<?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">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1103214</article-id><article-id pub-id-type="publisher-id">OALibJ-72665</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Evaluating the Triaxial Characteristics of Ultamafic Rocks from Central Greece Using the Physical, Dynamic and Mechanical Properties
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Konstantinos</surname><given-names>Diamantis</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>Georges</surname><given-names>Exarhakos</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>George</surname><given-names>Migiros</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>Efthimios</surname><given-names>Gartzos</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Sciences, Division of Geological Science and Atmospheric Environment, Laboratory of Mineralogy-Geology, Agricultural University of Athens, Athens, Greece</addr-line></aff><aff id="aff2"><addr-line>Department of Civil Engineering, Piraeus University of Applied Sciences, Athens, Greece</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>kostasdiam@aua.gr(KD)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>01</day><month>12</month><year>2016</year></pub-date><volume>03</volume><issue>12</issue><fpage>1</fpage><lpage>20</lpage><history><date date-type="received"><day>November</day>	<month>8,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>21,</year>	</date><date date-type="accepted"><day>December</day>	<month>9,</month>	<year>2016</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>
 
 
  Due to the fact that the estimation of the triaxial parameters is very important in any geotechnical project, many attempts have become with the aim of their determination. In spite of its relative simplicity, triaxial tests are time consuming, expensive, and require a large number of well prepared (regularly shaped) rock specimens and suitable testing procedures. For this reason, they cannot be easily determined in rocks which are thinly bedded, highly fractured, weak, and so indirect, fast, practical, easy and economical ways should be used such as the correlation of them with some other characteristics which are calculated easily. The aim of this study is to apply correlation analysis to investigate the relationships between physical, dynamic and mechanical characteristics and triaxial parameters for ultramafic rocks. Thus, sixteen samples, taken from the western part of Othrysmt (ten samples) and the Kallidromomt (six samples, central Greece), were tested and the relations among the properties 
  were described by simple regression analyses. The study reveals strong negative, logarithmic correlations between the effective porosity and triaxial parameters (
  c
  , 
  φ
  ). Positive, linear relationships are also indicated between wave velocities, apparent cohesion and friction angle, while the increase of serpentinization percentage causes decrease of the 
  c
  , 
  φ
  . Both dry unit weight and Schmidt Hammer Values are logarithmically affected with 
  c
  , 
  φ
  . The point load strength index and apparent cohesion and friction angle are strongly correlated by both logarithmic and linear functions, but logarithmic trends present higher determination coefficients.
 
</p></abstract><kwd-group><kwd>Triaxial Tests</kwd><kwd> Apparent Cohesion</kwd><kwd> Friction Angle</kwd><kwd> Ultramafic</kwd><kwd> Correlation</kwd><kwd> Greece</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The construction of geotechnical engineering projects like foundations, rock slopes and underground structures is based on the estimation of the rock mass properties. The determination of the triaxial parameters is very important because the rock-mass properties are estimated through them. Despite of its relative simplicity, triaxial tests are time consuming, expensive, and require a large number of well prepared (regularly shaped) rock specimens and suitabletesting procedures. Some rocks are thinly bedded, highly fractured, weak, present alterations such as ultramafic rocks with the result they are usually not suitable for preparing specimens and the determination of triaxial parameters is very difficult. On the other hand the fact that ultramafic rocks are met in many areas all over the world and especially south-eastern Europe has as a result many engineering geology projects to be constructed on/in them [<xref ref-type="bibr" rid="scirp.72665-ref1">1</xref>] . For the above-mentioned reasons, indirect, reliable, quick, sample and economical ways are necessary to estimate the triaxial parameters for the ultramafic rocks.</p><p>Ultramafic rocks are members of ophiolitic suite rocks which represent remnants of the Earth’s oceanic crust and upper mantle. Basic, hypabyssal and extrusive rocks cover ultramafic rocks. This succession is idealized and in most cases some members may be absent. This research focuses on ultramafic rocks. They include particular types of geological formation with both petrographic variety (harzburgites, lherzolites, plagioclastic peridotites, dunites, etc.) and structural complexity due to tectonic deformation and alteration. This ocean-floor metamorphism (serpentinization) lead to a modification of their petrographic characteristics (serpentinized varieties of them). Thus, they are from massive strong to weak rocks (peridotites and serpentinites, [<xref ref-type="bibr" rid="scirp.72665-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.72665-ref8">8</xref>] ).</p><p>Within the framework of the present study, sixteen ultramafic rocks (six peridotites and ten serpentinites) were taken from the Kallidromomt and the western part of Othrysmt (Central Greece), the dry unit weight (γ<sub>d</sub>), the effective porosity (n<sub>e</sub>), the compressional wave velocity (V<sub>p</sub>), the shear wave velocity (V<sub>s</sub>), the Schmidt Hammer Values (SHV), the point load strength index (I<sub>s</sub><sub>50</sub>) were determined and presented. The Uniaxial Compressive Strength (σ<sub>ci</sub>) and the material constant (m<sub>i</sub>) were estimated by the Hoek and Brown failure criterion and the triaxial characteristics (apparent cohesion, c and friction angle φ) were presented.</p><p>The main objective of this research is was to determine the predictability of apparent cohesion (c) and friction angle (φ) of ultramafic rocks (serpentinites and peridotites) with a simple, fast, practical and economical way through the physical, dynamic and mechanical properties at the preliminary site investigation stage. The results were statistically analyzed using the method of least-squares regression. The relationships among these parameters were described by the best fit equations and the highest correlation coefficient, in each relationship, was also determined. The same samples were subjected to petrographic studies with the aim of describing the main mineralogical composition and the serpentinization percentage of ultramafic rocks.</p></sec><sec id="s2"><title>2. Location and Geology of the Study Area</title><p>The study area is to be found in the central part of Greece (<xref ref-type="fig" rid="fig1">Figure 1</xref>(a)) and specifically</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> (a) Study areas and ophiolitic complexes in Greece; (b) Geologigal map and sampling points of the study area at Othrys Mt; (c) Geologigal map and sampling points of the study area at Kallidromo Mt</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x2.png"/></fig><p>at western part of Othrys Mt. (near the villages of Moschokarya, Mega Isoma, LoutraKaitsas and Domokos, <xref ref-type="fig" rid="fig1">Figure 1</xref>(b)) and at the eastern-southeastern side of Kallidromo Mt (between the villages of Kallidromo, Reginio and Modio, <xref ref-type="fig" rid="fig1">Figure 1</xref>(c)). It belongs to the Sub-Pelagonian geotectonical unit, which is part of the Internal Hellenides and is mainly comprised of Alpine formations ( [<xref ref-type="bibr" rid="scirp.72665-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref12">12</xref>] ). They can be distinguished into:</p><p>1) A carbonate sequence of Triassic-Jurassic age which constitutes the basement of the area.</p><p>2) A tectonic nappe, mainly ophiolitic (volcano-sedimentary formations, basaltic lavas, basic rocks and ultramafic masses, [<xref ref-type="bibr" rid="scirp.72665-ref11">11</xref>] ).</p><p>3) An unconformable sequence of Cretaceous limestones which passes upward to flysch.</p><p>The present study research focuses on ophiolitic sequence and mainly on ultramafic masses. They are mainly represented by the peridotites whose degree of serpentinization varies.</p></sec><sec id="s3"><title>3. Methods and Results</title><sec id="s3_1"><title>3.1. Sample Preparation and Test Procedures</title><p>The data pertains to ultramafic rocks sampled from sixteen sites in the study areas (eleven from Othrys and six from Kallidromo, <xref ref-type="fig" rid="fig1">Figure 1</xref>). The samples were taken from the surface and cylindrical rock specimens for laboratory testing were prepared according [<xref ref-type="bibr" rid="scirp.72665-ref13">13</xref>] requirements. To reduce the uncertainty regarding the influence of the sample size on the measured properties and especially on strength [<xref ref-type="bibr" rid="scirp.72665-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref15">15</xref>] , their diameters range between 53 and 55 mm, the length to diameter ratio was between 2.0 and 2.5 and the edges of the specimens were cut parallel and smooth [<xref ref-type="bibr" rid="scirp.72665-ref13">13</xref>] . After a macroscopical inspection, seventy-four isotropic, homogeneous, unweathered (or slightly weathered) and free of visible joints ultramafic specimens were considered. The dry unit weight and the effective porosity were determined in accordance with [<xref ref-type="bibr" rid="scirp.72665-ref16">16</xref>] . The sound velocities (V<sub>p</sub>, V<sub>s</sub>) were calculated from the travel time with the application of ultrasonic compression wave pulses to the samples in accordance with test designations [<xref ref-type="bibr" rid="scirp.72665-ref17">17</xref>] . Moreover, point load strength index values were determined according to [<xref ref-type="bibr" rid="scirp.72665-ref18">18</xref>] requirements (in sixteen specimens, ten serpentinites and six peridotites) and a Type L Schmidt Hammer was used for the determination of Schmidt Hammer Values. Ten points on each specimen were taken and the mean values were calculated. The Schmidt hammer tests were carried out according to [<xref ref-type="bibr" rid="scirp.72665-ref16">16</xref>] . In addition, the triaxial tests were determined using a Hoek cell according to [<xref ref-type="bibr" rid="scirp.72665-ref19">19</xref>] . Three or four different confining pressures (σ<sub>3</sub>) applied during the triaxial tests (fifty-eight specimens). Range of confining pressures of 0 &lt; σ<sub>3</sub>&lt; 0.5σ<sub>ci</sub>, proposed by [<xref ref-type="bibr" rid="scirp.72665-ref14">14</xref>] , was used. The specimens were first subjected to the required confining pressure and then the axial load was applied until the specimen failed.</p><p>Thin sections, from samples of the sixteen areas, were prepared and examined under the polarizing microscope, at the Mineralogy-Geology Laboratory of the Agricultural University of Athens, with the aim of describing the main mineralogical composition and the serpentinization percentage of ultramafic rocks. Fractures created by the tests, did not follow internal discontinuities and were always fresh. The tests were carried out in dry conditions for a better relation of the results.</p></sec><sec id="s3_2"><title>3.2. Petrographic Properties of Ultramafic Rocks</title><p>The ultramafic rocks include rock types (peridotites) with large variability (harzburgites, lherzolites, plagioclasticperidotites, dunites, etc.), which due to their tectonic deformation and a low grade metamorphism (serpentinization, [<xref ref-type="bibr" rid="scirp.72665-ref20">20</xref>] ) lead to a modification of their petrographic characteristics (serpentinites). Serpentinisation is the transformation of ferromagnesian minerals, olivine in particular, to serpentine, which is a lattice mineral of either fibrous or laminar form. This alteration allows the understanding of the dramatic changes in the behavior of ultramafic rocks, reduces their strength and generally the physical, dynamic and mechanical characteristics [<xref ref-type="bibr" rid="scirp.72665-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.72665-ref8">8</xref>] .</p><p>In this paper, sixteen thin sections were prepared and examined under a polarizing microscope. The studied rock samples are unaltered or slightly serpentinized (serpentinization &lt; 30% by volume) ultramafic rock types, characterized as peridotites and partially to completely serpentinizedperidotites (serpentinization &gt; 70% by volume) called as serpentinites. The investigated peridotites mainly comprised of olivines, ortho and clino pyroxenes which are characterised as parent-primary minerals (P<sub>m</sub> &gt; 74% by volume, <xref ref-type="table" rid="table1">Table 1</xref>).</p><p>When the peridotites are influenced by the serpentinization, they transformed into Serpentinites. Serpentinites are mainly composed of secondary minerals (70% - 92%, by volume, <xref ref-type="table" rid="table1">Table 1</xref>). Serpentine is the major mineral phase (62% - 84% by volume, Table1, [<xref ref-type="bibr" rid="scirp.72665-ref1">1</xref>] ). Also, some other secondary minerals are chlorite, talc and actinolite comprising up to 13%. Thus, the percentage of the remaining parent rock minerals (olivine, pyroxene), is less than 30%. The mean values of serpentinization for peridotites and serpentinites are 9.17% and 79.90% respectively, while the standard deviations are 8.75 and 7.02 respectively (<xref ref-type="table" rid="table2">Table 2</xref>).</p></sec><sec id="s3_3"><title>3.3. Physical, Dynamic and Mechanical Properties</title><p>The dry unit weight (γ<sub>d</sub>) and effective porosity (n<sub>e</sub>) were determinedfor 6 peridotites and 10 serpentinites samples and their values are listed in <xref ref-type="table" rid="table3">Table 3</xref>. The γ<sub>d</sub> and n<sub>e</sub> for peridotites range from 31.67 to 33.17 KN/m<sup>3</sup> and from 0.07 to 0.19 respectively. On the other hand, the values of γ<sub>d</sub> and n<sub>e</sub> for serpentinites fluctuate between 24.95 and 26.79 KN/m<sup>3</sup> and from 0.39 to 3.59 respectively. The serpentinites present lower dry unit weight values and higher effective porosity than peridotites because they are mainly composed of secondary minerals (as it is afore-mentioned) which have lower specific gravity and more voids.</p><p>The compressional wave velocity (V<sub>p</sub>) and shear wave velocity (V<sub>s</sub>), which were determined as above-mentioned in chapter 3.1, are given in <xref ref-type="table" rid="table3">Table 3</xref> as well. The values of V<sub>p</sub> for peridotites and serpentinites fluctuate between 7412 and 7991 m/sec and from 4955 to 5645 m/sec respectively, while the mean values are 7781 m/sec (S.D. 211) and 5361</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Primary minerals, secondary minerals and serpentinization percentage for ultramafic rocks</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample No</th><th align="center" valign="middle"  colspan="5"  >Primary Minerals</th><th align="center" valign="middle"  colspan="4"  >Secondary Minerals</th><th align="center" valign="middle"  rowspan="2"  >Degree of Serpentinization b (%)</th></tr></thead><tr><td align="center" valign="middle" >Ol (%)</td><td align="center" valign="middle" >Opx (%)</td><td align="center" valign="middle" >Cpx (%)</td><td align="center" valign="middle" >Pl (%)</td><td align="center" valign="middle" >Sp (%)</td><td align="center" valign="middle" >Serp (%)</td><td align="center" valign="middle" >Chl (%)</td><td align="center" valign="middle" >Tc (%)</td><td align="center" valign="middle" >Act (%)</td></tr><tr><td align="center" valign="middle" >KP01</td><td align="center" valign="middle" >71</td><td align="center" valign="middle" >22</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >KP02</td><td align="center" valign="middle" >75</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >OP01</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >22</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >26</td></tr><tr><td align="center" valign="middle" >0P02</td><td align="center" valign="middle" >66</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >11</td></tr><tr><td align="center" valign="middle" >OP03</td><td align="center" valign="middle" >74</td><td align="center" valign="middle" >19</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >OP04</td><td align="center" valign="middle" >85</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >4</td></tr><tr><td align="center" valign="middle" >KS01</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >63</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >76</td></tr><tr><td align="center" valign="middle" >KS02</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >71</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >80</td></tr><tr><td align="center" valign="middle" >KS03</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >62</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >OS01</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >84</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >92</td></tr><tr><td align="center" valign="middle" >OS02</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >76</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >86</td></tr><tr><td align="center" valign="middle" >OS03</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >79</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >87</td></tr><tr><td align="center" valign="middle" >OS04</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >66</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >73</td></tr><tr><td align="center" valign="middle" >OS05</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >79</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >83</td></tr><tr><td align="center" valign="middle" >OS06</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >68</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >78</td></tr><tr><td align="center" valign="middle" >OS07</td><td align="center" valign="middle" >14</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >69</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >74</td></tr></tbody></table></table-wrap><p>KP: Peridotite of Kallidromo, OP: Peridotite of Othrys, KS: Serpentinite of Kallidromo, OS: Serpentinite of Othrys.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Statistical analysis of the serpentinization percentage for ultramafic rocks</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >Peridotites</th><th align="center" valign="middle" >Serpentinites</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >Serpentinization percentage, β (%)</td><td align="center" valign="middle" >Serpentinization percentage, β (%)</td></tr><tr><td align="center" valign="middle" >Maximum value</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >92</td></tr><tr><td align="center" valign="middle" >Minimum value</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >70</td></tr><tr><td align="center" valign="middle" >Mean value</td><td align="center" valign="middle" >9.17</td><td align="center" valign="middle" >79.90</td></tr><tr><td align="center" valign="middle" >Standard Deviation</td><td align="center" valign="middle" >8.75</td><td align="center" valign="middle" >7.02</td></tr></tbody></table></table-wrap><p>m/sec (S.D. 225) respectively. As far as V<sub>s</sub> values are concerned, they vary between 4171 and 4539 m/sec for peridotites and from 2464 to 3044 m/sec for serpentinites. The mean values for serpentinites and peridotites are 2795 and 4392 m/sec respectively. According to [<xref ref-type="bibr" rid="scirp.72665-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.72665-ref5">5</xref>] , both unit weight and velocities decrease with increasing of serpentinization.</p><p>Moreover, the Schmidt Hammer Values (SHV) range between 61.25 and 64.69 for peridotites (<xref ref-type="table" rid="table3">Table 3</xref>), present mean value 63.75 and their standard deviation is 1.24. On</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Physical, dynamic and mechanical property values for ultramafic rocks</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Samples No</th><th align="center" valign="middle" >Effective Porosity, n<sub>e</sub></th><th align="center" valign="middle" >Dry Unit Weight, γ<sub>d</sub> (KN/m<sup>3</sup>)</th><th align="center" valign="middle" >Comp. Wave Velocity, V<sub>p</sub> (m/sec)</th><th align="center" valign="middle" >Shear Wave Velocity, V<sub>s</sub> (m/sec)</th><th align="center" valign="middle" >Schmidt Hammer Values, SHV</th><th align="center" valign="middle" >The point load strength index, I<sub>s</sub><sub>50</sub> (MPa)</th></tr></thead><tr><td align="center" valign="middle" >KP01</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >33.1</td><td align="center" valign="middle" >7959</td><td align="center" valign="middle" >4539</td><td align="center" valign="middle" >64.08</td><td align="center" valign="middle" >10.63</td></tr><tr><td align="center" valign="middle" >KP02</td><td align="center" valign="middle" >0.11</td><td align="center" valign="middle" >32.92</td><td align="center" valign="middle" >7850</td><td align="center" valign="middle" >4458</td><td align="center" valign="middle" >64.69</td><td align="center" valign="middle" >10.14</td></tr><tr><td align="center" valign="middle" >OP01</td><td align="center" valign="middle" >0.19</td><td align="center" valign="middle" >31.67</td><td align="center" valign="middle" >7412</td><td align="center" valign="middle" >4171</td><td align="center" valign="middle" >61.25</td><td align="center" valign="middle" >8.27</td></tr><tr><td align="center" valign="middle" >0P02</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >32.13</td><td align="center" valign="middle" >7704</td><td align="center" valign="middle" >4290</td><td align="center" valign="middle" >64.13</td><td align="center" valign="middle" >7.27</td></tr><tr><td align="center" valign="middle" >OP03</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >33.02</td><td align="center" valign="middle" >7769</td><td align="center" valign="middle" >4372</td><td align="center" valign="middle" >64.17</td><td align="center" valign="middle" >10.53</td></tr><tr><td align="center" valign="middle" >OP04</td><td align="center" valign="middle" >0.08</td><td align="center" valign="middle" >33.17</td><td align="center" valign="middle" >7991</td><td align="center" valign="middle" >4524</td><td align="center" valign="middle" >64.15</td><td align="center" valign="middle" >10.42</td></tr><tr><td align="center" valign="middle" >KS01</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >26.2</td><td align="center" valign="middle" >5442</td><td align="center" valign="middle" >2850</td><td align="center" valign="middle" >52.97</td><td align="center" valign="middle" >3.94</td></tr><tr><td align="center" valign="middle" >KS02</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >26.12</td><td align="center" valign="middle" >5473</td><td align="center" valign="middle" >2888</td><td align="center" valign="middle" >52.73</td><td align="center" valign="middle" >3.41</td></tr><tr><td align="center" valign="middle" >KS03</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >26.79</td><td align="center" valign="middle" >5646</td><td align="center" valign="middle" >3044</td><td align="center" valign="middle" >54.49</td><td align="center" valign="middle" >4.91</td></tr><tr><td align="center" valign="middle" >OS01</td><td align="center" valign="middle" >3.59</td><td align="center" valign="middle" >24.95</td><td align="center" valign="middle" >4955</td><td align="center" valign="middle" >2464</td><td align="center" valign="middle" >49.52</td><td align="center" valign="middle" >2.01</td></tr><tr><td align="center" valign="middle" >OS02</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >25.08</td><td align="center" valign="middle" >5152</td><td align="center" valign="middle" >2666</td><td align="center" valign="middle" >50.55</td><td align="center" valign="middle" >2.28</td></tr><tr><td align="center" valign="middle" >OS03</td><td align="center" valign="middle" >2.29</td><td align="center" valign="middle" >25.37</td><td align="center" valign="middle" >5154</td><td align="center" valign="middle" >2640</td><td align="center" valign="middle" >50.7</td><td align="center" valign="middle" >3.19</td></tr><tr><td align="center" valign="middle" >OS04</td><td align="center" valign="middle" >0.51</td><td align="center" valign="middle" >26.6</td><td align="center" valign="middle" >5637</td><td align="center" valign="middle" >3000</td><td align="center" valign="middle" >54.02</td><td align="center" valign="middle" >4.42</td></tr><tr><td align="center" valign="middle" >OS05</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >25.61</td><td align="center" valign="middle" >5313</td><td align="center" valign="middle" >2727</td><td align="center" valign="middle" >51.5</td><td align="center" valign="middle" >3.23</td></tr><tr><td align="center" valign="middle" >OS06</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >25.93</td><td align="center" valign="middle" >5320</td><td align="center" valign="middle" >2748</td><td align="center" valign="middle" >51.89</td><td align="center" valign="middle" >2.81</td></tr><tr><td align="center" valign="middle" >OS07</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >26.35</td><td align="center" valign="middle" >5520</td><td align="center" valign="middle" >2928</td><td align="center" valign="middle" >53.34</td><td align="center" valign="middle" >3.85</td></tr></tbody></table></table-wrap><p>the other hand, in serpentinites the SHV vary from 49.52 to 54.49, the mean value is 52.17 and their standard deviation is 1.61 (<xref ref-type="table" rid="table4">Table 4</xref>).</p><p>In this research, only diametrical point load tests were carried out on the samples. The point load strength index (I<sub>s</sub><sub>50</sub>) (referred to a standard size 50 mm) values are listed in <xref ref-type="table" rid="table3">Table 3</xref>. The point load strength index values range from 2.01 to 4.91 MPa in serpentinites and between 7.27 and 10.63 MPa in peridotites. The mean values are 3.41 (S.D. 0.91) and 9.54 MPa (S.D. 1.42) respectively (<xref ref-type="table" rid="table4">Table 4</xref>).</p><p>In this research, the triaxial tests were carried out in fifty-eight specimens (three confining pressures at least in each sample ranging from 3 to 18 MPa, <xref ref-type="table" rid="table5">Table 5</xref>) and the material constant (m<sub>i</sub>) and the σ<sub>ci</sub> were estimated by the Hoek and Brown failure criterion (<xref ref-type="table" rid="table5">Table 5</xref>). For this criterion [<xref ref-type="bibr" rid="scirp.72665-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.72665-ref24">24</xref>] , the maximum and minimum total stresses at failure (σ<sub>1</sub> and σ<sub>3</sub>) for intact rock are correlated by the following equation:</p><disp-formula id="scirp.72665-formula1"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x3.png"  xlink:type="simple"/></disp-formula><p>where,</p><p>σ<sub>1</sub>, σ<sub>3</sub>, the maximum and minimum (confining) total stresses at failure for intact rock,</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Statistical analysis of the physical, dynamic and mechanical properties for ultramafic rocks</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" >Maximum value</th><th align="center" valign="middle" >Minimum value</th><th align="center" valign="middle" >Mean value</th><th align="center" valign="middle" >Standard Deviation</th></tr></thead><tr><td align="center" valign="middle"  rowspan="6"  >Peridotites</td><td align="center" valign="middle" >Effective Porosity, n<sub>e</sub></td><td align="center" valign="middle" >0.19</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.12</td><td align="center" valign="middle" >0.04</td></tr><tr><td align="center" valign="middle" >Dry Unit Weight, γ<sub>d</sub> (KN/m<sup>3</sup>)</td><td align="center" valign="middle" >33.17</td><td align="center" valign="middle" >31.67</td><td align="center" valign="middle" >32.67</td><td align="center" valign="middle" >0.62</td></tr><tr><td align="center" valign="middle" >Comp. Wave Velocity, V<sub>p</sub> (m/sec)</td><td align="center" valign="middle" >7991</td><td align="center" valign="middle" >7412</td><td align="center" valign="middle" >7781</td><td align="center" valign="middle" >211</td></tr><tr><td align="center" valign="middle" >Shear Wave Velocity, V<sub>s</sub> (m/sec)</td><td align="center" valign="middle" >4539</td><td align="center" valign="middle" >4171</td><td align="center" valign="middle" >4392</td><td align="center" valign="middle" >143</td></tr><tr><td align="center" valign="middle" >Schmidt Hammer Values, SHV</td><td align="center" valign="middle" >64.69</td><td align="center" valign="middle" >61.25</td><td align="center" valign="middle" >63.75</td><td align="center" valign="middle" >1.24</td></tr><tr><td align="center" valign="middle" >The point load strength index, I<sub>s</sub><sub>50</sub> (MPa)</td><td align="center" valign="middle" >10.63</td><td align="center" valign="middle" >7.27</td><td align="center" valign="middle" >9.54</td><td align="center" valign="middle" >1.42</td></tr><tr><td align="center" valign="middle"  rowspan="6"  >Serpentinites</td><td align="center" valign="middle" >Effective Porosity, n<sub>e</sub></td><td align="center" valign="middle" >3.59</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >1.39</td><td align="center" valign="middle" >1.06</td></tr><tr><td align="center" valign="middle" >Dry Unit Weight, γ<sub>d</sub> (KN/m<sup>3</sup>)</td><td align="center" valign="middle" >26.79</td><td align="center" valign="middle" >24.95</td><td align="center" valign="middle" >25.90</td><td align="center" valign="middle" >0.63</td></tr><tr><td align="center" valign="middle" >Comp. Wave Velocity, V<sub>p</sub> (m/sec)</td><td align="center" valign="middle" >5645</td><td align="center" valign="middle" >4955</td><td align="center" valign="middle" >5361</td><td align="center" valign="middle" >225</td></tr><tr><td align="center" valign="middle" >Shear Wave Velocity, V<sub>s</sub> (m/sec)</td><td align="center" valign="middle" >3044</td><td align="center" valign="middle" >2464</td><td align="center" valign="middle" >2795</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >Schmidt Hammer Values, SHV</td><td align="center" valign="middle" >54.49</td><td align="center" valign="middle" >49.52</td><td align="center" valign="middle" >52.17</td><td align="center" valign="middle" >1.61</td></tr><tr><td align="center" valign="middle" >The point load strength index, I<sub>s</sub><sub>50</sub> (MPa)</td><td align="center" valign="middle" >4.91</td><td align="center" valign="middle" >2.01</td><td align="center" valign="middle" >3.41</td><td align="center" valign="middle" >0.91</td></tr></tbody></table></table-wrap><p>σ<sub>ci</sub>, the uniaxial compressive strength of intact rock,</p><p>m<sub>i</sub>, the material constant which depends on the properties of intact rock.</p><p>Finally the apparent cohesion (c) and the friction angle (φ) for intact rock were calculated using triaxial compressive strength test data (<xref ref-type="table" rid="table5">Table 5</xref>). The confining pressures were plotted against axial stresses with the σ<sub>3</sub> as abscissa and the σ<sub>1</sub> as ordinates (<xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref>). The best linear lines passing through the points are fitted using the least squares technique. The regression functions of this line for peridotites and serpentinites are respectively:</p><disp-formula id="scirp.72665-formula2"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x4.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.72665-formula3"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x5.png"  xlink:type="simple"/></disp-formula><p>Furthermore, c and φ were calculated using the following equations:</p><table-wrap-group id="5"><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> The maximum and minimum (confining) total stresses, the material constant, the friction angle, the apparent cohesion and the estimated uniaxial compressive Strength values for ultramafic rocks</title></caption><table-wrap id="5_1"><table><tbody><thead><tr><th align="center" valign="middle" >Sample No</th><th align="center" valign="middle" >Axial Load, Ρ (kN)</th><th align="center" valign="middle" >Axial Stress, σ<sub>1</sub> = P/A (MPa)</th><th align="center" valign="middle" >Confining Pressure, σ<sub>3</sub> (MPa)</th><th align="center" valign="middle" >Material constant, m<sub>i</sub></th><th align="center" valign="middle" >Friction Angle, φ (˚)</th><th align="center" valign="middle" >Apparent Cohesion, c (MPa)</th><th align="center" valign="middle" >Estimated Uniax. Compressive Strength, σ<sub>ciestm</sub> (Mpa)</th></tr></thead><tr><td align="center" valign="middle" >KP01A</td><td align="center" valign="middle" >520</td><td align="center" valign="middle" >224.66</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >26.58</td><td align="center" valign="middle"  rowspan="4"  >54.13</td><td align="center" valign="middle"  rowspan="4"  >32.18</td><td align="center" valign="middle"  rowspan="4"  >184.43</td></tr><tr><td align="center" valign="middle" >KP01B</td><td align="center" valign="middle" >605</td><td align="center" valign="middle" >261.39</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >KP01C</td><td align="center" valign="middle" >857</td><td align="center" valign="middle" >370.26</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >KP01D</td><td align="center" valign="middle" >651</td><td align="center" valign="middle" >281.26</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >KP02A</td><td align="center" valign="middle" >573</td><td align="center" valign="middle" >247.56</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >28.16</td><td align="center" valign="middle"  rowspan="4"  >54.78</td><td align="center" valign="middle"  rowspan="4"  >35.54</td><td align="center" valign="middle"  rowspan="4"  >206.44</td></tr><tr><td align="center" valign="middle" >KP02B</td><td align="center" valign="middle" >609</td><td align="center" valign="middle" >263.12</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >KP02C</td><td align="center" valign="middle" >906</td><td align="center" valign="middle" >391.43</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >KP02D</td><td align="center" valign="middle" >809</td><td align="center" valign="middle" >349.53</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >KS01A</td><td align="center" valign="middle" >220</td><td align="center" valign="middle" >95.05</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="3"  >14.27</td><td align="center" valign="middle"  rowspan="3"  >44.10</td><td align="center" valign="middle"  rowspan="3"  >16.98</td><td align="center" valign="middle"  rowspan="3"  >73.97</td></tr><tr><td align="center" valign="middle" >KS01B</td><td align="center" valign="middle" >269</td><td align="center" valign="middle" >116.22</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >KS01C</td><td align="center" valign="middle" >338</td><td align="center" valign="middle" >146.03</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >KS02A</td><td align="center" valign="middle" >232</td><td align="center" valign="middle" >102.11</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="3"  >14.39</td><td align="center" valign="middle"  rowspan="3"  >44.64</td><td align="center" valign="middle"  rowspan="3"  >17.94</td><td align="center" valign="middle"  rowspan="3"  >79.95</td></tr><tr><td align="center" valign="middle" >KS02B</td><td align="center" valign="middle" >276</td><td align="center" valign="middle" >121.47</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >KS02C</td><td align="center" valign="middle" >350</td><td align="center" valign="middle" >154.04</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >KS03A</td><td align="center" valign="middle" >337</td><td align="center" valign="middle" >148.87</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >16.04</td><td align="center" valign="middle"  rowspan="4"  >46.58</td><td align="center" valign="middle"  rowspan="4"  >24.48</td><td align="center" valign="middle"  rowspan="4"  >115.37</td></tr><tr><td align="center" valign="middle" >KS03B</td><td align="center" valign="middle" >344</td><td align="center" valign="middle" >151.96</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >KS03C</td><td align="center" valign="middle" >539</td><td align="center" valign="middle" >238.11</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >KS03D</td><td align="center" valign="middle" >406</td><td align="center" valign="middle" >179.35</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OP01A</td><td align="center" valign="middle" >284</td><td align="center" valign="middle" >122.70</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >21.09</td><td align="center" valign="middle"  rowspan="4"  >48.17</td><td align="center" valign="middle"  rowspan="4"  >20.96</td><td align="center" valign="middle"  rowspan="4"  >95.89</td></tr><tr><td align="center" valign="middle" >OP01B</td><td align="center" valign="middle" >369</td><td align="center" valign="middle" >159.43</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OP01C</td><td align="center" valign="middle" >534</td><td align="center" valign="middle" >230.71</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OP01D</td><td align="center" valign="middle" >398</td><td align="center" valign="middle" >171.95</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OP02A</td><td align="center" valign="middle" >486</td><td align="center" valign="middle" >214.69</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >25.20</td><td align="center" valign="middle"  rowspan="4"  >53.37</td><td align="center" valign="middle"  rowspan="4"  >30.33</td><td align="center" valign="middle"  rowspan="4"  >170.27</td></tr><tr><td align="center" valign="middle" >OP02B</td><td align="center" valign="middle" >531</td><td align="center" valign="middle" >233.70</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OP02C</td><td align="center" valign="middle" >789</td><td align="center" valign="middle" >348.54</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OP02D</td><td align="center" valign="middle" >596</td><td align="center" valign="middle" >263.29</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OP03A</td><td align="center" valign="middle" >582</td><td align="center" valign="middle" >250.53</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >27.76</td><td align="center" valign="middle"  rowspan="4"  >55.01</td><td align="center" valign="middle"  rowspan="4"  >33.85</td><td align="center" valign="middle"  rowspan="4"  >200.41</td></tr><tr><td align="center" valign="middle" >OP03B</td><td align="center" valign="middle" >609</td><td align="center" valign="middle" >262.15</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OP03C</td><td align="center" valign="middle" >918</td><td align="center" valign="middle" >395.16</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OP03D</td><td align="center" valign="middle" >726</td><td align="center" valign="middle" >312.51</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OP04A</td><td align="center" valign="middle" >520</td><td align="center" valign="middle" >229.71</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >26.69</td><td align="center" valign="middle" >54.09</td><td align="center" valign="middle" >32.84</td><td align="center" valign="middle" >187.52</td></tr></tbody></table></table-wrap><table-wrap id="5_2"><table><tbody><thead><tr><th align="center" valign="middle" >OP04B</th><th align="center" valign="middle" >567</th><th align="center" valign="middle" >250.48</th><th align="center" valign="middle" >6</th><th align="center" valign="middle"  rowspan="3"  ></th><th align="center" valign="middle"  rowspan="3"  ></th><th align="center" valign="middle"  rowspan="3"  ></th><th align="center" valign="middle"  rowspan="3"  ></th></tr></thead><tr><td align="center" valign="middle" >OP04C</td><td align="center" valign="middle" >837</td><td align="center" valign="middle" >369.75</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OP04D</td><td align="center" valign="middle" >685</td><td align="center" valign="middle" >302.60</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OS01A</td><td align="center" valign="middle" >116</td><td align="center" valign="middle" >50.12</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="3"  >12.76</td><td align="center" valign="middle"  rowspan="3"  >38.05</td><td align="center" valign="middle"  rowspan="3"  >9.88</td><td align="center" valign="middle"  rowspan="3"  >33.55</td></tr><tr><td align="center" valign="middle" >OS01B</td><td align="center" valign="middle" >163</td><td align="center" valign="middle" >70.42</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS01C</td><td align="center" valign="middle" >208</td><td align="center" valign="middle" >89.54</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >OS02A</td><td align="center" valign="middle" >133</td><td align="center" valign="middle" >57.25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="3"  >13.10</td><td align="center" valign="middle"  rowspan="3"  >39.59</td><td align="center" valign="middle"  rowspan="3"  >10.44</td><td align="center" valign="middle"  rowspan="3"  >37.96</td></tr><tr><td align="center" valign="middle" >OS02B</td><td align="center" valign="middle" >168</td><td align="center" valign="middle" >72.32</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS02C</td><td align="center" valign="middle" >228</td><td align="center" valign="middle" >98.14</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >OS03A</td><td align="center" valign="middle" >161</td><td align="center" valign="middle" >69.30</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >13.52</td><td align="center" valign="middle"  rowspan="4"  >39.44</td><td align="center" valign="middle"  rowspan="4"  >12.54</td><td align="center" valign="middle"  rowspan="4"  >45.00</td></tr><tr><td align="center" valign="middle" >OS03B</td><td align="center" valign="middle" >174</td><td align="center" valign="middle" >74.90</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS03C</td><td align="center" valign="middle" >311</td><td align="center" valign="middle" >133.87</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OS03D</td><td align="center" valign="middle" >222</td><td align="center" valign="middle" >95.56</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OS04A</td><td align="center" valign="middle" >238</td><td align="center" valign="middle" >102.45</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="3"  >14.82</td><td align="center" valign="middle"  rowspan="3"  >44.92</td><td align="center" valign="middle"  rowspan="3"  >18.15</td><td align="center" valign="middle"  rowspan="3"  >81.01</td></tr><tr><td align="center" valign="middle" >OS04B</td><td align="center" valign="middle" >291</td><td align="center" valign="middle" >125.73</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS04C</td><td align="center" valign="middle" >362</td><td align="center" valign="middle" >155.83</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >OS05A</td><td align="center" valign="middle" >174</td><td align="center" valign="middle" >74.90</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="3"  >13.67</td><td align="center" valign="middle"  rowspan="3"  >42.00</td><td align="center" valign="middle"  rowspan="3"  >13.81</td><td align="center" valign="middle"  rowspan="3"  >55.47</td></tr><tr><td align="center" valign="middle" >OS05B</td><td align="center" valign="middle" >222</td><td align="center" valign="middle" >95.56</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS05C</td><td align="center" valign="middle" >282</td><td align="center" valign="middle" >121.39</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >OS06A</td><td align="center" valign="middle" >221</td><td align="center" valign="middle" >97.27</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >13.86</td><td align="center" valign="middle"  rowspan="4"  >42.17</td><td align="center" valign="middle"  rowspan="4"  >18.24</td><td align="center" valign="middle"  rowspan="4"  >73.9</td></tr><tr><td align="center" valign="middle" >OS06B</td><td align="center" valign="middle" >246</td><td align="center" valign="middle" >108.27</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS06C</td><td align="center" valign="middle" >391</td><td align="center" valign="middle" >172.08</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OS06D</td><td align="center" valign="middle" >305</td><td align="center" valign="middle" >134.23</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" >OS07A</td><td align="center" valign="middle" >268</td><td align="center" valign="middle" >117.95</td><td align="center" valign="middle" >3</td><td align="center" valign="middle"  rowspan="4"  >15.52</td><td align="center" valign="middle"  rowspan="4"  >44.64</td><td align="center" valign="middle"  rowspan="4"  >21.21</td><td align="center" valign="middle"  rowspan="4"  >92.32</td></tr><tr><td align="center" valign="middle" >OS07B</td><td align="center" valign="middle" >297</td><td align="center" valign="middle" >131.20</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >OS07C</td><td align="center" valign="middle" >460</td><td align="center" valign="middle" >202.45</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" >OS07D</td><td align="center" valign="middle" >365</td><td align="center" valign="middle" >160.05</td><td align="center" valign="middle" >9</td></tr></tbody></table></table-wrap></table-wrap-group><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The confining pressures (σ<sub>3</sub>) against axial stresses (σ<sub>1</sub>) for Peridotites</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x6.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The confining pressures (σ<sub>3</sub>) against axial stresses (σ<sub>1</sub>) for Serpentinites</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x7.png"/></fig><disp-formula id="scirp.72665-formula4"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x8.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72665-formula5"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x9.png"  xlink:type="simple"/></disp-formula><p>where</p><p>a, the gradient of the Equations (2) and (3).</p></sec></sec><sec id="s4"><title>4. Correlation Analysis</title><p>Least squares regression analysis was applied in order to describe the relationships among triaxial characteristics (c, φ), physical, dynamic, mechanical properties and the petrographic data of the ultramafic rocks. The equation of the best-fit line and the determination coefficient (R<sup>2</sup>) were determined for each regression. Techniques from Excel 2003 software (Analysis ToolPak program) was used to process the data.</p>Correlation between Triaxial Parameters and Physical, Dynamic and Mechanical Properties<p>In this study, an attempt to correlate c and φ with dry unit weight is respectively presented in <xref ref-type="fig" rid="fig4">Figure 4</xref> and <xref ref-type="fig" rid="fig5">Figure 5</xref>. The logarithmic equation seems to fit better (R<sup>2</sup> = 0.84) the dry unit weight with the apparent cohesion while the relationship between φ and γ<sub>d</sub> is better described by the linear equation (R<sup>2</sup> = 0.92). The regression lines representing the best fit between effective porosity and c, φ are logarithmic (<xref ref-type="fig" rid="fig6">Figure 6</xref> and <xref ref-type="fig" rid="fig7">Figure 7</xref>). The apparent cohesion and the friction angle using the effective porosity values can be expressed by the empirical equations:</p><disp-formula id="scirp.72665-formula6"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x10.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72665-formula7"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/72665x11.png"  xlink:type="simple"/></disp-formula><p>Moreover, the plots of the apparent cohesion values as a function of sound velocities (V<sub>p</sub>, V<sub>s</sub>) values are shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>. The best fit relationships are found to be linear and the determination coefficients are 0.83 and 0.84 respectively. The correlations between the friction angle and the wave velocities were also determined. A positive</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Relationship between apparent cohesion and dry unit weight for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x12.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Correlation between friction angle and dry unit weight for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x13.png"/></fig><p>relationship was found between the φ and the V<sub>p</sub>, V<sub>s</sub> (<xref ref-type="fig" rid="fig9">Figure 9</xref>) indicating that the friction angle increase with increasing wave velocities. The logarithmic model gives high R<sup>2</sup> values, but better correlation is described by the linear trends (<xref ref-type="fig" rid="fig9">Figure 9</xref>).</p><p>As it is illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>0, <xref ref-type="fig" rid="fig1">Figure 1</xref>1 the friction angle and apparent cohesion present visible correlations with the degree of serpentinization (β). The c, φ decrease linearly with the increase of β. The relationship between φ and β presents higher</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Relation between apparent cohesion and effective porosity for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x14.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Logarithmic function between friction angle and effective porosity for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x15.png"/></fig><p>determination coefficient (R<sup>2</sup> = 0.93) than that between c and β (R<sup>2</sup> = 0.86).</p><p>In addition, <xref ref-type="fig" rid="fig1">Figure 1</xref>2 presents the plot of the apparent cohesion against Schmidt Hammer Values (SHV). The best fit equation is logarithmic and the relation between them presents high determination coefficient (R<sup>2</sup> = 0.88). The plots of the friction angle as a function of the SHV are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>3. The best fit equation is logarithmic with high determination coefficient (R<sup>2</sup> = 0.95).</p><p>As shown in <xref ref-type="table" rid="table6">Table 6</xref>, linear and logarithmic functions can describe the relationships between c and I<sub>s</sub><sub>50</sub> and between φ and I<sub>s</sub><sub>50</sub>. The logarithmic equations seem to fit better</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Relationship of wave velocities with apparent cohesion for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x16.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Correlation between wave velocities and friction angle for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x17.png"/></fig><p>the above-mentioned properties than the linear equations, exhibiting R-square values 0.87 and 0.93 respectively. The logarithmic functions are illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>4 and <xref ref-type="fig" rid="fig1">Figure 1</xref>5.</p></sec><sec id="s5"><title>5. Conclusions</title><p>The estimation of the triaxial parameters is considered to be the most important component in any engineering geology project because the rock-mass properties are calculated through them. Despite of their simple, fast and easy determination, they require a</p><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Relationship between degree of serpentinization and apparent cohesion for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x18.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Correlation between degree of serpentinization and friction angle for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x19.png"/></fig><p>large number of well prepared (regularly shaped) rock specimens. But ultramafic rocks (especially serpentinites) are usually not suitable for preparing specimens. Thus, the immediate determination of the triaxial characteristics is usually difficult for these rocks. For this reason, this study mainly attempts to develop empirical equations between triaxial parameters and physico-mechanical properties.</p><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Relationship of Schmidt hammer values with apparent cohesion for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x20.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> Variation of Schmidt hammer values against friction angle for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x21.png"/></fig><p>In this paper ultramafic samples, taken from sixteen sites of central Greece (western part of Othrysmt and the Kallidromomt), were tested in laboratory and the triaxial properties were predicted through the wave velocities by simple regression analysis.</p><p>The research demonstrates that the friction angle (φ) exhibits strong linear correlation with the dry unit weight (γ<sub>d</sub>) (R<sup>2</sup> = 0.92) while the logarithmic equation seems to correlate better (R<sup>2</sup> = 0.84) the dry unit weight with the apparent cohesion (c).</p><p>Significant negative logarithmic relationships exist between the triaxial parameters</p><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> Correlation between point load strength index and friction angle for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x22.png"/></fig><fig id="fig15"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>5</label><caption><title> Relationship between point load strength index and apparent cohesion for ultramafic rocks</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/72665x23.png"/></fig><p>and the effective porosity (n<sub>e</sub>). The relation between φ and n<sub>e</sub> presents higher determination coefficient (R<sup>2</sup> = 0.96) than that between c and n<sub>e</sub> (R<sup>2</sup> = 0.91).</p><p>The wave velocities are positively correlated with c and φ and provide high determination coefficient. In particular, φ presents higher correlation with V<sub>p</sub>, V<sub>s</sub> (R<sup>2</sup> = 0.91, R<sup>2</sup> = 0.92 respectively) than c (R<sup>2</sup> = 0.83, R<sup>2</sup> = 0.84 respectively).</p><p>The effect of alteration on the physico-mechanical properties of ultramafic rocks can be characterized quantitatively by the serpentinization percentage (β). Strong inverse linear</p><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Regression equations and determination coefficients (R<sup>2</sup>) for ultramafic rocks</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameters to be related</th><th align="center" valign="middle" >Regression Equations</th><th align="center" valign="middle" >R<sup>2</sup></th></tr></thead><tr><td align="center" valign="middle" >Apparent cohesion and point load strength index</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/72665x24.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.87</td></tr><tr><td align="center" valign="middle" >Apparent cohesion and point load strength index</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/72665x25.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.85</td></tr><tr><td align="center" valign="middle" >Friction angle and point load strength index</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/72665x26.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.93</td></tr><tr><td align="center" valign="middle" >Friction angle and point load strength index</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/72665x27.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.91</td></tr></tbody></table></table-wrap><p>relationships exist between the β and c, φ. The relationship between φ and β presents higher determination coefficient (R<sup>2</sup> = 0.93) than that between c and β (R<sup>2</sup> = 0.86).</p><p>The relations between c, φ and Schmidt hammer values (SHV) are also expressed by logarithmic functions. The SHV shows higher correlation (R<sup>2</sup> = 0.95) with the friction angle than that with apparent cohesion (R<sup>2</sup> = 0.88).</p><p>Both the c and φ exhibit negative relationships with the point load strength index (I<sub>s</sub><sub>50</sub>). Τhe best fit trends are logarithmic and φ presents higher correlation with I<sub>s</sub><sub>50</sub> (R<sup>2</sup> = 0.93) than that c with I<sub>s</sub><sub>50</sub> (R<sup>2</sup> = 0.87).</p><p>Some observed deviations may be due to the petrographic variety, the different serpentinization degree, the structural complexity and the internally imprinted tectonic deformation of studied rocks.</p><p>All empirical methods evaluated in this study can be used for an assessment of the triaxial characteristics of ultramafic rocks, especially for serpentinites whose preparation in standard size cores, is quite difficult. However, it is commonly known that the prediction equations derived by different researches are dependent on rock types, quality, test conditions and different tectonic settings.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This study was funded by the State Scholarship Foundation of Greece (I.K.Y). The authors would also like to express their thanks to the Public Works Central Laboratory of Greece (KEDE) and to Ass. Professor Anastasios Tsagalidis for his help in petrography.</p></sec><sec id="s7"><title>Cite this paper</title><p>Diamantis, K., Exarhakos, G., Migiros, G. and Gartzos, E. (2016) Evaluating the Triaxial Charac- teristics of Ultamafic Rocks from Central Greece Using the Physical, Dynamic and Mechanical Properties. Open Access Library Journal, 3: e3214. http://dx.doi.org/10.4236/oalib.1103214</p></sec></body><back><ref-list><title>References</title><ref id="scirp.72665-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Diamantis, K. (2010) Engineering Geological Properties of the Ultrabasic Rocks in Othrys and Kallidromo Mountains (Central Greece). 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