<?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.2018.85027</article-id><article-id pub-id-type="publisher-id">OJG-84426</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>
 
 
  MASW Survey with Fixed Receiver Geometry and CMP Cross-Correlation Technique for Data Processing: A Case Study of Wadi Fatima, Western Saudi Arabia
 
</article-title></title-group><contrib-group><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="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>Sherif</surname><given-names>M. El-Hady</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>Faisal</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>Hussein</surname><given-names>M. Harbi</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</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="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Saifur</surname><given-names>Rehman</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>Muhammad</surname><given-names>Kashif</given-names></name><xref ref-type="aff" rid="aff5"><sup>5</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Earthquake Department, National Research Institute of Astronomy and Geophysics, Helwan, Egypt</addr-line></aff><aff id="aff3"><addr-line>Oil and Gas Development Company Limited, Islamabad, Pakistan</addr-line></aff><aff id="aff5"><addr-line>China University of Petroleum (East China), Qingdao, China</addr-line></aff><aff id="aff4"><addr-line>Department of Geophysics, Faculty of Earth Sciences, King Abdulaziz University, Jeddah, KSA</addr-line></aff><aff id="aff1"><addr-line>Department of Earth Sciences, University of Sargodha, Sargodha, Pakistan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mail.faisalrehman@gmail.com(FR)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>05</month><year>2018</year></pub-date><volume>08</volume><issue>05</issue><fpage>463</fpage><lpage>473</lpage><history><date date-type="received"><day>16,</day>	<month>February</month>	<year>2018</year></date><date date-type="rev-recd"><day>7,</day>	<month>May</month>	<year>2018</year>	</date><date date-type="accepted"><day>10,</day>	<month>May</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>
 
 
  Multichannel analysis of surface waves is a noninvasive technique for subsurface shear wave velocity imagining. This method is one of the most effective geophysical tools for geotechnical investigations. In this paper, we present multichannel surface wave data acquisition in a non-conventional manner in alluvium deposits. Fixed receiver and multi-source offset geometry were applied to obtain field data. The data processing comprised of generating CMP cross-correlated traces and then inversion to obtain dispersion curves. The inversion of dispersion curves is achieved by employing a genetic algorithm to obtain subsurface shear wave velocity. Finally, the one-dimensional shear wave models are obtained. The multi-source offset data acquisition with fixed receiver geometry technique in combination with CMP cross-correlation gathers for data processing worked in a quite efficient way to obtain subsurface shear wave model.
 
</p></abstract><kwd-group><kwd>Shallow Geophysics</kwd><kwd> Noninvasive Technique</kwd><kwd> MASW</kwd><kwd> Shear Wave Velocity</kwd><kwd> Genetic Algorithm</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Near surface geophysical techniques and tools are more extensively applied in geological and geotechnical applications. The non invasive nature and rapid data acquisition in cost efficient manner make them an essentially necessary tool to invasive techniques. The multi channel analysis of surface waves (MASW) is one of the near surface geophysics techniques which have seen intensive applications in the geotechnical and engineering geology [<xref ref-type="bibr" rid="scirp.84426-ref1">1</xref>] . Multichannel analysis of surface waves (MASW) has been successfully applied in various shallow geophysical soundings [<xref ref-type="bibr" rid="scirp.84426-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.84426-ref9">9</xref>] . MASW is a rapid and quick methodology to estimate the near surface shear wave velocity (Vs) and overcome more than a few shortcomings of other different techniques which lead to the false impression of phase velocities [<xref ref-type="bibr" rid="scirp.84426-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref12">12</xref>] . Fundamental mode of surface waves is often used, which comprised of the highest energy portion amongst all wave types [<xref ref-type="bibr" rid="scirp.84426-ref13">13</xref>] .</p><p>The arrival time coherency difference is the base for identifying the ground roll on multichannel record. The confidence level on shear wave velocity estimation results can be increased using appropriate data processing methodology [<xref ref-type="bibr" rid="scirp.84426-ref14">14</xref>] . Each wavelength has typical velocity signature, named as phase velocity [<xref ref-type="bibr" rid="scirp.84426-ref15">15</xref>] . There is a fundamental assumption that approximately 92% of ground roll phase velocity is comprised subsurface shear wave velocity [<xref ref-type="bibr" rid="scirp.84426-ref16">16</xref>] . The Rayleigh waves or ground rolls can be produced with impact source like hammer and non impact source like vibrosis. The depth penetration of this type of waves in normal conditions is assumed approximately equal to its wavelength [<xref ref-type="bibr" rid="scirp.84426-ref17">17</xref>] .</p><p>In current study, we applied fixed receiver geometry for MASW data acquisition in alluvial deposits. In conventional MASW technique, we need to move source and receiver positions for each shot. The current study is an attempt to explore the efficiency of fixed receiver geometry for data acquisition and CMP cross-correlation technique for data processing in alluvium deposits. The study area is located in Wadi Fatima, east of Jeddah city, Saudi Arabia (<xref ref-type="fig" rid="fig1">Figure 1</xref>). The Wadi Fatima is one of the distinctive foreland fold-thrust belts in the Arabian-Nubian Shield. The quaternary sediments are comprised of alluvial fillings and fan deposits [<xref ref-type="bibr" rid="scirp.84426-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref18">18</xref>] .</p></sec><sec id="s2"><title>2. Study Area</title><p>The study area is located in the Wadi Fatima. The outcrops rock comprised of Neo-Proterozoic age in the study area. These outcrops (<xref ref-type="fig" rid="fig2">Figure 2</xref>) can be divided into two major lithological units: Fatima group and pre-Fatima basement. The outcrops of pre-Fatima basement include granites, amphibolites, gabbros, andesites and local rhyolitic intrusions. The Fatima group comprised of sedimentary rocks, volcanic rocks and lower greenschist facies. The Wadi fills comprised of moderate to poorly sorted, unconsolidated sand and gravels deposits of tertiary and quaternary age [<xref ref-type="bibr" rid="scirp.84426-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref20">20</xref>] . The Wadi Fatima is a designated as graben structure, commonly termed as Fatima graben having major structural trend NE-SW. Many NW-SE faults dissect Fatima graben. These faults are linked with rifting at Red Sea [<xref ref-type="bibr" rid="scirp.84426-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref21">21</xref>] .</p></sec><sec id="s3"><title>3. Field Survey</title><p>A long receiver array as possible is used in MASW method. Although, the lateral resolution of survey is compromised in longer array, the velocity model provided by the conventional MASW method is averaged over the total length of the spread. A smaller array is more suitable for enhancing lateral resolution [<xref ref-type="bibr" rid="scirp.84426-ref22">22</xref>] . The methodology to acquire data for current survey is similar to conventional MASW Data acquisition; however the receiver’s position was kept fixed. The source offset was increased. The MASW data is collected in 24 points in the study area (<xref ref-type="fig" rid="fig3">Figure 3</xref>). The Geometrics System and 24 vertical geophones with 4.5 Hz frequency are employed to acquire surface wave data. A 16lb sledgehammer was employed as a source of seismic waves. The choice of seismic source which meets the project’s goals and requirements has strong influence on project’s efficiency in shallow seismic surveys. Seismic source selected should be efficient to produce strong signal having specific frequency response [<xref ref-type="bibr" rid="scirp.84426-ref23">23</xref>] . Different offset geometries were applied to acquire 24 MASW profiles summarized in <xref ref-type="table" rid="table1">Table 1</xref>. A land streamer was built for MASW survey with one meter geophone interval using flat metals base connected along flexible Irrigation pipe</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Description of various offset geometries with number of profiles acquired</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sr. No</th><th align="center" valign="middle" >Shot Locations</th><th align="center" valign="middle" >No of Profiles</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >−10, 11.5, 33</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−10, −5, 11.5, 28, 33</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >−12, −6, 11.5, 29, 37</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >−12, −6, 11.5, 29, 35</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >−24, −12, −6, 29, 35, 47</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >−24, −12, −6, 29, 35</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >−30, −24, −12, −6, 29, 35, 47, 53</td><td align="center" valign="middle" >5</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >−30, −24, −12, −6, 29, 35, 47, 53, 59</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >−42, −24, −12, −6, 29, 35, 47, 65</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle"  colspan="2"  >Total Profiles Acquired</td><td align="center" valign="middle" >24</td></tr></tbody></table></table-wrap><p>(PVC HDPE). The amplitude of surface-wave energy acquired in MASW is several times larger than body wave’s energy which is recorded in other seismic waves methods. Thus, pressure contact geophones can be utilized to record surface wave instead of the normally planted geophones. Pressure coupling actually permits the use of towable “land streamers” for MASW surveys, which results in continuous data acquisition. The efficiency of data acquisition is increased greatly as compared to traditional body wave seismic methods [<xref ref-type="bibr" rid="scirp.84426-ref24">24</xref>] .</p><p>Figures 4(a)-(c) are a field photographs demonstrating the procedure adopted for MASW data acquisition. It started with laying down the streamer along the location of surveyed profile, assigning the shots locations using zero distance from first channel (<xref ref-type="table" rid="table1">Table 1</xref>). Each shot location comprised of 5 stacks recorded in a single file in the recording unit (<xref ref-type="fig" rid="fig4">Figure 4</xref>(b)). After finishing the acquisition for all shots, the streamer was dragged by car to next location (<xref ref-type="fig" rid="fig4">Figure 4</xref>(c)). The major objective is to test various offset geometries in different alluvial deposits and the effectiveness of cross-correlation CMP gathers processing technique in this environment.</p></sec><sec id="s4"><title>4. Data Processing and Results</title><p>The Common Midpoint (CMP) cross-correlation gathers for MASW data is a known technique with good estimation and accuracy of phase velocity. The CMP stacked gathers are utilized to obtain surface wave dispersion curve [<xref ref-type="bibr" rid="scirp.84426-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref27">27</xref>] . The most vital step is shear wave’s velocity reconstruction in 1D by means of dispersion curve inversion [<xref ref-type="bibr" rid="scirp.84426-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref29">29</xref>] . The inversion can be achieved by many methods like Genetic Algorithms [<xref ref-type="bibr" rid="scirp.84426-ref30">30</xref>] and/or least-squares approach [<xref ref-type="bibr" rid="scirp.84426-ref31">31</xref>] .</p><sec id="s4_1"><title>4.1. Common Mid-Point Cross-Correlation (CMPCC)</title><p>In case of MASW, the surface wave analysis package of SeisImager 4.2 version is utilized for data processing and inversion. Common mid-point (CMP) cross-</p><p>correlation gathers of MASW data are generated. This technique furnishes much better estimation and accuracy of phase-velocity curves. Data acquisition procedure for this technique is identical to acquisition of seismic refraction data. The CMP gathers are generated after calculation for cross correlation of the original waveform [<xref ref-type="bibr" rid="scirp.84426-ref32">32</xref>] . <xref ref-type="fig" rid="fig5">Figure 5</xref>(a) is example of shot gather acquired in the field. The basic scheme applied in this current study to generate CCCMP gathers is as follows: First, in each shot record, cross-correlation of each pair of traces is carried out. Second, correlation traces with identical CMPs are collected, and then traces with equal spacing are stacked in time domain. The resultant cross correlated gathers are referred as CMP cross-correlation gathers (<xref ref-type="fig" rid="fig5">Figure 5</xref>(b)). The Phase velocity dispersion plots from CMP cross correlation gathers are generated by applying multi-channel analysis (<xref ref-type="fig" rid="fig5">Figure 5</xref>(c)). Finally the genetic algorithm is utilized to obtain inversion of dispersion curves.</p></sec><sec id="s4_2"><title>4.2. Genetic Algorithm</title><p>Genetic Algorithms (GA) are these days well known for geophysical data inversion. The GA philosophy is fast, exact, stable, and has numerous favorable circumstances over the other ordinary procedures [<xref ref-type="bibr" rid="scirp.84426-ref33">33</xref>] . The genetic algorithm is based on Darwin‘s theory of evolution, in which likely solution is achieved [<xref ref-type="bibr" rid="scirp.84426-ref34">34</xref>] . The GA uses selection, crossover and mutation, the three fundamental operators of biological evolution process [<xref ref-type="bibr" rid="scirp.84426-ref35">35</xref>] . Geophysical parameters analogous to biological operators are wave speed, subsurface layer’s thicknesses and the densities</p><p>of these layers. The relative confidence on the inversion procedure can be altogether expanded for GA by utilizing most suitable initial input model [<xref ref-type="bibr" rid="scirp.84426-ref30">30</xref>] . Many scientist successfully applied GA effectively for inversion operations in geophysical Methods e.g., [<xref ref-type="bibr" rid="scirp.84426-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.84426-ref37">37</xref>] . The surface wave inversion carried out by GA calculation requires the minimum information [<xref ref-type="bibr" rid="scirp.84426-ref29">29</xref>] . The procedure is steady and exact, having different points of interest judged next to conventional methodologies. The best fits for calculated and observed dispersion curve is provided by genetic algorithm (<xref ref-type="fig" rid="fig5">Figure 5</xref>). The dispersion curves inversion is carried out to obtain 1D shear wave velocity profile. The shear wave’s velocity is presented by averaging the inverted dispersion curves velocity profiles at the center of MASW profile (<xref ref-type="fig" rid="fig6">Figure 6</xref>).</p></sec></sec><sec id="s5"><title>5. Discussion and Conclusion</title><p>The MASW data were acquired in Wadi Fatima, Jeddah, Saudi Arabia. Total 24 MASW profiles were acquired. CMP cross-correlated gather was generated and 1D shear wave velocities were obtained. Each profile was processed through CMP gathers generation, stacking of CMP gathers, generation of dispersion curves and finally by inverting those to obtain a 1D shear wave velocity model. Finally averaging was carried out for each velocity model obtained by inversion dispersion curves. The average velocity (1D) profile was assumed to the representative velocity at the center of each MASW profile obtained CMP stacks. The data acquisition with fixed receiver and multi-offset geometry reliably worked well in fluvial sediments. This technique provides a quicker way to acquire data in less accessible areas.</p></sec><sec id="s6"><title>Cite this paper</title><p>Rehman, F., El-Hady, S.M., Faisal, M., Harbi, H.M., Ullah, M.F., Rehman, S. and Kashif, M. 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