname><given-names>Rehman</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muhammad</surname><given-names>Riaz Khan</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Departments of Earth Sciences, University of Sargodha, Sargodha, Pakistan</addr-line></aff><aff id="aff4"><addr-line>Pakistan Meteorological Department, Flood Forecasting Division, Lahore, Pakistan</addr-line></aff><aff id="aff1"><addr-line>Provincial Disaster Management Authority, Project Implementation Unit Punjab, Lahore,</addr-line></aff><aff id="aff2"><addr-line>Institute of Geology, University of the Punjab, Lahore, Pakistan</addr-line></aff><pub-date pub-type="epub"><day>19</day><month>09</month><year>2018</year></pub-date><volume>08</volume><issue>10</issue><fpage>1002</fpage><lpage>1018</lpage><history><date date-type="received"><day>13,</day>	<month>August</month>	<year>2018</year></date><date date-type="rev-recd"><day>23,</day>	<month>September</month>	<year>2018</year>	</date><date date-type="accepted"><day>26,</day>	<month>September</month>	<year>2018</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>
 
 
  In current study an attempt is carried out by filling missing data of geopotiential height over Pakistan and identifying the optimum method for interpolation. In last thirteen years geopotential height values over were missing over Pakistan. These gaps are tried to be filled by interpolation Techniques. The techniques for interpolations included Bilinear interpolations [BI], Nearest Neighbor [NN], Natural [NI] and Inverse distance weighting [IDW]. These imputations were judged on the basis of performance parameters which include Root Mean Square Error [RMSE], Mean Absolute Error [MAE], Correlation Coefficient [Corr] and Coefficient of Determination [R
  <sup>2</sup>]. The NN and IDW interpolation Imputations were not precise and accurate. The Natural Neighbors and Bilinear interpolations immaculately fitted to the data set. A good correlation was found for Natural Neighbor interpolation imputations and perfectly fit to the surface of geopotential height. The root mean square error [maximum and minimum] values were ranges from &#177;5.10 to &#177;2.28 m respectively. However mean absolute error was near to 1. The validation of imputation revealed that NN interpolation produced more accurate results than BI. It can be concluded that Natural Interpolation was the best suited interpolation technique for filling missing data sets from AQUA satellite for geopotential height.
 
</p></abstract><kwd-group><kwd>AIRX3STML</kwd><kwd> Missing Data Imputations</kwd><kwd> Missing Climatic Data</kwd><kwd> Upper Air Temperature</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Missing data is a big problem encountered at a number of times during environmental research [<xref ref-type="bibr" rid="scirp.87521-ref1">1</xref>][<xref ref-type="bibr" rid="scirp.87521-ref2">2</xref>][<xref ref-type="bibr" rid="scirp.87521-ref3">3</xref>][<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>]. A lot of causes such as routine maintenances, sampling errors in satellite sensor, failures of satellite sensor during observations, meteorological abnormalities and human errors are responsible for the discontinuity of data set [<xref ref-type="bibr" rid="scirp.87521-ref3">3</xref>][<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>]. Geopotential height is the height of a pressure surface in the atmosphere above mean sea level [MSL]. The geopotential height data gathered from AQUA satellite contains incomplete data matrices in 24 standard pressures levels [<xref ref-type="bibr" rid="scirp.87521-ref5">5</xref>]. A research can become inaccurate if missing data sets are used [<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>][<xref ref-type="bibr" rid="scirp.87521-ref6">6</xref>]. Geopotential height was the function of air temperature, pressure, winds, and topography of the area, which required a careful method for its imputations. One of the oldest and most suggested methods to fill this missing information was replacing mean values of neighbor samples [<xref ref-type="bibr" rid="scirp.87521-ref1">1</xref>][<xref ref-type="bibr" rid="scirp.87521-ref2">2</xref>][<xref ref-type="bibr" rid="scirp.87521-ref3">3</xref>].</p><p>Many different interpolation techniques have been developed [<xref ref-type="bibr" rid="scirp.87521-ref2">2</xref>][<xref ref-type="bibr" rid="scirp.87521-ref6">6</xref>][<xref ref-type="bibr" rid="scirp.87521-ref7">7</xref>][<xref ref-type="bibr" rid="scirp.87521-ref8">8</xref>][<xref ref-type="bibr" rid="scirp.87521-ref9">9</xref>]. The best method depends upon the spatial and temporal variations of geopotential height in the atmosphere. Shen, Reiter [<xref ref-type="bibr" rid="scirp.87521-ref10">10</xref>], applied different interpolations on geopotential height keeping in view its variations in the atmosphere. Knox, Higuchi [<xref ref-type="bibr" rid="scirp.87521-ref11">11</xref>]investigate secular variations, Shabbar, Higuchi [<xref ref-type="bibr" rid="scirp.87521-ref12">12</xref>]did regional analysis, Griesser, Br&#246;nnimann [<xref ref-type="bibr" rid="scirp.87521-ref13">13</xref>]reconstructed geopotential height for 850, 700, 500, 300, 200 and 100 hPa. White [<xref ref-type="bibr" rid="scirp.87521-ref14">14</xref>]calculated statistics and climatology for the Northern Hemisphere’s geopotential height over 1000 and 500 hPa. Wallace, Zhang [<xref ref-type="bibr" rid="scirp.87521-ref15">15</xref>]investigated intera-decadal variability and teleconnections in the Northern hemisphere’s geopotential height over 500 and 700 hPa respectively.</p><p>Pakistan is the central country of South Asia bordered with India to East, China in North, South to Arabian Sea and Afghanistan to West (<xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref>). It is arid to semi-arid country except in the north areas which received annual rainfall of 760 mm to 2000 mm annually. Pakistan has four provinces, of which Baluchistan is the driest and desert area facing 210 mm of rain averagely [<xref ref-type="bibr" rid="scirp.87521-ref16">16</xref>]. 3/4<sup>th</sup> area of the country is getting no more than 250 mm of rain annually. In summer season relative humidity remains between 20% and 50%. In winter average temperature varies from 4˚C to 20˚C in most areas, while an increasing temperature of 0.6˚C to 1.0˚C is found along the coastal areas [<xref ref-type="bibr" rid="scirp.87521-ref17">17</xref>].</p><p>The actual thrust of this research work is to devise a workable methodology for carrying out scientific observations of upper atmosphere meteorology in Pakistan in spite of lacking modern equipment and technological resources in relevant departments. The published literature is not available in Pakistan, however, Saleem and Ahmed [<xref ref-type="bibr" rid="scirp.87521-ref18">18</xref>]; Saleem [<xref ref-type="bibr" rid="scirp.87521-ref19">19</xref>]; Saleem [<xref ref-type="bibr" rid="scirp.87521-ref20">20</xref>]are few initiatives on upper-level atmospheric observations.</p></sec><sec id="s2"><title>2. Material and Methods</title><sec id="s2_1"><title>2.1. Data Used</title><p>In this research, the monthly mean of geopotential height [in meters]for the past 13 years, obtained from Atmospheric Infrared Sounder [AIRS]level 3, was used. AIRS was the instrument on AQUA satellite, which launched in May 2002.</p><p>This satellite has very high spectral resolutions: e.g., it captures climate data through nearly 2382 bands in the electromagnetic spectrum and its geopotential height product is very high resolution 0.5˚ &#215; 0.5˚ grid cell. Version 6 of its product contains fewer biases in geopotential height [<xref ref-type="bibr" rid="scirp.87521-ref5">5</xref>]. Besides good quality of climate data, GESDISC<sup>1</sup> provides geopotential height data for the whole global.</p></sec><sec id="s2_2"><title>2.2. Spatial Interpolations of Missing Geopotential Height</title><p>Randomly 30% of the 324 samples were missing data which were then estimated from the 70% known data using different interpolation techniques like IDW, NN, BI and NI [<xref ref-type="bibr" rid="scirp.87521-ref2">2</xref>][<xref ref-type="bibr" rid="scirp.87521-ref7">7</xref>]. Robeson [<xref ref-type="bibr" rid="scirp.87521-ref21">21</xref>]; Price, McKenney [<xref ref-type="bibr" rid="scirp.87521-ref22">22</xref>]; Perry and Hollis [<xref ref-type="bibr" rid="scirp.87521-ref7">7</xref>]; Yozgatligil, Aslan [<xref ref-type="bibr" rid="scirp.87521-ref3">3</xref>]considered these performance parameters like, Mean Absolute Error [MAE], Root Mean Square Error [RMSE], Coefficient of Determinations [R<sup>2</sup>]and Correlation Coefficient [Corr], to find out the best interpolation technique for missing climatic data set.</p><p>1) INVERSE DISTANCE WEIGHTING</p><p>This imputation resembles to Tobler’s first law of geography in which the weight of the known samples will be determined based on the distances from the imputed sample [Robeson, 1994]. More will be the distance of neighbors from a predicted sample less will be their weight in interpolation. Ferrari and Ozaki [<xref ref-type="bibr" rid="scirp.87521-ref9">9</xref>]used Equation (1) which is given below:</p><p>z i j = ∑ a = 1 n z o a d a   j − r ∑ a = 1 n d a   j − r (1)</p><p>where d a j − r is the weighting factor of distance between the a<sup>th</sup> original neighbor sample z o i , z i j is j<sup>th</sup> the point to be estimated, n is the total number of the sample used, and r weighting factor. Langella [<xref ref-type="bibr" rid="scirp.87521-ref23">23</xref>], formula for IDW was used in the missing data imputations.</p><p>2) NEAREST NEIGHBORS INTERPOLATION [NN]</p><p>Missing values were directly imputed with a most suitable neighbor around the missing sample [<xref ref-type="bibr" rid="scirp.87521-ref24">24</xref>][<xref ref-type="bibr" rid="scirp.87521-ref25">25</xref>]in this interpolation technique.</p><p>3) BILINEAR INTERPOLATION [BI]</p><p>Junninen et al. [<xref ref-type="bibr" rid="scirp.87521-ref2004">2004</xref>]used Equations (2) and (3) for Bilinear Interpolations</p><p>z i = z i 1   + m ( z o + z o 1 ) (2)</p><p>m = z i 2 − z i 1 z o 2 − z o 1 z o 1 &lt; z o &lt; z o 2     and     z i 1   &lt; z i &lt; z i 2 (3)</p><p>It was a linear equation with ( z o 1 ,   z I 1 ) and ( z o 2 ,   z i 2 ) sample values, m being a gradient of this line.</p><p>4) NATURAL NEIGHBORS INTERPOLATION [NI]</p><p>This spatial interpolation gives the nearest neighbor value of the sample to the missing geopotential height. D. and Boissonnat and Cazals [<xref ref-type="bibr" rid="scirp.87521-ref25">25</xref>]explain the selection of such natural neighbors for randomly missing data being on Delaunay triangulation.</p></sec><sec id="s2_3"><title>2.3. Performance Indicators for Interpolations</title><p>These following performance parameters have been frequently used by Robeson [<xref ref-type="bibr" rid="scirp.87521-ref21">21</xref>]; Price, McKenney [<xref ref-type="bibr" rid="scirp.87521-ref22">22</xref>]; Junninen, Niska [<xref ref-type="bibr" rid="scirp.87521-ref2">2</xref>]; Perry and Hollis [<xref ref-type="bibr" rid="scirp.87521-ref7">7</xref>]; Stahl, Moore [<xref ref-type="bibr" rid="scirp.87521-ref24">24</xref>]; Norazian [<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>]; Ferrari and Ozaki [<xref ref-type="bibr" rid="scirp.87521-ref9">9</xref>]; Saleem and Ahmed [<xref ref-type="bibr" rid="scirp.87521-ref18">18</xref>]for imputation of missing climate data set.</p><p>1) ROOT MEAN SQUARE ERROR [RMSE]</p><p>Root Mean Square was calculated by dividing the sum of the square of the difference between imputed geopotential heights and actual value with the total number of samples, and then finally taking the square root of this term [<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>]. Smaller values indicate a perfect estimation of missing data set. Equation (4) was its mathematical formula used in this research.</p><p>R M S E = ( 1 n ∑ a = 1 n [ z o a   − z i a ] 2 ) 1 2 (4)</p><p>This parameter calculates the total difference [&#177;]between original and interpolated geopotential height.</p><p>2) MEAN ABSOLUTE ERROR [MAE]</p><p>This provides more information about the residual error as compared with RMSE. Junninen, Niska [<xref ref-type="bibr" rid="scirp.87521-ref2">2</xref>]and Norazian [<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>]provided Equation (5) for MAE.</p><p>M A E = 1 n ∑ a = 1 n | z a i   − z i a | (5)</p><p>MAE value range from 0 to ∞ . Its value close to 1 indicates more accurate and perfect imputation of missing data set.</p><p>3) CORRELATION COEFFICIENT [Corr]</p><p>Its value of +1 indicates very strong correlation and near to 0 signifies a bad correlation between actual and predicted geopotential height. Equation (6) was used for the correlation coefficient in this research.</p><p>c o r r   =     cov ( z i   , z o ) ∂ z i ∂ z O (6)</p><p>In Equation (6) nominator represents covariance while denominator represents the product of their standard deviations in the data set.</p><p>4) COEFFICIENT OF DETERMINATION [R<sup>2</sup>]</p><p>This parameter provides a degree of correlation between the actual and predicted sample geopotential height [<xref ref-type="bibr" rid="scirp.87521-ref1">1</xref>]which varies between 0 and 1. Noor, Abdullah [<xref ref-type="bibr" rid="scirp.87521-ref4">4</xref>], suggested values closer to 1 indicate a perfect fit for the data set. Rahman and Islam, [<xref ref-type="bibr" rid="scirp.87521-ref2011">2011</xref>]used the following formula for R<sup>2</sup>.</p><p>R 2 = [ 1 n   ∑ a = 1 n ( z i a − A i ) ( z o a − A o ) ∂ z i ∂ z o ] (7)</p><p>In Equation (7), A<sub>i</sub> was the average of predicted samples and A<sub>o</sub> is the average of sample values before prediction.</p></sec></sec><sec id="s3"><title>3. Results</title><p>These were the results of the performance parameter for each interpolation technique.</p><sec id="s3_1"><title>3.1. Performance Parameters from IDW</title><p>On all pressure level IDW showed very biased results. IDW produced highest RMSE &#177; 14.45 m over 1 hPa while lowest value of this error was &#177;3.66 m at 925 hPa. Actual and predicted values indicating low quality of interpolation for missing values of geopotential height with IDW as correlation coefficient was very low (<xref ref-type="table" rid="table1">Table 1</xref>).</p></sec><sec id="s3_2"><title>3.2. Performance Parameters from Nearest Neighbor Interpolation</title><p>RMSE value remains between &#177;4.925 and &#177;11.369 m with Nearest Neighbor Interpolations. Such a large RMSE, poor correlation, and poor fit to the surface indicated bad refilling of data with this interpolation technique (<xref ref-type="table" rid="table2">Table 2</xref>).</p></sec><sec id="s3_3"><title>3.3. Performance Parameters from Bilinear Interpolation</title><p>Bilinear Interpolation appeared to be relatively better as compared to the above mentioned two interpolations. RMSE was &#177;2.461 to &#177;5.241 m in refilling of gaps in data up to 1000 hPa. MAE remains less than 1 and strong correlation (0.98) was found in the imputation of geopotential height. Coefficient of Determination was close to 0.98 for imputation over 1, 1.5, 2, 3, 5, 7, 10, 15, 70, 100, 150, 200, 250, 300 hPa (<xref ref-type="table" rid="table3">Table 3</xref>).</p></sec><sec id="s3_4"><title>3.4. Performance Parameters from Natural Neighbor Interpolation</title><p>Reasonable low RMSE come in refilling of geopotential height over 2, 3, 5, 7, 30, 50, 70, 200, 250, 400, 500, 600 hPa. Largest RMSE was &#177;5.10 m at 10 hPa and lowest RMSE &#177;2.2 m for refilling of gaps in data at 850, 925, 1000 hPa. A good correlation coefficient [near to 0.99]was come in the refilling of geopotential height. R<sup>2</sup> was near to 1 concluding a good line of fit between actual and predicted data set (<xref ref-type="table" rid="table4">Table 4</xref>).</p></sec></sec><sec id="s4"><title>4. Discussions</title><p>Refilling of geopotential height over 24 pressure levels was good with Bilinear and Natural Neighbor Imputations (Tables 1-4). In order to nominate optimum interpolation from both of them, scatter plots of original and estimated geopotential heights were investigated. Poor data refilling was come in February and March (<xref ref-type="fig" rid="fig3">Figure 3</xref>(a)).</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Results indicating poor performance parameters with Inverse Distance Weighting Interpolation</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Pressure Level</th><th align="center" valign="middle" >RMSE</th><th align="center" valign="middle" >AME</th><th align="center" valign="middle" >Correlation</th><th align="center" valign="middle" >R<sup>2</sup></th></tr></thead><tr><td align="center" valign="middle" >1 hPa</td><td align="center" valign="middle" >5.241294</td><td align="center" valign="middle" >1.673678</td><td align="center" valign="middle" >0.994263</td><td align="center" valign="middle" >0.982482</td></tr><tr><td align="center" valign="middle" >1.5 hPa</td><td align="center" valign="middle" >4.727445</td><td align="center" valign="middle" >1.538098</td><td align="center" valign="middle" >0.992346</td><td align="center" valign="middle" >0.978878</td></tr><tr><td align="center" valign="middle" >2 hPa</td><td align="center" valign="middle" >5.144201</td><td align="center" valign="middle" >1.546157</td><td align="center" valign="middle" >0.992445</td><td align="center" valign="middle" >0.978924</td></tr><tr><td align="center" valign="middle" >3 hPa</td><td align="center" valign="middle" >4.216421</td><td align="center" valign="middle" >1.403774</td><td align="center" valign="middle" >0.992625</td><td align="center" valign="middle" >0.979272</td></tr><tr><td align="center" valign="middle" >5 hPa</td><td align="center" valign="middle" >4.258006</td><td align="center" valign="middle" >1.303426</td><td align="center" valign="middle" >0.988246</td><td align="center" valign="middle" >0.970826</td></tr><tr><td align="center" valign="middle" >7 hPa</td><td align="center" valign="middle" >3.712901</td><td align="center" valign="middle" >1.191135</td><td align="center" valign="middle" >0.991712</td><td align="center" valign="middle" >0.977557</td></tr><tr><td align="center" valign="middle" >10 hPa</td><td align="center" valign="middle" >4.406922</td><td align="center" valign="middle" >1.25975</td><td align="center" valign="middle" >0.988496</td><td align="center" valign="middle" >0.971253</td></tr><tr><td align="center" valign="middle" >15 hPa</td><td align="center" valign="middle" >4.131028</td><td align="center" valign="middle" >1.198271</td><td align="center" valign="middle" >0.989455</td><td align="center" valign="middle" >0.973121</td></tr><tr><td align="center" valign="middle" >20 hPa</td><td align="center" valign="middle" >4.807294</td><td align="center" valign="middle" >1.359347</td><td align="center" valign="middle" >0.985551</td><td align="center" valign="middle" >0.965473</td></tr><tr><td align="center" valign="middle" >30 hPa</td><td align="center" valign="middle" >4.615745</td><td align="center" valign="middle" >1.272488</td><td align="center" valign="middle" >0.975812</td><td align="center" valign="middle" >0.948054</td></tr><tr><td align="center" valign="middle" >50 hPa</td><td align="center" valign="middle" >4.481513</td><td align="center" valign="middle" >1.24537</td><td align="center" valign="middle" >0.978242</td><td align="center" valign="middle" >0.952734</td></tr><tr><td align="center" valign="middle" >70 hPa</td><td align="center" valign="middle" >4.001382</td><td align="center" valign="middle" >1.207328</td><td align="center" valign="middle" >0.989019</td><td align="center" valign="middle" >0.97236</td></tr><tr><td align="center" valign="middle" >100 hPa</td><td align="center" valign="middle" >3.815742</td><td align="center" valign="middle" >1.206655</td><td align="center" valign="middle" >0.996643</td><td align="center" valign="middle" >0.987169</td></tr><tr><td align="center" valign="middle" >150 hPa</td><td align="center" valign="middle" >3.96526</td><td align="center" valign="middle" >1.236372</td><td align="center" valign="middle" >0.99677</td><td align="center" valign="middle" >0.987438</td></tr><tr><td align="center" valign="middle" >200 hPa</td><td align="center" valign="middle" >4.67426</td><td align="center" valign="middle" >1.333385</td><td align="center" valign="middle" >0.998104</td><td align="center" valign="middle" >0.990057</td></tr><tr><td align="center" valign="middle" >250 hPa</td><td align="center" valign="middle" >4.395547</td><td align="center" valign="middle" >1.319586</td><td align="center" valign="middle" >0.996534</td><td align="center" valign="middle" >0.986976</td></tr><tr><td align="center" valign="middle" >300 hPa</td><td align="center" valign="middle" >4.593847</td><td align="center" valign="middle" >1.33011</td><td align="center" valign="middle" >0.995398</td><td align="center" valign="middle" >0.98474</td></tr><tr><td align="center" valign="middle" >400 hPa</td><td align="center" valign="middle" >4.281792</td><td align="center" valign="middle" >1.23829</td><td align="center" valign="middle" >0.991174</td><td align="center" valign="middle" >0.976463</td></tr><tr><td align="center" valign="middle" >500 hPa</td><td align="center" valign="middle" >4.30804</td><td align="center" valign="middle" >1.212168</td><td align="center" valign="middle" >0.983423</td><td align="center" valign="middle" >0.961512</td></tr><tr><td align="center" valign="middle" >600 hPa</td><td align="center" valign="middle" >4.509835</td><td align="center" valign="middle" >1.3308</td><td align="center" valign="middle" >0.980018</td><td align="center" valign="middle" >0.954683</td></tr><tr><td align="center" valign="middle" >700 hPa</td><td align="center" valign="middle" >4.140531</td><td align="center" valign="middle" >1.158596</td><td align="center" valign="middle" >0.97152</td><td align="center" valign="middle" >0.938137</td></tr><tr><td align="center" valign="middle" >850 hPa</td><td align="center" valign="middle" >2.461281</td><td align="center" valign="middle" >0.770069</td><td align="center" valign="middle" >0.981623</td><td align="center" valign="middle" >0.957836</td></tr><tr><td align="center" valign="middle" >925 hPa</td><td align="center" valign="middle" >2.722891</td><td align="center" valign="middle" >0.795279</td><td align="center" valign="middle" >0.988701</td><td align="center" valign="middle" >0.971507</td></tr><tr><td align="center" valign="middle" >1000 hPa</td><td align="center" valign="middle" >2.52145</td><td align="center" valign="middle" >0.669249</td><td align="center" valign="middle" >0.986646</td><td align="center" valign="middle" >0.968239</td></tr></tbody></table></table-wrap><table-wrap-group id="2"><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Results indicating poor performance indicators from Nearest Neighbor Interpolation</title></caption><table-wrap id="2_1"><table><tbody><thead><tr><th align="center" valign="middle" >Pressure Level</th><th align="center" valign="middle" >RMSE</th><th align="center" valign="middle" >AME</th><th align="center" valign="middle" >Correlation</th><th align="center" valign="middle" >R<sup>2</sup></th></tr></thead><tr><td align="center" valign="middle" >1 hPa</td><td align="center" valign="middle" >11.36953</td><td align="center" valign="middle" >4.694365</td><td align="center" valign="middle" >0.984868</td><td align="center" valign="middle" >0.964135</td></tr><tr><td align="center" valign="middle" >1.5 hPa</td><td align="center" valign="middle" >10.47272</td><td align="center" valign="middle" >4.227424</td><td align="center" valign="middle" >0.981804</td><td align="center" valign="middle" >0.95849</td></tr><tr><td align="center" valign="middle" >2 hPa</td><td align="center" valign="middle" >10.04097</td><td align="center" valign="middle" >4.013124</td><td align="center" valign="middle" >0.978183</td><td align="center" valign="middle" >0.952061</td></tr><tr><td align="center" valign="middle" >3 hPa</td><td align="center" valign="middle" >9.314465</td><td align="center" valign="middle" >3.667933</td><td align="center" valign="middle" >0.97511</td><td align="center" valign="middle" >0.945647</td></tr></tbody></table></table-wrap><table-wrap id="2_2"><table><tbody><thead><tr><th align="center" valign="middle" >5 hPa</th><th align="center" valign="middle" >8.37878</th><th align="center" valign="middle" >3.189218</th><th align="center" valign="middle" >0.974254</th><th align="center" valign="middle" >0.943877</th></tr></thead><tr><td align="center" valign="middle" >7 hPa</td><td align="center" valign="middle" >8.25621</td><td align="center" valign="middle" >3.144038</td><td align="center" valign="middle" >0.975983</td><td align="center" valign="middle" >0.94716</td></tr><tr><td align="center" valign="middle" >10 hPa</td><td align="center" valign="middle" >8.307455</td><td align="center" valign="middle" >3.156482</td><td align="center" valign="middle" >0.972696</td><td align="center" valign="middle" >0.940833</td></tr><tr><td align="center" valign="middle" >15 hPa</td><td align="center" valign="middle" >7.815421</td><td align="center" valign="middle" >2.909444</td><td align="center" valign="middle" >0.976439</td><td align="center" valign="middle" >0.947893</td></tr><tr><td align="center" valign="middle" >20 hPa</td><td align="center" valign="middle" >7.607512</td><td align="center" valign="middle" >2.753404</td><td align="center" valign="middle" >0.969492</td><td align="center" valign="middle" >0.935232</td></tr><tr><td align="center" valign="middle" >30 hPa</td><td align="center" valign="middle" >7.006525</td><td align="center" valign="middle" >2.610512</td><td align="center" valign="middle" >0.969131</td><td align="center" valign="middle" >0.93451</td></tr><tr><td align="center" valign="middle" >50 hPa</td><td align="center" valign="middle" >6.488704</td><td align="center" valign="middle" >2.500665</td><td align="center" valign="middle" >0.9731</td><td align="center" valign="middle" >0.942042</td></tr><tr><td align="center" valign="middle" >70 hPa</td><td align="center" valign="middle" >7.553283</td><td align="center" valign="middle" >2.904254</td><td align="center" valign="middle" >0.97597</td><td align="center" valign="middle" >0.947148</td></tr><tr><td align="center" valign="middle" >100 hPa</td><td align="center" valign="middle" >9.827749</td><td align="center" valign="middle" >4.04727</td><td align="center" valign="middle" >0.983055</td><td align="center" valign="middle" >0.96073</td></tr><tr><td align="center" valign="middle" >150 hPa</td><td align="center" valign="middle" >12.15678</td><td align="center" valign="middle" >5.267926</td><td align="center" valign="middle" >0.988911</td><td align="center" valign="middle" >0.972037</td></tr><tr><td align="center" valign="middle" >200 hPa</td><td align="center" valign="middle" >12.76332</td><td align="center" valign="middle" >5.485841</td><td align="center" valign="middle" >0.988962</td><td align="center" valign="middle" >0.972149</td></tr><tr><td align="center" valign="middle" >250 hPa</td><td align="center" valign="middle" >11.93628</td><td align="center" valign="middle" >5.083785</td><td align="center" valign="middle" >0.986951</td><td align="center" valign="middle" >0.968318</td></tr><tr><td align="center" valign="middle" >300 hPa</td><td align="center" valign="middle" >10.19128</td><td align="center" valign="middle" >4.385436</td><td align="center" valign="middle" >0.988056</td><td align="center" valign="middle" >0.970371</td></tr><tr><td align="center" valign="middle" >400 hPa</td><td align="center" valign="middle" >8.383855</td><td align="center" valign="middle" >3.392052</td><td align="center" valign="middle" >0.977312</td><td align="center" valign="middle" >0.949918</td></tr><tr><td align="center" valign="middle" >500 hPa</td><td align="center" valign="middle" >7.497696</td><td align="center" valign="middle" >2.884847</td><td align="center" valign="middle" >0.967422</td><td align="center" valign="middle" >0.930971</td></tr><tr><td align="center" valign="middle" >600 hPa</td><td align="center" valign="middle" >6.502538</td><td align="center" valign="middle" >2.370197</td><td align="center" valign="middle" >0.958783</td><td align="center" valign="middle" >0.91434</td></tr><tr><td align="center" valign="middle" >700 hPa</td><td align="center" valign="middle" >5.504249</td><td align="center" valign="middle" >1.981821</td><td align="center" valign="middle" >0.950236</td><td align="center" valign="middle" >0.897891</td></tr><tr><td align="center" valign="middle" >850 hPa</td><td align="center" valign="middle" >4.930112</td><td align="center" valign="middle" >1.53327</td><td align="center" valign="middle" >0.940682</td><td align="center" valign="middle" >0.879706</td></tr><tr><td align="center" valign="middle" >925 hPa</td><td align="center" valign="middle" >4.925109</td><td align="center" valign="middle" >1.46762</td><td align="center" valign="middle" >0.96189</td><td align="center" valign="middle" >0.919613</td></tr><tr><td align="center" valign="middle" >1000 hPa</td><td align="center" valign="middle" >5.786711</td><td align="center" valign="middle" >1.375848</td><td align="center" valign="middle" >0.981378</td><td align="center" valign="middle" >0.95728</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap-group id="3"><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Results indicating good performance parameters for refilling of gaps in data with Bilinear Interpolation</title></caption><table-wrap id="3_1"><table><tbody><thead><tr><th align="center" valign="middle" >Pressure Level</th><th align="center" valign="middle" >RMSE</th><th align="center" valign="middle" >AME</th><th align="center" valign="middle" >Correlation</th><th align="center" valign="middle" >R<sup>2</sup></th></tr></thead><tr><td align="center" valign="middle" >1 hPa</td><td align="center" valign="middle" >5.241294</td><td align="center" valign="middle" >1.673678</td><td align="center" valign="middle" >0.994263</td><td align="center" valign="middle" >0.982482</td></tr><tr><td align="center" valign="middle" >1.5 hPa</td><td align="center" valign="middle" >4.727445</td><td align="center" valign="middle" >1.538098</td><td align="center" valign="middle" >0.992346</td><td align="center" valign="middle" >0.978878</td></tr><tr><td align="center" valign="middle" >2 hPa</td><td align="center" valign="middle" >5.144201</td><td align="center" valign="middle" >1.546157</td><td align="center" valign="middle" >0.992445</td><td align="center" valign="middle" >0.978924</td></tr><tr><td align="center" valign="middle" >3 hPa</td><td align="center" valign="middle" >4.216421</td><td align="center" valign="middle" >1.403774</td><td align="center" valign="middle" >0.992625</td><td align="center" valign="middle" >0.979272</td></tr><tr><td align="center" valign="middle" >5 hPa</td><td align="center" valign="middle" >4.258006</td><td align="center" valign="middle" >1.303426</td><td align="center" valign="middle" >0.988246</td><td align="center" valign="middle" >0.970826</td></tr><tr><td align="center" valign="middle" >7 hPa</td><td align="center" valign="middle" >3.712901</td><td align="center" valign="middle" >1.191135</td><td align="center" valign="middle" >0.991712</td><td align="center" valign="middle" >0.977557</td></tr><tr><td align="center" valign="middle" >10 hPa</td><td align="center" valign="middle" >4.406922</td><td align="center" valign="middle" >1.25975</td><td align="center" valign="middle" >0.988496</td><td align="center" valign="middle" >0.971253</td></tr><tr><td align="center" valign="middle" >15 hPa</td><td align="center" valign="middle" >4.131028</td><td align="center" valign="middle" >1.198271</td><td align="center" valign="middle" >0.989455</td><td align="center" valign="middle" >0.973121</td></tr><tr><td align="center" valign="middle" >20 hPa</td><td align="center" valign="middle" >4.807294</td><td align="center" valign="middle" >1.359347</td><td align="center" valign="middle" >0.985551</td><td align="center" valign="middle" >0.965473</td></tr><tr><td align="center" valign="middle" >30 hPa</td><td align="center" valign="middle" >4.615745</td><td align="center" valign="middle" >1.272488</td><td align="center" valign="middle" >0.975812</td><td align="center" valign="middle" >0.948054</td></tr><tr><td align="center" valign="middle" >50 hPa</td><td align="center" valign="middle" >4.481513</td><td align="center" valign="middle" >1.24537</td><td align="center" valign="middle" >0.978242</td><td align="center" valign="middle" >0.952734</td></tr><tr><td align="center" valign="middle" >70 hPa</td><td align="center" valign="middle" >4.001382</td><td align="center" valign="middle" >1.207328</td><td align="center" valign="middle" >0.989019</td><td align="center" valign="middle" >0.97236</td></tr><tr><td align="center" valign="middle" >100 hPa</td><td align="center" valign="middle" >3.815742</td><td align="center" valign="middle" >1.206655</td><td align="center" valign="middle" >0.996643</td><td align="center" valign="middle" >0.987169</td></tr><tr><td align="center" valign="middle" >150 hPa</td><td align="center" valign="middle" >3.96526</td><td align="center" valign="middle" >1.236372</td><td align="center" valign="middle" >0.99677</td><td align="center" valign="middle" >0.987438</td></tr></tbody></table></table-wrap><table-wrap id="3_2"><table><tbody><thead><tr><th align="center" valign="middle" >200 hPa</th><th align="center" valign="middle" >4.67426</th><th align="center" valign="middle" >1.333385</th><th align="center" valign="middle" >0.998104</th><th align="center" valign="middle" >0.990057</th></tr></thead><tr><td align="center" valign="middle" >250 hPa</td><td align="center" valign="middle" >4.395547</td><td align="center" valign="middle" >1.319586</td><td align="center" valign="middle" >0.996534</td><td align="center" valign="middle" >0.986976</td></tr><tr><td align="center" valign="middle" >300 hPa</td><td align="center" valign="middle" >4.593847</td><td align="center" valign="middle" >1.33011</td><td align="center" valign="middle" >0.995398</td><td align="center" valign="middle" >0.98474</td></tr><tr><td align="center" valign="middle" >400 hPa</td><td align="center" valign="middle" >4.281792</td><td align="center" valign="middle" >1.23829</td><td align="center" valign="middle" >0.991174</td><td align="center" valign="middle" >0.976463</td></tr><tr><td align="center" valign="middle" >500 hPa</td><td align="center" valign="middle" >4.30804</td><td align="center" valign="middle" >1.212168</td><td align="center" valign="middle" >0.983423</td><td align="center" valign="middle" >0.961512</td></tr><tr><td align="center" valign="middle" >600 hPa</td><td align="center" valign="middle" >4.509835</td><td align="center" valign="middle" >1.3308</td><td align="center" valign="middle" >0.980018</td><td align="center" valign="middle" >0.954683</td></tr><tr><td align="center" valign="middle" >700 hPa</td><td align="center" valign="middle" >4.140531</td><td align="center" valign="middle" >1.158596</td><td align="center" valign="middle" >0.97152</td><td align="center" valign="middle" >0.938137</td></tr><tr><td align="center" valign="middle" >850 hPa</td><td align="center" valign="middle" >2.461281</td><td align="center" valign="middle" >0.770069</td><td align="center" valign="middle" >0.981623</td><td align="center" valign="middle" >0.957836</td></tr><tr><td align="center" valign="middle" >925 hPa</td><td align="center" valign="middle" >2.722891</td><td align="center" valign="middle" >0.795279</td><td align="center" valign="middle" >0.988701</td><td align="center" valign="middle" >0.971507</td></tr><tr><td align="center" valign="middle" >1000 hPa</td><td align="center" valign="middle" >2.52145</td><td align="center" valign="middle" >0.669249</td><td align="center" valign="middle" >0.986646</td><td align="center" valign="middle" >0.968239</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Good results of performance indicators with Natural Neighbor Interpolation</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Pressure Level</th><th align="center" valign="middle" >RMSE</th><th align="center" valign="middle" >AME</th><th align="center" valign="middle" >Correlation</th><th align="center" valign="middle" >R<sup>2</sup></th></tr></thead><tr><td align="center" valign="middle" >1 hPa</td><td align="center" valign="middle" >4.900104</td><td align="center" valign="middle" >1.64291</td><td align="center" valign="middle" >0.995605</td><td align="center" valign="middle" >0.98512</td></tr><tr><td align="center" valign="middle" >1.5 hPa</td><td align="center" valign="middle" >4.997688</td><td align="center" valign="middle" >1.620178</td><td align="center" valign="middle" >0.993656</td><td align="center" valign="middle" >0.981326</td></tr><tr><td align="center" valign="middle" >2 hPa</td><td align="center" valign="middle" >4.323708</td><td align="center" valign="middle" >1.466286</td><td align="center" valign="middle" >0.99451</td><td align="center" valign="middle" >0.982965</td></tr><tr><td align="center" valign="middle" >3 hPa</td><td align="center" valign="middle" >4.154958</td><td align="center" valign="middle" >1.328781</td><td align="center" valign="middle" >0.990859</td><td align="center" valign="middle" >0.975959</td></tr><tr><td align="center" valign="middle" >5 hPa</td><td align="center" valign="middle" >4.32224</td><td align="center" valign="middle" >1.388351</td><td align="center" valign="middle" >0.990687</td><td align="center" valign="middle" >0.975515</td></tr><tr><td align="center" valign="middle" >7 hPa</td><td align="center" valign="middle" >4.122477</td><td align="center" valign="middle" >1.27077</td><td align="center" valign="middle" >0.991668</td><td align="center" valign="middle" >0.977389</td></tr><tr><td align="center" valign="middle" >10 hPa</td><td align="center" valign="middle" >5.101086</td><td align="center" valign="middle" >1.41484</td><td align="center" valign="middle" >0.986257</td><td align="center" valign="middle" >0.96693</td></tr><tr><td align="center" valign="middle" >15 hPa</td><td align="center" valign="middle" >3.737039</td><td align="center" valign="middle" >1.146604</td><td align="center" valign="middle" >0.992122</td><td align="center" valign="middle" >0.978282</td></tr><tr><td align="center" valign="middle" >20 hPa</td><td align="center" valign="middle" >4.537878</td><td align="center" valign="middle" >1.274444</td><td align="center" valign="middle" >0.977021</td><td align="center" valign="middle" >0.950391</td></tr><tr><td align="center" valign="middle" >30 hPa</td><td align="center" valign="middle" >4.0766</td><td align="center" valign="middle" >1.160489</td><td align="center" valign="middle" >0.988907</td><td align="center" valign="middle" >0.972017</td></tr><tr><td align="center" valign="middle" >50 hPa</td><td align="center" valign="middle" >4.311496</td><td align="center" valign="middle" >1.22233</td><td align="center" valign="middle" >0.984238</td><td align="center" valign="middle" >0.963129</td></tr><tr><td align="center" valign="middle" >70 hPa</td><td align="center" valign="middle" >4.096588</td><td align="center" valign="middle" >1.184038</td><td align="center" valign="middle" >0.985229</td><td align="center" valign="middle" >0.965527</td></tr><tr><td align="center" valign="middle" >100 hPa</td><td align="center" valign="middle" >4.589851</td><td align="center" valign="middle" >1.356172</td><td align="center" valign="middle" >0.991379</td><td align="center" valign="middle" >0.976963</td></tr><tr><td align="center" valign="middle" >150 hPa</td><td align="center" valign="middle" >3.846614</td><td align="center" valign="middle" >1.223615</td><td align="center" valign="middle" >0.997187</td><td align="center" valign="middle" >0.988257</td></tr><tr><td align="center" valign="middle" >200 hPa</td><td align="center" valign="middle" >3.941453</td><td align="center" valign="middle" >1.285059</td><td align="center" valign="middle" >0.997698</td><td align="center" valign="middle" >0.989262</td></tr><tr><td align="center" valign="middle" >250 hPa</td><td align="center" valign="middle" >4.263726</td><td align="center" valign="middle" >1.286571</td><td align="center" valign="middle" >0.997583</td><td align="center" valign="middle" >0.989028</td></tr><tr><td align="center" valign="middle" >300 hPa</td><td align="center" valign="middle" >4.500221</td><td align="center" valign="middle" >1.31535</td><td align="center" valign="middle" >0.995976</td><td align="center" valign="middle" >0.985874</td></tr><tr><td align="center" valign="middle" >400 hPa</td><td align="center" valign="middle" >4.340019</td><td align="center" valign="middle" >1.27953</td><td align="center" valign="middle" >0.991552</td><td align="center" valign="middle" >0.977225</td></tr><tr><td align="center" valign="middle" >500 hPa</td><td align="center" valign="middle" >4.370527</td><td align="center" valign="middle" >1.287437</td><td align="center" valign="middle" >0.984613</td><td align="center" valign="middle" >0.963743</td></tr><tr><td align="center" valign="middle" >600 hPa</td><td align="center" valign="middle" >3.963257</td><td align="center" valign="middle" >1.203221</td><td align="center" valign="middle" >0.983525</td><td align="center" valign="middle" >0.961471</td></tr><tr><td align="center" valign="middle" >700 hPa</td><td align="center" valign="middle" >3.71123</td><td align="center" valign="middle" >1.096937</td><td align="center" valign="middle" >0.976069</td><td align="center" valign="middle" >0.947018</td></tr><tr><td align="center" valign="middle" >850 hPa</td><td align="center" valign="middle" >2.398759</td><td align="center" valign="middle" >0.70676</td><td align="center" valign="middle" >0.983242</td><td align="center" valign="middle" >0.960856</td></tr><tr><td align="center" valign="middle" >925 hPa</td><td align="center" valign="middle" >2.287255</td><td align="center" valign="middle" >0.683341</td><td align="center" valign="middle" >0.991601</td><td align="center" valign="middle" >0.977208</td></tr><tr><td align="center" valign="middle" >1000 hPa</td><td align="center" valign="middle" >2.484222</td><td align="center" valign="middle" >0.706179</td><td align="center" valign="middle" >0.987709</td><td align="center" valign="middle" >0.970155</td></tr></tbody></table></table-wrap><p>The Imputations for months of January, February and March were not precise (over 20, 30, 50, 70, 100, 150, 200, 250 hPa) with Bilinear Interpolation. Bilinear Interpolation for remaining pressure levels accurately filled the gaps in the Geopotential height (<xref ref-type="fig" rid="fig3">Figure 3</xref>(b)).</p><p>The original sample and imputed sample for each months were plotted together to create theses scatter plots. However (over 500, 600, 850, 1000 hPa) Bilinear Interpolation poorly filled months of February, March and April (<xref ref-type="fig" rid="fig3">Figure 3</xref>(c)).</p><p>The similar technique of plotting original samples with imputed samples was used to create scatter plot of each month. Natural Neighbor Interpolation Imputations were more precise than Bilinear Interpolation. Only month of February was not good by Natural Neighbor Interpolation. Natural Neighbor Interpolation precisely filled the Geopotential height (over 1, 1.5, 2, 3, 5, 7, 10 and 15 hPa) (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)). The imputation with NNI for 20 hPa to 250 hPa and 300 hPa to 1000 hPa are illustrated in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) respectively.</p></sec><sec id="s5"><title>5. Conclusion</title><p>AQUA Satellite data was interpolated for Missing Data of Geopotential height. Based on critical checks and evaluation of interpolations regarding their product, it concluded that the NN and IDW interpolations for filling of missing</p><p>geopotential height data were proved not to be best and perfect (<xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>). Good results were found between BI and NI. However, after examining scatter plots of each month, it was found that NI was more accurate and reliable for missing data of geopotential height over 24 hPa levels.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors wish to acknowledge valuable guidance provided by Mr. Thomas Hearty and Mr. Edward T Olsen to refill gaps in AIRS relative humidity data set. The valuable suggestions are appreciated by Mr. Alessio Martion, University of the Rome, La Sapienza Italy which helped to improve this research.</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Saleem, U., Akram, M.S., Ullah, M.F., Rehman, F. and Khan, M.R. (2018) AQUA Satellite Data and Imputation of Geopotential Height: A Case Study for Pakistan. 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