<?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">OJCE</journal-id><journal-title-group><journal-title>Open Journal of Civil Engineering</journal-title></journal-title-group><issn pub-type="epub">2164-3164</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojce.2018.84038</article-id><article-id pub-id-type="publisher-id">OJCE-89392</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Sixth Scale Model Studies of Masonry Arch Rib Behaviour at Different Eccentricities
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abbagana</surname><given-names>Mohammed</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>T.</surname><given-names>G. Hughes</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>School of Engineering, Cardiff University, Cardiff, UK</addr-line></aff><aff id="aff1"><addr-line>Department of Civil Engineering, Abubakar Tafawa Balewa University, Bauchi, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>09</day><month>10</month><year>2018</year></pub-date><volume>08</volume><issue>04</issue><fpage>533</fpage><lpage>543</lpage><history><date date-type="received"><day>30,</day>	<month>August</month>	<year>2018</year></date><date date-type="rev-recd"><day>22,</day>	<month>December</month>	<year>2018</year>	</date><date date-type="accepted"><day>25,</day>	<month>December</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>
 
 
  This paper reports a validation study involving sixth scale masonry model to replicate prototype tests carried out on five unit high masonry prisms. In order to test the applicability of small masonry models to real life problems, an investigation into masonry behaviour relevant to the serviceability requirement of masonry arch bridges was chosen as prototype test to validate the small scale masonry tests. Only representative masonry specimens were considered in the study; this corresponded to parts of an arch ring in a complete masonry arch. Two mortar designations; designation iv and designation v were used. These weak mortars tend to conform better to existing old structures. Loads were applied at four eccentricities of 0, 5, 9, and 14 mm from the centre of the specimens. This corresponds to e/d ratios of 0, 0.14, 0.25, and 0.39, where e is the eccentricity of the load and d the length of the transverse section of the specimens. The result shows that validation study corresponds with prototype study for low eccentricities; therefore, strength enhancement is seen over the concentric compressive strength. However, this does not apply at higher eccentricities as specimens were noticed to fail by elastic instability characterised by tension debonding of the top mortar joint.
 
</p></abstract><kwd-group><kwd>Masonry</kwd><kwd> Arch Bridge</kwd><kwd> Prototype</kwd><kwd> Eccentricity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In order to test the applicability of small masonry models to real life problems, an investigation by Roberts et al. [<xref ref-type="bibr" rid="scirp.89392-ref1">1</xref>] into masonry behaviour relevant to the serviceability requirement of masonry arch bridges was chosen as prototype test to validate the small scale masonry tests by Mohammed [<xref ref-type="bibr" rid="scirp.89392-ref2">2</xref>].</p><p>In masonry arches, the arch barrel, which is the main structural component, carries the applied load principally through the induced axial compressive thrust. However, as traffic moves over the bridge, the arch barrel may also be subjected to significantly reversed bending and shear forces. This may result in the arch barrel being subjected to considerable cyclic stress ranges, which could affect the use of the bridge adversely [<xref ref-type="bibr" rid="scirp.89392-ref3">3</xref>].</p><p>Recently there has been interest in the establishment of serviceability limits for masonry bridges, BD 21/97 [<xref ref-type="bibr" rid="scirp.89392-ref4">4</xref>] and Boothby et al. [<xref ref-type="bibr" rid="scirp.89392-ref5">5</xref>]. In BD 21/97 (1997), it is suggested that the service load should be limited to 50% of the predicted ultimate load. This conclusion is based on the results of numerous large and full scale tests, which show that the load deflection response of masonry arch bridges remains approximately linear up to 50% of the ultimate load. However, because of the uncertainties in the material properties of masonry due to environmental effects, theoretical predictions of the ultimate loads of masonry arch bridges are usually not reliable [<xref ref-type="bibr" rid="scirp.89392-ref3">3</xref>].</p><p>In masonry arches the compressive force will generally be eccentric and in approaching failure; the force on some units will be highly eccentric and these forces will generally be concentrated on a small part of the surface area of the unit and form a so called hinge [<xref ref-type="bibr" rid="scirp.89392-ref6">6</xref>]. Various prototype studies [<xref ref-type="bibr" rid="scirp.89392-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.89392-ref8">8</xref>] have shown that the compressive stress at failure under eccentric loading is greater than under axial loading and further enhancement to the apparent compressive strength has been established under highly concentrated loads by other studies [<xref ref-type="bibr" rid="scirp.89392-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.89392-ref9">9</xref>].</p><p>Therefore, the main objective of the application study was to investigate the effect of eccentric concentrated loading on sixth scale masonry with a view to comparing it to the prototype study by using static tests as a tool for the understanding of the overall behaviour of masonry arches.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Masonry Specimens</title><p>Only representative masonry specimens were considered in the study, this corresponded to parts of an arch ring in a complete masonry arch. For the purpose of this study a five unit high, sixth scale masonry specimen as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> was used. Two mortar designations; designation iv and designation v were used. These weak mortars tend to conform better to existing old structures. The proportions of the constituent elements used in the mortar are as given in BS 5628 [<xref ref-type="bibr" rid="scirp.89392-ref10">10</xref>] and the dry mass proportions in BS 4551 [<xref ref-type="bibr" rid="scirp.89392-ref11">11</xref>] were used and are shown in <xref ref-type="table" rid="table1">Table 1</xref>. All mortars were made using HST 95 sand. All the specimens were allowed to cure normally in the laboratory after preparation and tested at or shortly after 28 days of curing.</p><p>Other specimen formats were also used in the original study [<xref ref-type="bibr" rid="scirp.89392-ref1">1</xref>] , but for the purpose of the application study, only the five unit high stack bonded specimen was used. This was because the objective was to see if it was feasible to conduct such tests at sixth scale.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Mortar proportions</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Mortar</th><th align="center" valign="middle" >Proportions</th><th align="center" valign="middle" >W/c ratio</th></tr></thead><tr><td align="center" valign="middle" >Type</td><td align="center" valign="middle" >Cement:lime:sand</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >iv</td><td align="center" valign="middle" >I:2:9</td><td align="center" valign="middle" >2.50</td></tr><tr><td align="center" valign="middle" >v</td><td align="center" valign="middle" >I:1.5:13</td><td align="center" valign="middle" >3.12</td></tr></tbody></table></table-wrap></sec><sec id="s2_2"><title>2.2. Tests</title><p>Testing was carried in a 20 kN capacity testing machine under constant rate of displacement of 0.25 mm/min. Load was applied via an arrangement of 6 mm steel plates and 6mm steel bars as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The specimens were also supported on similar arrangement of plates and bars as used in applying the loads in order to ensure uniform eccentricity from the centre of the specimens. Loads were applied at four eccentricities of 0, 5, 9, and 14 mm from the centre of the specimens. This corresponds to e/d ratios of 0, 0.14, 0.25, and 0.39, where e is the eccentricity of the load and d the length of the transverse section of the specimens as defined in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Test set up for the e/d ratio = 0.25 is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec><sec id="s2_3"><title>2.3. Calculation</title><p>The assumed stress blocks used in calculations are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. For concentric and eccentric loading within the middle third of the section the stress distribution is as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). In this case the maximum compressive</p><p>stress f m is given by (1)</p><p>f m = P b d + 6 P e b d 2 (1)</p><p>where P is the applied compressive force and bd is the loaded cross-section area (width &#215; depth).</p><p>When the eccentricity of load is beyond the middle third of the cross-section the cracked triangular stress block in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) was assumed. For this distribution, equilibrium of external and internal forces entails that Equations (2) and (3) applies</p><p>f m b h 2 = P (2)</p><p>f m b h 2 [ d 2 − h 3 ] = P e (3)</p><p>Substituting for P in (3) gives (4) and (5)</p><p>h = 3 [ d 2 − e ] (4)</p><p>f m = 2 P b h (5)</p><p>The cracked triangular no tension distribution was chosen for this solution because it gave an upper bound solution rather than the cracked parabolic no tension distribution (not presented here).</p></sec></sec><sec id="s3"><title>3. Discussion of Results</title><p>In the prototype test failure of the specimens was initiated by crushing and squeezing of the mortar from the mortar joints followed by vertical splitting of the bricks as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref> show the variation of compressive strength with load eccentricity for mortar designation v. Both of the figures show that the compressive strength is increased as the eccentricity is increased in line with findings by most authors, notably Page and Hendry [<xref ref-type="bibr" rid="scirp.89392-ref12">12</xref>] who have even suggested design rules for concentrated loads with varying eccentricities on masonry. The reason for the enhancement as suggested by Drysdale and Hamid [<xref ref-type="bibr" rid="scirp.89392-ref7">7</xref>] is due to the strain</p><p>gradient effect on the compressive strength. They argued that the gradient of vertical compression strain across a brick due to eccentricity of a load will be accompanied by a corresponding tensile strain gradient in the lateral direction. But because the tensile strength of masonry units are affected by strain gradient (as shown by the greater flexural tensile strength in comparison to the direct axial tensile strength), they concluded that the apparent compressive strength should be higher for eccentrically loaded brickwork.</p><p>Typical failure of the specimens in the model study was usually characterised by vertical splitting cracks under the load point as well as at the sides of the specimens. This was followed by crushing of the loaded point in some cases. <xref ref-type="fig" rid="fig7">Figure 7</xref> shows a typical failure in one of the tests. In the case of the specimens with e/d of 0.39 there were cases in which tension debonding was noticeable at the edge furthest from the load point just before failure, in specimens made with both designation iv and designation v mortar. <xref ref-type="fig" rid="fig8">Figure 8</xref> shows the debonding on the tensile side in one of the tests. This type of failure represents an elastic instability</p><p>characterised by debonding on the tensile side for loads with high eccentricity according Sahlin [<xref ref-type="bibr" rid="scirp.89392-ref13">13</xref>].</p><p>The results as tabulated in <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref> for tests using mortar designations iv (test; S4) and v (test; S5) show a mixed picture as seen in <xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>0, which show the variation of maximum compressive strength with e/d ratio for tests using mortar designations iv and v, respectively. In <xref ref-type="fig" rid="fig9">Figure 9</xref>, it is seen that there is an initial increase in strength from the point of zero eccentricity to point e/d = 0.14. Followed by a decrease in strength from this point up to the last point e/d = 0.39. While in <xref ref-type="fig" rid="fig1">Figure 1</xref>0, there is an increase in strength from the point of zero eccentricity up to the point e/d = 0.25 before decreasing at the last point e/d = 0.39. Therefore, as seen from the trend lines in both figures there is only a marginal increase in compressive strength as the eccentricity is increased for the eccentricities considered (neglecting e/d = 0.39). But the actual compressive strength in the model tests was higher because of the higher model unit compressive strength, which is about 57% higher than the prototype unit strength.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>1 shows a comparison of the effect of eccentricity in the prototype and model scale for the same mortar type. The vertical axis has been made dimensionless by normalising it with respect to their (both prototype and model) respective compressive strengths at zero eccentricity. It is seen from the figure that the fitted trend line for the prototype test is significantly steeper than that for the model test. The ratio of their gradients is 5.4 which is nearly equal to their scale ratio. From the foregoing, it therefore seems that in the S4 model test for e/d ratios of 0.25 and 0.39 (outside the middle third of the section), the expected enhancement in compressive strength is not seen while in the S5 model test strength enhancement does not hold for the e/d of 0.39. However, since in the prototype tests the highest eccentricity used was 0.33 it can still be argued that there is some agreement of the S5 test to the prototype test since there is strength increase with load eccentricity within their comparable range of eccentricities. The reason for the greater enhancement in the prototype over the model scale is not certain, but it could to be due to the elastic instability characterised by the cracking on the tension side of the model specimens before material failure in the units. But since the geometries of the test specimens and load eccentricities for the prototype and model tests are similar, the expectation was for a comparable enhancement factor in the model test. It therefore seems that there is better agreement between the failure mechanics of prototype and model specimens in axial compression than in eccentric loading. This may be because it is difficult to model mortar at very small scales because of the thinness of the joints. Because as reported by Mohammed et al. [<xref ref-type="bibr" rid="scirp.89392-ref14">14</xref>] effects with regards to joint thickness are difficult to model at sixth scale. The reason for this is not certain but it offers a possible area of further investigation in the future.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Test results for specimens made with designation iv mortar, S4, with COV in brackets</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Test</th><th align="center" valign="middle"  rowspan="2"  >e/d</th><th align="center" valign="middle"  rowspan="2"  >Load, N</th><th align="center" valign="middle" >Masonry</th><th align="center" valign="middle" >Mean</th><th align="center" valign="middle" >Mortar</th></tr></thead><tr><td align="center" valign="middle" >Reference</td><td align="center" valign="middle" >Strength, N/mm<sup>2</sup></td><td align="center" valign="middle" >N/mm<sup>2</sup></td><td align="center" valign="middle" >Strength, Nmm<sup>2</sup></td></tr><tr><td align="center" valign="middle" >S4-A1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >9812</td><td align="center" valign="middle" >16.0</td><td align="center" valign="middle"  rowspan="5"  >13.1 (17.2)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-A2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >8153</td><td align="center" valign="middle" >13.3</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-A3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >6745</td><td align="center" valign="middle" >11.0</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-A4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >6573</td><td align="center" valign="middle" >10.7</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-A5</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >8860</td><td align="center" valign="middle" >14.5</td><td align="center" valign="middle" >1.7</td></tr><tr><td align="center" valign="middle" >S4-B1</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >4813</td><td align="center" valign="middle" >14.4</td><td align="center" valign="middle"  rowspan="6"  >18.2 (12.6)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-B2</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >6142</td><td align="center" valign="middle" >18.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-B3</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >7105</td><td align="center" valign="middle" >21.3</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-B4</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >5973</td><td align="center" valign="middle" >17.9</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-B5</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >5873</td><td align="center" valign="middle" >17.6</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-B6</td><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >6563</td><td align="center" valign="middle" >19.7</td><td align="center" valign="middle" >3.0</td></tr><tr><td align="center" valign="middle" >S4-C1</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >3860</td><td align="center" valign="middle" >16.9</td><td align="center" valign="middle"  rowspan="6"  >16.6 (16.0)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-C2</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >4298</td><td align="center" valign="middle" >18.8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-C3</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >3343</td><td align="center" valign="middle" >14.6</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-C4</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >4421</td><td align="center" valign="middle" >19.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-C5</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >4022</td><td align="center" valign="middle" >17.6</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-C6</td><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >2830</td><td align="center" valign="middle" >12.4</td><td align="center" valign="middle" >1.9</td></tr><tr><td align="center" valign="middle" >S4-D1</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1565</td><td align="center" valign="middle" >15.6</td><td align="center" valign="middle"  rowspan="6"  >13.4 (15.9)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-D2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1028</td><td align="center" valign="middle" >10.3</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-D3</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1284</td><td align="center" valign="middle" >12.8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-D4</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1589</td><td align="center" valign="middle" >15.9</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-D5</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1327</td><td align="center" valign="middle" >13.3</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S4-D6</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1229</td><td align="center" valign="middle" >12.3</td><td align="center" valign="middle" >2.1</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Test results for specimens made with designation v mortar, S5, with COV in brackets</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Test</th><th align="center" valign="middle" >e/d</th><th align="center" valign="middle" >Load, N</th><th align="center" valign="middle" >Masonry</th><th align="center" valign="middle" >Mean</th><th align="center" valign="middle" >Mortar</th></tr></thead><tr><td align="center" valign="middle" >Reference</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >Strength, N/mm<sup>2</sup></td><td align="center" valign="middle" >N/mm<sup>2</sup></td><td align="center" valign="middle" >Strength, Nmm<sup>2</sup></td></tr><tr><td align="center" valign="middle" >S5-A1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >7811</td><td align="center" valign="middle" >12.8</td><td align="center" valign="middle"  rowspan="6"  >12.2 (16.2)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-A2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >6361</td><td align="center" valign="middle" >10.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-A3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >8720</td><td align="center" valign="middle" >14.2</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-A4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >8720</td><td align="center" valign="middle" >14.2</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-A5</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5780</td><td align="center" valign="middle" >9.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-A6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >7516</td><td align="center" valign="middle" >12.3</td><td align="center" valign="middle" >1.1</td></tr><tr><td align="center" valign="middle" >S5-B1</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >7521</td><td align="center" valign="middle" >12.3</td><td align="center" valign="middle"  rowspan="6"  >13.9 (23.7)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-B2</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >4600</td><td align="center" valign="middle" >13.8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-B3</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >4990</td><td align="center" valign="middle" >15.0</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-B4</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >5259</td><td align="center" valign="middle" >15.8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-B5</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >6012</td><td align="center" valign="middle" >18.0</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-B6</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >2822</td><td align="center" valign="middle" >8.5</td><td align="center" valign="middle" >0.9</td></tr><tr><td align="center" valign="middle" >S5-C1</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >3784</td><td align="center" valign="middle" >16.6</td><td align="center" valign="middle"  rowspan="6"  >14.8 (32.0)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-C2</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >3276</td><td align="center" valign="middle" >14.3</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-C3</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >2282</td><td align="center" valign="middle" >10.0</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-C4</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >3535</td><td align="center" valign="middle" >15.5</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-C5</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >2240</td><td align="center" valign="middle" >9.8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-C6</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >5145</td><td align="center" valign="middle" >22.5</td><td align="center" valign="middle" >0.8</td></tr><tr><td align="center" valign="middle" >S5-D1</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >1168</td><td align="center" valign="middle" >11.7</td><td align="center" valign="middle"  rowspan="5"  >10.1 (40.7)</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-D2</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >638</td><td align="center" valign="middle" >6.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-D3</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >1643</td><td align="center" valign="middle" >16.4</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-D4</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >879</td><td align="center" valign="middle" >8.8</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >S5-D5</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >708</td><td align="center" valign="middle" >7.1</td><td align="center" valign="middle" >1.1</td></tr></tbody></table></table-wrap></sec><sec id="s4"><title>4. Conclusion</title><p>The application study somewhat agrees with the prototype study for low eccentricities; therefore, strength enhancement is seen over the concentric compressive strength. However, this does not apply at higher eccentricities as specimens were noticed to fail by elastic instability characterised by tension debonding of the top mortar joint.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Mohammed, A. and Hughes, T.G. (2018) Sixth Scale Model Studies of Masonry Arch Rib Behaviour at Different Eccentricities. Open Journal of Civil Engineering, 8, 533-543. https://doi.org/10.4236/ojce.2018.84038</p></sec></body><back><ref-list><title>References</title><ref id="scirp.89392-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Roberts, T.M, Hughes, T.G. and Dandamudi, V.R. 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