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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">MC</journal-id>
<journal-title-group>
<journal-title>Materiales de Construcci&#x00F3;n</journal-title>
</journal-title-group>
<issn pub-type="epub">0465-2746</issn>
<publisher>
<publisher-name>Consejo Superior de Investigaciones Cientificas</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">MC201910_e188</article-id>
<article-id pub-id-type="doi">10.3989/mc.2019.04118</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Articles</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>Petrophysical-mechanical behavior of Grisolia stone found in the architectural heritage of southern Italy</article-title>
<trans-title-group xml:lang="es">
<trans-title>Comportamiento petrof&#x00ED;sico-mec&#x00E1;nico de la piedra de Grisolia del patrimonio arquitect&#x00F3;nico del sur de Italia</trans-title>
</trans-title-group>
<alt-title alt-title-type="running-head">Petrophysical-mechanical behavior of Grisolia stone found in the architectural heritage of southern Italy</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Forestieri</surname>
<given-names>G.</given-names>
</name>
<xref ref-type="aff" rid="aff0001">a</xref>
<xref ref-type="corresp" rid="cor1">&#x002A;</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Alvarez de Buergo</surname>
<given-names>M.</given-names>
</name>
<xref ref-type="aff" rid="aff0002">b</xref>
</contrib>
</contrib-group>
<aff id="aff0001"><label>a</label>Facultad de Ingenier&#x00ED;a, Universidad de la Sabana, Campus Universitario del Puente del Com&#x00FA;n, (Ch&#x00ED;a, Cundinamarca, Colombia)</aff>
<aff id="aff0002"><label>b</label>Instituto de Geociencias IGEO (CSIC-UCM). Consejo Superior de Investigaciones Cient&#x00ED;ficas &#x2013; Universidad Complutense de Madrid, (Madrid, Spain)</aff>
<author-notes>
<corresp id="cor1"><label>&#x002A;</label><email xlink:href="giulia.forestieri@unisabana.edu.co">giulia.forestieri@unisabana.edu.co</email></corresp>
<fn><p><bold>ORCID ID:</bold> G. Forestieri (<ext-link ext-link-type="uri" xlink:href="https://orcid.org/0000-0003-2557-8637">https://orcid.org/0000-0003-2557-8637</ext-link>); M. &#x00C1;lvarez de Buergo (<ext-link ext-link-type="uri" xlink:href="https://orcid.org/0000-0002-7520-2390">https://orcid.org/0000-0002-7520-2390</ext-link>)</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>30</day>
<month>06</month>
<year>2019</year>
</pub-date>
<pub-date pub-type="collection">
<year>2019</year>
</pub-date>
<volume>69</volume>
<issue>334</issue>
<elocation-id content-type="doi">10.3989/mc.2019.04118</elocation-id>
<history>
<date date-type="received">
<day>18</day>
<month>04</month>
<year>2018</year>
</date>
<date date-type="accepted">
<day>27</day>
<month>11</month>
<year>2018</year>
</date>
<date date-type="Available on line">
<day>03</day>
<month>04</month>
<year>2019</year>
</date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2019 CSIC</copyright-statement>
<copyright-year>2019</copyright-year>
<license license-type="open-access" xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution 4.0 International (CC BY 4.0) License.</license-p>
</license>
</permissions>
<abstract>
<title>ABSTRACT</title>
<p>Grisolia is one of the building stones most commonly found in the architectural heritage of southern Italy. Also known commercially as &#x201C;gold stone&#x201D; for its yellow intrusions, Grisolia was employed by the leading Calabrian schools of stonemasons, principally in the southern Italian regions of Calabria and Basilicata. It is an Upper Triassic crystalline carbonate quarried in the Verbicaro Unit on Calabria&#x2019;s northern Tyrrhenian coast.</p>
<p>Possessing petrographic, physical and mechanical properties that ensure stone strength and durability, it is a high-quality building material suitable for structural and ornamental uses. These properties can be attributed to its low open porosity and excellent hydric behavior (low capillary water absorption), as well as to its high mechanical strength and low anisotropy. These characteristics make it recommendable as a building material for both restoration and new construction.</p>
</abstract>
<trans-abstract xml:lang="es">
<title>RESUMEN</title>
<p><italic>Comportamiento petrof&#x00ED;sico-mec&#x00E1;nico de la piedra de Grisolia del patrimonio arquitect&#x00F3;nico del sur de Italia</italic> La &#x201C;piedra de Grisolia&#x201D; es una de las piedras de construcci&#x00F3;n m&#x00E1;s utilizadas en el patrimonio arquitect&#x00F3;nico del sur de Italia. Tambi&#x00E9;n conocida comercialmente como &#x201C;piedra de oro&#x201D; por su color dorado, fue empleada por las m&#x00E1;s importantes escuelas de canter&#x00ED;a, principalmente en las regiones italianas del sur, Calabria y Basilicata. Se trata de un carbonato cristalino del Tri&#x00E1;sico Superior extra&#x00ED;do en la Unidad Verbicaro, en la costa Tirr&#x00E9;nica del norte de Calabria.</p>
<p>Gracias a sus propiedades petrogr&#x00E1;ficas, f&#x00ED;sicas y mec&#x00E1;nicas que aseguran su resistencia y durabilidad, es un material de alta calidad adecuado para fines estructurales y ornamentales. Estas propiedades se deben a su baja porosidad, excelente comportamiento h&#x00ED;drico - baja absorci&#x00F3;n capilar -, as&#x00ED; como a su alta resistencia mec&#x00E1;nica y baja anisotrop&#x00ED;a. Gracias a esas buenas propiedades, se recomienda su empleo como material de construcci&#x00F3;n tanto para la recuperaci&#x00F3;n de edificios antiguos as&#x00ED; como para la construcci&#x00F3;n de obra nueva.</p></trans-abstract>
<kwd-group xml:lang="en">
<title>KEYWORDS</title>
<kwd>Limestone</kwd>
<kwd>Characterization</kwd>
<kwd>Physical properties</kwd>
<kwd>Mechanical properties</kwd>
</kwd-group>
<kwd-group xml:lang="es">
<title>PALABRAS CLAVE</title>
<kwd>Caliza</kwd>
<kwd>Caracterizaci&#x00F3;n</kwd>
<kwd>Propiedades f&#x00ED;sicas</kwd>
<kwd>Propiedades mec&#x00E1;nicas</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="sec1" sec-type="intro">
<title>1. INTRODUCTION</title>
<p>For centuries, Grisolia stone (DG) has been used as a building material both in the towns of the Upper Tyrrhenian part of Calabria (particularly in the province of Cosenza) and throughout the historic centers of the neighboring Basilicata region (<xref ref-type="bibr" rid="cit0001">1</xref>).</p>
<p>This stone has long been employed not only in vernacular construction in the above-mentioned towns, but also in construction of the major religious and aristocratic buildings that form part of Calabria&#x2019;s architectural heritage. One of the foremost of these is the church of San Francesco (14th century) in Aieta, in which Grisolia stone provides the main building material. Other examples of aristocratic Calabrian architecture are the famous Principi Spinelli (13th century) and Martirano-Spinelli (14th century) palaces (<xref ref-type="fig" rid="f0001">Figure 1</xref>) in Scalea and Aieta, respectively. Grisolia stone has been employed for both decorative purposes (elements of palace fa&#x00E7;ades and portals) and structural uses (masonry, arches and retaining walls).</p>
<fig id="f0001">
<label>Figure 1</label>
<caption>
<p>&#x201C;Spinelli&#x2019;s Prince Palace&#x201D; of the 13<sup>th</sup> century in Scalea and &#x201C;Martirano-Spinelli Palace&#x201D; of the 14<sup>th</sup> century in Aieta, southern Italy, built with Grisolia stone.</p>
</caption>
<graphic xlink:href="MC201910_e188-g001.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>Over the centuries, this building material has been quarried extensively and, in the Pollino and coastal Tyrrhenian ranges in particular, this lithology has also been used to produce artificial stone. Commercially, Grisolia stone, also known as &#x201C;gold stone&#x201D; for its yellow intrusions (<xref ref-type="bibr" rid="cit0002">2</xref>), which are visible to the naked eye and are probably due to impurities, was also used as a &#x201C;comparing stone&#x201D; to judge the purity of silver or gold.</p>
<p>Macroscopically, Grisolia stone is a compact, deep-grey limestone. The stone varieties differ only in slight variations in tone, which ranges from dark grey to greenish bronze.</p>
<p>Due to Grisolia stone&#x2019;s historical and architectural importance, several authors have studied it extensively from a geological point of view (<xref ref-type="bibr" rid="cit0003">3</xref>&#x2013;<xref ref-type="bibr" rid="cit0006">6</xref>). Nevertheless, complete petrophysical and mechanical characterization has not yet been performed. This paper focuses on complete characterization of this stone in order to highlight its properties and encourage its use as a building stone in both conservation of heritage and construction of new buildings.</p>
</sec>
<sec id="sec2">
<title>2. GEOLOGICAL SETTING</title>
<p>Geologically, Grisolia stone is part of the carbonatic deposits of the Upper Triassic found in the Verbicaro Unit (39&#x00B0;45&#x2032;N and 15&#x00B0;54&#x2032;E) (<xref ref-type="bibr" rid="cit0003">3</xref>) (<xref ref-type="fig" rid="f0002">Figure 2</xref>). These deposits are also referred to as &#x201C;Trias Dolomitique&#x201D; (<xref ref-type="bibr" rid="cit0007">7</xref>) or &#x201C;dark dolostones&#x201D; (<xref ref-type="bibr" rid="cit0004">4</xref>). The upper part of the Verbicaro Unit, which corresponds to the Grisolia Formation, is characterized by a succession of grey limestones alternating with yellowish/reddish argillites and marls (<xref ref-type="bibr" rid="cit0005">5</xref>). The Grisolia Formation extends from the Lao river to Papasidero, with outcrops found in the Serra la Limpida mountains and between the Lao river and the road that connects Santa Domenica Talao to Papasidero.</p>
<fig id="f0002">
<label>Figure 2</label>
<caption>
<p>Geological sketch map of Verbicaro Unit of the Upper Triassic and localization of &#x201C;Anania quarry&#x201D; in Grisolia, southern Italy.</p>
</caption>
<graphic xlink:href="MC201910_e188-g002.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>It is considered a transitional stone positioned between dark dolostone and grey limestone and has an average thickness of 50&#x2013;60 m (<xref ref-type="bibr" rid="cit0004">4</xref>). The Grisolia Formation is composed of clayschists, quartzarenites and crystalline carbonates that are dark grey in color and contain microfossils (<xref ref-type="bibr" rid="cit0005">5</xref>).</p>
<p>In the Verbicaro Unit, Grisolia stone was traditionally quarried in large blocks for ornamental use, while other limestones and dolostones were mainly used for aggregates. Although quarries were scattered throughout the area bounded by the towns of S. Maria del Cedro, Grisolia, Cetraro, Guardia Piemontese, Fuscaldo, Paola, San Lucido and Belmonte Calabro, most of the stone was quarried within the municipal districts of Verbicaro and Grisolia.</p>
</sec>
<sec id="sec3" sec-type="methods">
<title>3. METHODS</title>
<p>Petrophysical, mineralogical and mechanical characterization of the crystalline carbonates taken from the active Anania quarry (39&#x00B0;43&#x2019;N and 15&#x00B0;51&#x2019;E) (<xref ref-type="fig" rid="f0003">Figure 3</xref>) were carried out on a set of specimens collected at two different levels of the quarry in Grisolia. Characterization was performed on two blocks per level, taking into account the macroscopic features.</p>
<fig id="f0003">
<label>Figure 3</label>
<caption>
<p>Active quarry &#x201C;Anania&#x201D; in Grisolia, southern Italy.</p>
</caption>
<graphic xlink:href="MC201910_e188-g003.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>Quarry blocks were cut with a diamond cutting wheel to obtain specimens with shapes and dimensions specific to each test. Specimens were labelled with the letters &#x201C;DG&#x201D; (indicating &#x201C;Grisolia dolostone&#x201D;) and were numbered in ascending order (<xref ref-type="bibr" rid="cit0004">4</xref>). For each sample, splitting planes were determined in the quarry according both to the coordinate reference system established for the three orthogonal directions (X, Y and Z) and to stratification.</p>
<p>The number of samples used for each analysis was set according to the existing European standard (EN). Thin sections for petrographic analysis (<xref ref-type="bibr" rid="cit0008">8</xref>) were cut according to the splitting planes, considering the anisotropy of the rock (one thin section was cut along the XY quarry plane and the other two, perpendicular to the first one, were cut along the YZ and the XZ planes, respectively) (<xref ref-type="fig" rid="f0004">Figure 4a</xref>).</p>
<fig id="f0004">
<label>Figure 4</label>
<caption>
<p>Schematic representation of splitting planes (a) and capillary water absorption test along the X and Z direction (b).</p>
</caption>
<graphic xlink:href="MC201910_e188-g004.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>Specimen lengths were measured in the three orthogonal directions with a Mitutoyo digital caliper with a precision of &#x00B1;0.01 mm. Measurements were taken in each of the three orthogonal directions and averaged.</p>
<p>Petrographic analysis was performed on uncovered and polished thin sections using an Olympus BX 51 polarized light microscope (PM) fitted with a DP 12-coupled camera. Analysis aimed to identify primary minerals and to describe stone samples in petrographical terms. A mineralogical study of the samples was conducted using X-Ray Diffraction (XRD) analysis. The XRD analysis was carried out using a Bruker diffractometer (D8 Advance) coupled to a copper tube. The diffractograms obtained were studied using qualitative and quantitative analysis software (PC-ADP DIFFRACTION).</p>
<p>Physical-mechanical characterization was performed using analytical methodologies: mercury intrusion porosimetry (MIP), chromatic analysis, capillary water absorption test, ultrasonic pulse velocity test (UPV), uniaxial compressive strength test (UCS) and flexural strength test (FST).</p>
<p>Pore diameter distribution, total cumulative mercury volume, average pore diameter and open porosity were determined by MIP. This test, performed using a Micromeritics Autopore IV mercury porosimeter, furnished information about pore specific surface and apparent and skeletal density. Regarding pore size, the Ordaz and Esbert classification for stone decay (<xref ref-type="bibr" rid="cit0009">9</xref>) was used, which differentiates between micropores (&#x003C; 7.5 &#x03BC;m) and macropores (&#x003E; 7.5 &#x03BC;m). Nine prismatic samples measuring 0.5 &#x00D7; 0.5 &#x00D7; 0.8 cm were prepared for MIP analysis.</p>
<p>Chromatic analysis was carried out on the surface specimens with the aid of a spectrophotometer (Minolta CM-700d) and Color Data Spectramagic TM NX CM-S100W software to obtain the color parameters for the CIE 1976 L&#x002A;a&#x002A;b&#x002A; system (L&#x002A; = lightness; a&#x002A; = green/red coordinates; b&#x002A; = blue/yellow coordinates; C&#x002A; = chroma parameter; the function of the a&#x002A; and b&#x002A; values is given by the formula C&#x002A; = &#x221A;(<italic>a</italic>&#x002A;<sup>2</sup> + <italic>b</italic>&#x002A;<sup>2</sup>)). Eight cubic specimens of 50 mm (&#x00B1; 5 mm) per side were used for chromatic analysis (<xref ref-type="bibr" rid="cit0010">10</xref>). Thirty readings were taken from each cubic specimen (five readings per cube face) in order to provide an average representative result.</p>
<p>The same eight cubic specimens of 50 mm (&#x00B1; 5 mm) per side employed for the non-destructive chromatic analysis were used for the capillary water absorption (<xref ref-type="bibr" rid="cit0011">11</xref>), UPV (<xref ref-type="bibr" rid="cit0012">12</xref>) and UCS tests (<xref ref-type="bibr" rid="cit0013">13</xref>).</p>
<p>The capillary water absorption test was carried out on cubic specimens aligned in the two anisotropic directions (X and Z). Specimens were placed in water of a depth of 3 mm (&#x00B1;1 mm) and the weight increase due to water absorption was measured at the time intervals stipulated in the corresponding standards until constant mass was reached (<xref ref-type="bibr" rid="cit0011">11</xref>) (<xref ref-type="fig" rid="f0004">Figure 4b</xref>). In order to describe the capillary water absorption behavior of the material, capillary coefficients parallel and perpendicular to the stratification planes (X and Z, respectively, obtaining C<sub>2</sub> and C<sub>1</sub>, respectively) and the average coefficient Cc were evaluated according to the Snethlage classification (<xref ref-type="bibr" rid="cit0014">14</xref>). The stones were then classified as &#x201C;slightly absorbing&#x201D; (Cc &#x003C; 8 g/m<sup>2</sup>s<sup>0.5</sup>), &#x201C;medium absorbing&#x201D; (Cc &#x003C; 8&#x2013;50 g/m<sup>2</sup>s<sup>0.5</sup>) or &#x201C;highly absorbing&#x201D; (Cc &#x003E; 80 g/m<sup>2</sup>s<sup>0.5</sup>). Water-related properties and parameters provide an insight into the behavior of the stone when exposed to the action of fluids, in particular water, and can be used to predict the stone&#x2019;s propensity to decay in the future (<xref ref-type="bibr" rid="cit0015">15</xref>).</p>
<p>The UPV values were obtained to an accuracy of 0.1 microseconds using the portable, non-destructive MATEST Meter Ver equipment fitted with two 55-kHz frequency transducers (diameter of 1.5 cm). During measurement, in order to improve coupling of the transducers (transmitter and receiver) to the surface of the stone substrate, a Farnell ultrasound couplant gel was applied to the opposing faces of the cubic samples. Direct mode was used, placing both transducers in parallel and on opposite sides of the specimens. UPV determination was performed in each of the three orthogonal directions &#x2014;X, Y and Z&#x2014; of the cubic specimens in order to analyze the spatial variation of the UPV. The anisotropy indices were also evaluated (<xref ref-type="bibr" rid="cit0016">16</xref>): total anisotropy (dM<sub>UPV</sub>%) &#x2014;using the three directions&#x2014; and relative or bi-dimensional anisotropy (dm<sub>UPV</sub>%). Five measurements were taken in each of the three orthogonal directions and averaged (<xref ref-type="bibr" rid="cit0012">12</xref>).</p>
<p>UCS (<xref ref-type="bibr" rid="cit0013">13</xref>) was performed using the MFL SYSTEM testing machine at a constant speed of 1 mm/min and a maximum load capacity of 3000 kg. UCS under unconfined conditions was performed in the three spatial directions: X, Y, and Z. The corresponding UCS<sub>max,X</sub>, UCS<sub>max,Y,</sub> and UCS<sub>max,Z</sub> values were calculated as the ratio between the maximum applied compressive load at failure and the cross-sectional area of the tested specimens. The UCS<sub>mean</sub> value, characteristic of each stone type, was calculated as the average value (<xref ref-type="bibr" rid="cit0017">17</xref>) and the strength anisotropy was evaluated as the ratio of UCS<sub>max</sub>/UCS<sub>min</sub>.</p>
<p>For the FST, the three-point-load bending test was performed. For each direction, eight parallelepiped specimens measuring 300 &#x00D7; 50 &#x00D7; 50 mm (&#x00B1; 5 mm) were loaded to failure using an INSTRON 1195 testing machine at a maximum load capacity of 5000 kg and at a constant speed of 1 mm/min. For each specimen, the test was performed along the three splitting planes. The FST value of each sample was calculated according to current standards (<xref ref-type="bibr" rid="cit0018">18</xref>). In addition, the anisotropic FST index was evaluated as the ratio of the maximum and minimum values within the three spatial directions.</p>
<p>The mechanical strength values were compared against the Anon classification (<xref ref-type="bibr" rid="cit0019">19</xref>, <xref ref-type="bibr" rid="cit0020">20</xref>, <xref ref-type="bibr" rid="cit0021">21</xref>), classifying stones as &#x201C;moderately strong&#x201D; (UCS of 12.5&#x2013;50 MPa), &#x201C;strong&#x201D; (UCS of 50&#x2013;100 MPa), &#x201C;very strong&#x201D; (UCS of 100&#x2013;200 MPa) and &#x201C;low&#x201D; (FST of &#x003C; 5 MPa), &#x201C;moderate&#x201D; (FST of 5&#x2013;10 MPa), &#x201C;high&#x201D; (FST of 10&#x2013;15 MPa) and &#x201C;very high&#x201D; (FST of &#x003E; 15 MPa) to define the quality of the building stone.</p>
</sec>
<sec id="sec4" sec-type="results">
<title>4. RESULTS</title>
<sec id="sec4.1">
<title>4.1. Petrographic and mineralogical characterization</title>
<p>Petrographically, Grisolia stone was revealed to be a compact limestone with very low porosity. It showed a non-recognizable depositional texture and an intense level of diagenesis. It could be classified as a &#x201C;crystalline carbonate&#x201D; (<xref ref-type="bibr" rid="cit0022">22</xref>). Although it was fine-grained, it showed coarser calcite crystals near the veins. Its microstructure was very dense and no porosity was detected under the optical microscope (<xref ref-type="fig" rid="f0005">Figure 5</xref>).</p>
<fig id="f0005">
<label>Figure 5</label>
<caption>
<p>Micrographs under the polarized optical microscope of the analyzed thin sections of Grisolia stone, parallel (//) and crossed nicols (&#x2534;), from left to right, respectively.</p>
</caption>
<graphic xlink:href="MC201910_e188-g005.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>The diagenetic process &#x2014;due to recrystallization&#x2014; could be related to neomorphism, in particular to aggrading neomorphism, which provoked formation of coarser crystalline mosaics (<xref ref-type="bibr" rid="cit0023">23</xref>). The micritic matrix was replaced by a neomorphic pseudosparite (crystal size of between 10 and 50 &#x03BC;m), distinguishable by the irregular distribution of the granulometry composed of coarse mosaics and fine-grained areas.</p>
<p>Analysis of the thin sections in the three directions (X, Y and Z) did not reveal any significant differences, at least at this microscopic level and considering the reduced area analyzed in the thin sections. In this crystalline limestone, diagenesis was governed by recrystallization and cementation processes that eliminated primary (inter- and intraparticle) porosity and generated secondary porosity in which the pore size distribution was homogeneous and the pores were partially sealed as a result of later cementation, as occurred in limestones and calcarenites (<xref ref-type="bibr" rid="cit0024">24</xref>).</p>
<p>The XRD results revealed that calcite is the main mineral. Dolomite was detected only in very small amounts.</p>
</sec>
<sec id="sec4.2">
<title>4.2. Physical-mechanical characterization</title>
<p>The MIP results and colorimetric values obtained are given in <xref ref-type="table" rid="t0001">Table 1</xref>. Skeletal and bulk densities were very similar and typical of carbonate rocks containing calcite in particular (<xref ref-type="bibr" rid="cit0014">14</xref>). The porosity was probably due to the presence of secondary fissures (<xref ref-type="bibr" rid="cit0014">14</xref>), as demonstrated by the low open porosity (p<sub>o</sub>) and the high compactness index (defined as the ratio between real density and bulk density). Average pore diameter corresponded to the range of macroporosity (76%) (<xref ref-type="bibr" rid="cit0008">8</xref>) with a unimodal distribution (<xref ref-type="fig" rid="f0006">Figure 6</xref>). These low porosity values were similar to stones with a crystalline texture such as granite and marble and were lower than ornamental limestones (<xref ref-type="bibr" rid="cit0024">24</xref>, <xref ref-type="bibr" rid="cit0025">25</xref>, <xref ref-type="bibr" rid="cit0026">26</xref>).</p>
<table-wrap id="t0001">
<label>Table 1</label>
<caption>
<p>Physical parameters obtained by MIP test: skeletal density (&#x03C1;<sub>sk</sub>) and bulk density (&#x03C1;<sub>b</sub>) in kg/m<sup>3</sup>; open porosity to mercury (p<sub>o</sub>) in %; compactness index (I<sub>c</sub>) in %; average pore diameter (D) in &#x00B5;m. Chromatic parameters: L&#x002A; = lightness; a&#x002A; = green/red coordinate; b&#x002A; = blue/yellow coordinate; C&#x002A; = chroma.</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<th align="left"/>
<th align="center">q<sub>sk</sub></th>
<th align="center">q<sub>b</sub></th>
<th align="center">p<sub>o</sub></th>
<th align="center">I<sub>c</sub></th>
<th align="center">D</th>
<th align="center">L&#x002A;<sub>(D65)</sub></th>
<th align="center">a&#x002A;<sub>(D65)</sub></th>
<th align="center">b&#x002A;<sub>(D65)</sub></th>
<th align="center">C&#x002A;<sub>(D65)</sub></th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">mean value</td>
<td align="center">2720</td>
<td align="center">2700</td>
<td align="center">0.54</td>
<td align="center">0.99</td>
<td align="center">0.70</td>
<td align="center">71.27</td>
<td align="center">&#x2212;0.24</td>
<td align="center">&#x2212;1.38</td>
<td align="center">1.96</td>
</tr>
<tr>
<td align="left"><italic>st.dev.</italic></td>
<td align="center"><italic>101</italic></td>
<td align="center"><italic>110</italic></td>
<td align="center"><italic>0.08</italic></td>
<td align="center"><italic>0.01</italic></td>
<td align="center"><italic>0.03</italic></td>
<td align="center"><italic>1.11</italic></td>
<td align="center"><italic>0.16</italic></td>
<td align="center"><italic>1.45</italic></td>
<td align="center"><italic>0.48</italic></td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="f0006">
<label>Figure 6</label>
<caption>
<p>Pore size distribution curves [Log differential intrusion (mL/g) vs. pore size diameter (&#x03BC;m)] obtained by MIP analysis.</p>
</caption>
<graphic xlink:href="MC201910_e188-g006.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>The chromatic parameters revealed Grisolia stone to be homogeneous (due to the low standard deviations) (<xref ref-type="table" rid="t0001">Table 1</xref>).</p>
<p>The capillary water absorption coefficients obtained were, respectively, 1.22 + 0.12 g/m<sup>2</sup>s<sup>0.5</sup> for C1 and 1.29 + 0.22 g/m<sup>2</sup>s<sup>0.5</sup> for C2 corresponding to the &#x201C;slightly absorbing&#x201D; stone classification (<xref ref-type="bibr" rid="cit0014">14</xref>). Capillary water absorption was found to be very low, a common characteristic in highly compact crystalline stones (<xref ref-type="fig" rid="f0007">Figure 7</xref>). Analyzing capillary absorption revealed how the stone&#x2019;s hydric behavior was quite similar in the two directions studied, demonstrating an isotropic hydric absorption trend. Moreover, macropores, which are often found in limestones like DG and were detected by MIP, influenced water absorption capability and aided water evaporation (<xref ref-type="bibr" rid="cit0014">14</xref>). The results of the hydric tests were directly related to the stone texture formed during the diagenesis stage.</p>
<fig id="f0007">
<label>Figure 7</label>
<caption>
<p>Capillary water absorption curves along the X and Z directions.</p>
</caption>
<graphic xlink:href="MC201910_e188-g007.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>UPV was used to find the absolute and relative anisotropy indices. The anisotropy values obtained (<xref ref-type="table" rid="t0002">Table 2</xref>) were considerably lower than those reported for other carbonate stones (<xref ref-type="bibr" rid="cit0027">27</xref>, <xref ref-type="bibr" rid="cit0028">28</xref>). UPV values in the three directions (X, Y and Z) were very similar and indicative of DG&#x2019;s low anisotropy. Moreover, the high UPV values demonstrated the high compactness of the stone and were related to the &#x201C;high velocity class&#x201D;. UPV depended largely on stone characteristics such as mineralogical composition, porosity and fracture density (<xref ref-type="bibr" rid="cit0029">29</xref>). The high UPV values observed were indicative of DG&#x2019;s high dynamic quality (<xref ref-type="bibr" rid="cit0030">30</xref>, <xref ref-type="bibr" rid="cit0031">31</xref>).</p>
<table-wrap id="t0002">
<label>Table 2</label>
<caption>
<p>UPV<sub>x</sub>, UPV<sub>y</sub>, UPV<sub>z</sub> = ultrasonic pulse velocity (m/s) recorded in the X, Y and Z directions, respectively; UPV= average ultrasonic pulse velocity (m/s); dM<sub>UPV</sub>% = total anisotropy index; and dm<sub>UPV</sub>% = relative anisotropy index.</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<th align="left"/>
<th align="center">UPV<sub>X</sub> (m/s)</th>
<th align="center">UPV<sub>Y</sub> (m/s)</th>
<th align="center">UPV<sub>Z</sub> (m/s)</th>
<th align="center">UPV(m/s)</th>
<th align="center">dM<sub>UPV</sub> (%)</th>
<th align="center">dm<sub>UPV</sub> (%)</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">mean value</td>
<td align="center">6633</td>
<td align="center">6600</td>
<td align="center">6542</td>
<td align="center">6592</td>
<td align="center">1.1</td>
<td align="center">0.5</td>
</tr>
<tr>
<td align="left"><italic>st.dev.</italic></td>
<td align="center"><italic>56</italic></td>
<td align="center"><italic>76</italic></td>
<td align="center"><italic>73</italic></td>
<td align="center"><italic>76</italic></td>
<td align="center"><italic>0.5</italic></td>
<td align="center"><italic>0.5</italic></td>
</tr>
</tbody>
</table>
</table-wrap>
<p>Under mechanical stress, DG proved to be fragile. Young&#x2019;s modulus (E), determined from the stress&#x2013;strain curves, depended slightly on the orientation of the specimen with respect to the bedding plane. E values ranged from 83 GPa to 85 GPa (<xref ref-type="table" rid="t0003">Table 3</xref>) and were higher when compared to similar resistant limestones (<xref ref-type="bibr" rid="cit0015">15</xref>). The respective Poisson coefficients (&#x03C5;) varied from 0.34 to 0.35, with the highest value registered when the force was applied perpendicularly to the bedding plane. The values for the three orthogonal directions presented few differences, corroborating the low total anisotropy value obtained above. UCS values presented slight differences in the three spatial directions. This fact was in agreement with the low anisotropy ratio, DG&#x2019;s homogeneous features and its ultrasonic isotropic behavior. The maximum value of UCS was recorded along the Z-axis, the intermediate value was recorded along the Y-axis and the minimum value was recorded along the X-axis, with the averaged value corresponding to &#x201C;strong&#x201D; stone. The stress&#x2013;strain curves in unconfined state (<xref ref-type="fig" rid="f0008">Figure 8</xref>) for the two directions analyzed showed that the behavior of the stone samples was almost quasi-linear elastic until failure. Graphically, the initial tangent modulus (i.e. the slope of the initial part of the stress&#x2013;strain curve) remained almost equal to the tangent modulus at 50 % of the failure strength. Furthermore, samples showed the same quasi-elastic behavior along the two axes. The only difference appeared for the strain part, which was longer in the Z-direction than the X-direction. Regarding the schematic representation of the failure orientations (<xref ref-type="fig" rid="f0009">Figure 9</xref>), the specimens broke in three different ways: splitting, shear, and splitting and shear. No difference was observed in the three directions analyzed and the difference in mode failure was probably due to the presence or absence of internal weak planes. Fractures were long, extended for the height of the sample and ran mainly parallel to the direction of loading. In the case of shear failure, fractures were oriented towards the inside of the sample. After the rupture, the sample presented an hourglass shape. Shear failure, i.e. complex conjugate failures (<xref ref-type="bibr" rid="cit0032">32</xref>), occurred along planes of weakness.</p>
<table-wrap id="t0003">
<label>Table 3</label>
<caption>
<p>E<sub>x</sub>, E<sub>y</sub>, E<sub>z</sub> = Young&#x2019;s modulus (GPa); &#x03C5;<sub>x</sub>, &#x03C5;<sub>y</sub>, &#x03C5;<sub>z</sub> = Poisson coefficient recorded in the directions X, Y and Z, respectively; UCS<sub>x</sub>, UCS<sub>y</sub>, UCS<sub>z</sub> = uniaxial compressive strength (MPa) and; UCS = average uniaxial compressive strength (MPa); and max/min = anisotropy UCS strength ratio.</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<th align="left"/>
<th align="center">E<sub>X</sub></th>
<th align="center">E<sub>Y</sub></th>
<th align="center">E<sub>Z</sub></th>
<th align="center">t<sub>X</sub></th>
<th align="center">t<sub>Y</sub></th>
<th align="center">t<sub>Z</sub></th>
<th align="center">UCS<sub>X</sub></th>
<th align="center">UCS<sub>Y</sub></th>
<th align="center">UCS<sub>Z</sub></th>
<th align="center">UCS</th>
<th align="center">max/min</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">mean value</td>
<td align="center">83</td>
<td align="center">84</td>
<td align="center">85</td>
<td align="center">0.34</td>
<td align="center">0.34</td>
<td align="center">0.35</td>
<td align="center">60</td>
<td align="center">64</td>
<td align="center">65</td>
<td align="center">63</td>
<td align="center">1.1</td>
</tr>
<tr>
<td align="left"><italic>st.dev.</italic></td>
<td align="center"><italic>1</italic></td>
<td align="center"><italic>2</italic></td>
<td align="center"><italic>1</italic></td>
<td align="center"><italic>0.01</italic></td>
<td align="center"><italic>0.02</italic></td>
<td align="center"><italic>0.01</italic></td>
<td align="center"><italic>2</italic></td>
<td align="center"><italic>1</italic></td>
<td align="center"><italic>2</italic></td>
<td align="center"><italic>2</italic></td>
<td align="center"/>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="f0008">
<label>Figure 8</label>
<caption>
<p>Stress-strain curve under UCS unconfined conditions, along the X and Z directions.</p>
</caption>
<graphic xlink:href="MC201910_e188-g008.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<fig id="f0009">
<label>Figure 9</label>
<caption>
<p>Diagrammatic view of the fractures developed in DG specimens under UCS conditions: splitting (a); shear (b); splitting and shear (c).</p>
</caption>
<graphic xlink:href="MC201910_e188-g009.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>FST values were in line with the values reported for other building stones with similar textural and compositional characteristics (<xref ref-type="bibr" rid="cit0025">25</xref>). As was the case for UCS, no significant differences were noticed in the three directions, with the highest values being reached on the Z-axis (<xref ref-type="table" rid="t0004">Table 4</xref>). According to the mean value of FST, DG corresponded to the &#x201C;high&#x201D; flexural strength class (<xref ref-type="bibr" rid="cit0019">19</xref>, <xref ref-type="bibr" rid="cit0020">20</xref>, <xref ref-type="bibr" rid="cit0021">21</xref>). When compared to UCS, under FST conditions DG exhibited greater anisotropic behavior, as shown by the higher FST anisotropy ratio (1.6 <italic>vs.</italic> 1.1).</p>
<table-wrap id="t0004">
<label>Table 4</label>
<caption>
<p>FST<sub>x</sub>, FST<sub>y</sub>, FST<sub>z</sub> = flexural strength resistance (MPa) recorded in the directions X, Y and Z, respectively; FST = average flexural strength (MPa); and max/min = anisotropy FST strength ratio.</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<th align="left"/>
<th align="center">FST<sub>X</sub></th>
<th align="center">FST<sub>Y</sub></th>
<th align="center">FST<sub>Z</sub></th>
<th align="center">FST</th>
<th align="center">max/min</th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">mean value</td>
<td align="center">9</td>
<td align="center">13</td>
<td align="center">15</td>
<td align="center">12</td>
<td align="center">1.6</td>
</tr>
<tr>
<td align="left"><italic>st.dev.</italic></td>
<td align="center"><italic>1</italic></td>
<td align="center"><italic>1</italic></td>
<td align="center"><italic>2</italic></td>
<td align="center"><italic>2</italic></td>
<td align="center"/>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec id="sec5" sec-type="discussion">
<title>5. DISCUSSION</title>
<p>From a petrographic point of view, the existence of veins and crystals of differing sizes &#x2014;thin and thick&#x2014; means that DG is neither homogenous nor isotropic. Rather, it is somewhat heterogeneous. Its relative textural heterogeneity (veins and crystal size, areas of large crystals and areas of fine crystals) may be responsible for the anisotropy (albeit low) and may also be responsible for the non-optimal correlations. Regarding capillary behavior, even though the anisotropy is low, it seems to condition capillary absorption, as shown in <xref ref-type="fig" rid="f0007">Figure 7</xref> where, based on the X-direction, DG would be expected to absorb more water after a certain amount of time. The low anisotropy, revealed by the UPV test, also seems to influence mechanical behavior, as shown by the slight differences in UCS and FST values in the three directions analyzed.</p>
<p>Correlations between petrophysical and mechanical properties are obtained (<xref ref-type="fig" rid="f0010">Figure 10</xref>). As expected, the lower the bulk density (&#x03C1;<sub>b</sub>), the lower the mechanical strength. Regarding the relationship between open porosity (p<sub>o</sub>)and UPV (<xref ref-type="fig" rid="f0010">Figure 10a</xref>), it can be said that no strong correlation exists between the above-mentioned properties. Rather, there is only an inverse relationship: the lower the p<sub>o</sub>, the higher the UPV propagation (<xref ref-type="bibr" rid="cit0033">33</xref>). In this case, the inverse correlation does seem strong and linear for UPV. This can be explained by the very low p<sub>o</sub> and by the low standard deviation that influences the very low variability among the values obtained. The low p<sub>o</sub> does not affect the UPV, as demonstrated by the very low values of correlation, considered as statistically insignificant. The non-linear relationship is in agreement with other authors, in particular for carbonate stones such as DG, with low p<sub>o</sub> (&#x003C; 2%) occurring where there is no significant correlation between p<sub>o</sub> and UPV (<xref ref-type="bibr" rid="cit0014">14</xref>). Even though there is not a linear correlation, it is possible to say that an inverse relationship exists between UPV and p<sub>o</sub>, as has also been proved by several authors in various lithological types (<xref ref-type="bibr" rid="cit0034">34</xref>, <xref ref-type="bibr" rid="cit0035">35</xref>).</p>
<fig id="f0010">
<label>Figure 10</label>
<caption>
<p>Relationships between physical and mechanical properties: UPV <italic>vs.</italic> &#x03C1;<sub>b</sub> (a), p<sub>o</sub> (b), UCS (c), FST (d); &#x03C1;<sub>b</sub> <italic>vs</italic>. UCS (e), FST (f); p<sub>o</sub> <italic>vs</italic>. UCS (g), FST (h).</p>
</caption>
<graphic xlink:href="MC201910_e188-g010.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<fig id="f0011">
<label>Figure 11</label>
<caption>
<p>Examples of portals realized with Grisolia stone and affected by slight decay forms.</p>
</caption>
<graphic xlink:href="MC201910_e188-g011.tif" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</fig>
<p>Weak relationships are also reached for p<sub>o</sub> when using UCS and FST (<xref ref-type="fig" rid="f0010">Figures 10d</xref>, <xref ref-type="fig" rid="f0010">10e</xref>), with these possibly being weaker or non-linear. UCS and FST decrease as p<sub>o</sub> increases, as previously stated (<xref ref-type="bibr" rid="cit0035">35</xref>, <xref ref-type="bibr" rid="cit0036">36</xref>). In the case of materials with very low porosity such as DG, no linear relationship exists even though UCS and FST decrease as p<sub>o</sub> increases (but without a linear correlation). This result is in contrast with the results of other researchers investigating lithotypes with low p<sub>o</sub> (<xref ref-type="bibr" rid="cit0035">35</xref>, <xref ref-type="bibr" rid="cit0037">37</xref>), but is in agreement with other researchers (<xref ref-type="bibr" rid="cit0016">16</xref>) who found that other factors, such as variable grain size and not p<sub>o</sub>, seem to be the main causes of the variability of the strength of low porosity stones.</p>
<p>The correlation between UPV and UCS and FSTs is significant. There is a linear relationship between these properties (<xref ref-type="fig" rid="f0010">Figures 10b</xref>, <xref ref-type="fig" rid="f0010">10c</xref>). As expected, the lower the UPV, the lower the UCS (<xref ref-type="bibr" rid="cit0021">21</xref>) and FST (<xref ref-type="bibr" rid="cit0038">38</xref>), and <italic>vice versa</italic>.</p>
<p>Analysis of decay on buildings constructed from DG reveals that decay is insignificant and almost absent. DG&#x2019;s open porosity, which conditions its permeability to fluids (<xref ref-type="bibr" rid="cit0014">14</xref>), combined with the presence of macropores instead of micropores that influence the stone&#x2019;s durability (<xref ref-type="bibr" rid="cit0039">39</xref>), play an important role with respect to the stone&#x2019;s resistance to decay factors. Fluids hardly circulate inside the stone because its low capillary coefficient &#x2014;due to its low porosity&#x2014; makes DG quite impermeable. These same internal features provide adequate protection against pollution ingress. DG&#x2019;s durability is also the result of its excellent mechanical properties and low structural anisotropy index. These make DG better able to endure (<xref ref-type="bibr" rid="cit0039">39</xref>, <xref ref-type="bibr" rid="cit0040">40</xref>, <xref ref-type="bibr" rid="cit0041">41</xref>) the expansion and contraction induced by the mechanical stresses associated with external temperature variations or to endure internal salt-crystallization pressures (<xref ref-type="bibr" rid="cit0042">42</xref>).</p>
<p>Structural flaws, intrinsic discontinuities, surface deposits (<xref ref-type="fig" rid="f0011">Figure 11a</xref>), biological colonization and missing parts (<xref ref-type="fig" rid="f0011">Figure 11b</xref>) are the only forms of decay detected. Crumbling also occurs, although less frequently, and is associated with the structural instability of the entire building rather than with the mechanical strength of its building stone. Thus, restoration and conservation of DG require minimal work, consisting merely of cleaning and repair as necessary. Minor protection and consolidation are also recommended.</p>
</sec>
<sec id="sec6" sec-type="conclusions">
<title>6. CONCLUSIONS</title>
<p>The complete petrophysical and mechanical characterization performed explains why Grisolia stone is a good natural building stone. Petrographically, DG has a heterogenous composition and texture. It is compact and petrographically quite isotropic. In fact, examining the oriented thin sections in the three directions analyzed does not reveal any significant preferential orientation. This is in agreement with the other tests performed where the corresponding anisotropy indices are very low. Similarly, in agreement with the low porosity values, the compactness index is high.</p>
<p>DG&#x2019;s petrographic characteristics, low porosity levels, predominant macroporosity, low water absorption capability, isotropic hydric behavior and high ultrasonic wave velocity stand as proof of the suitability of this stone for use in construction. The only recommended conservation techniques consist of removing stains and other surface deposits and repairing damaged stones.</p>
<p>Its high compressive strength also makes DG an ideal material for structural elements such as pilasters, portals, pedestals, staircases, flooring and baseboards, as well as for pavement cobbles and curbing. Its low strength anisotropy means it can be chiseled into shape and placed in constructions without having to pay attention to stone block orientation. Moreover, thanks to its durability, DG can be employed in both internal and external decorative and structural elements. The degree of conservation of historic buildings made from this material demonstrates that it is also resistant to most of the extrinsic factors that usually damage building stone, such as water, biological agents, salt and air pollution. For all these reasons, its use is recommended in both restoration and new building.</p>
</sec>
</body>
<back>
<ack>
<title>ACKNOWLEDGEMENTS</title>
<p>This study was supported by &#x201C;Programa Geomateriales 2 (S2013/MIT-2914)&#x201D; and by &#x201C;Fondi 5 per mille D.P.C.M. 23/04/2010&#x201D;.</p>
</ack>
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