<?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">AMPC</journal-id><journal-title-group><journal-title>Advances in Materials Physics and Chemistry</journal-title></journal-title-group><issn pub-type="epub">2162-531X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ampc.2018.86018</article-id><article-id pub-id-type="publisher-id">AMPC-85683</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Study of Chromium-Lead-Phosphate Glasses by XRD, IR, Density and Chemical Durability
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Radouan</surname><given-names>Makhlouk</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>Nadia</surname><given-names>Beloued</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>Said</surname><given-names>Aqdim</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Mineral Chemistry Laboratory, Department of Chemistry, Faculty of Science, Hassan II University Ain Chock, Casablanca, Morocco</addr-line></aff><aff id="aff1"><addr-line>Laboratory of Materials Engineering for Environment and Valorization, Faculty of Sciences, Hassan II University Ain Chock, Casablanca, Morocco</addr-line></aff><pub-date pub-type="epub"><day>29</day><month>06</month><year>2018</year></pub-date><volume>08</volume><issue>06</issue><fpage>269</fpage><lpage>280</lpage><history><date date-type="received"><day>13,</day>	<month>April</month>	<year>2018</year></date><date date-type="rev-recd"><day>26,</day>	<month>June</month>	<year>2018</year>	</date><date date-type="accepted"><day>29,</day>	<month>June</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>
 
 
  Glasses in the ternary system Cr<sub>2</sub>O<sub>3</sub>-PbO-P<sub>2</sub>O<sub>5</sub> were prepared by direct melting of the mixture with stoichiometric proportions of the reagents Cr<sub>2</sub>O<sub>3</sub>, PbO and (NH<sub>4</sub>)<sub>2</sub>HPO<sub>4</sub> at 1080
  &amp;#8451;. The glasses obtained are transparent in colour and have a non-hygroscopic appearance. The study of the dissolution rate was carried out on ternary glasses xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> with (1
   
  ≤
   
  x
   
  ≤
   
  4; mol%), immersed in distilled water at 90
  &amp;#8451; for 24 days, indicat
  ing
   a maximum of chemical durability when the level of chromium oxide passed through 2 mol%. Both, IR spectra and X-ray diffraction have indicated the predominance of metaphosphate or cyclic metaphosphate groups with some traces of isolated orthophosphate groups when the Cr<sub>2</sub>O<sub>3</sub> content is equal to x = 2. Analysis of the density values also, ha
  s
   showed a maximum density for x = 2 mol%. The covalent radius values of oxygen ha
  ve
   indicated that the minimum value rcal
   
  (O<sup>2&amp;ndash;</sup>) is observed for x
   
  =
   
  2 mol% and therefore a relatively high reinforcement of the metal-oxygen-phosphorus (Cr-O-P) bonds. SEM Micrographs have exhibited two phases, a vitreous phase and a crystalline phase. The radical change in the structure from ultraphosphate Q<sup>3</sup> groups to ring metaphosphate Q<sup>2</sup> and orthophosphate groups Q<sup>0</sup>
   
  seems to be the cause of the formation of crystallites. Beyond 2 mol% of Cr<sub>2</sub>O<sub>3</sub>, the structure of the glass changed relatively and the orthophosphate phases increased to the detriment of the metaphosphate phases. We observed a decrease in chemical durability. However, it was confirmed that the dissolution rate (D<sub>R</sub>) of the S<sub>2</sub> analysed compound is comparable to the values of borosilicate glasses which are used as alternative materials for the immobilisation of nuclear waste substances.
 
</p></abstract><kwd-group><kwd>Chemical Durability</kwd><kwd> Phosphate Glasses</kwd><kwd> Chromium Oxide</kwd><kwd> IR</kwd><kwd> XRD</kwd><kwd> SEM</kwd><kwd> Nu-clear and Chemical Wastes</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The phosphate-based oxide glasses P<sub>2</sub>O<sub>5</sub>, compared to their silicate homologous, have important properties due to their low preparation temperatures. These properties, such as a low melting point, high coefficient of thermal expansion and optical properties, make these glasses potential candidates for many technological applications such as: medical field (biomaterials), solid electrolytes, vitrification of nuclear waste, etc. [<xref ref-type="bibr" rid="scirp.85683-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.85683-ref10">10</xref>]. The lead iron phosphate glasses used for the disposal of nuclear waste were produced in 1984 [<xref ref-type="bibr" rid="scirp.85683-ref9">9</xref>]. The combination of chromium-doped phosphate glasses with different types of nuclear waste has shown that it is possible to have a waste form with a corrosion rate comparable to that of borosilicate glasses [<xref ref-type="bibr" rid="scirp.85683-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref7">7</xref>]. The previous work performed by our group demonstrated that the substitution of Na<sub>2</sub>O with lead oxide by more than 28 mol%, with the presence of 2 mol% of Cr<sub>2</sub>O<sub>3</sub> in the vitreous lattice appears to be an unfavourable factor for chemical durability. The phenomenon has been explained by the approach of the boundary zone between the crystal and the glass by the continuous formation of groups of isolated phosphate PO 4 3 − [<xref ref-type="bibr" rid="scirp.85683-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref11">11</xref>]. Hence, the crystallites exceed a certain limit, and the equilibrium between the glass bath and these crystallites are not longer maintained; we notice, once, a few decrease in the chemical durability. The purpose of this work is to study the evolution of the dissolution rate as a function of the chromium oxide content in distilled water at 90˚C for the studied glasses of the series xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> with (1 ≤ x ≤ 4; mol%). The study of the dissolution rate, carried out on these glasses, reveals an important chemical durability for the low contents of chromium oxides (2 mol%).</p></sec><sec id="s2"><title>2. Experimental Section</title><p>The synthesis of chromium lead phosphate glasses of composition xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> avec (1 ≤ x ≤ 4; mol%) was carried out by the direct fusion of mixtures of (NH<sub>4</sub>)<sub>2</sub>HPO<sub>4</sub>, Pb(NO<sub>3</sub>)<sub>2</sub> and Cr<sub>2</sub>O<sub>3</sub> in proper proportions. The reagents are finely crushed and then introduced into a porcelain crucible. They are heated to 300˚C for 1 h in the first instance and then to 500˚C for 1 h to complete their decomposition. The reaction mixture is then carried to 1050˚C &#177; 10˚C for 15 min. The liquid obtained is homogeneous. It is then poured on to an aluminium plate previously heated to 200˚C to avoid thermal shocks. The vitreous state was first evidenced from the shiny and transparency aspect, which was then confirmed from the X-ray diffraction (XRD) patterns. Samples S<sub>1</sub>, S<sub>2</sub> and S<sub>4</sub> were respectively annealed at 560˚C and 580˚C, for 72 hours. The chemical durability of these glasses was evaluated by the weight loss of the sample. The samples were polished by glass paper of silica carbon (CSI), cleaned with acetone and immersed in beakers of Pyrex containing 100 ml of distilled water and brought to 90˚C. The surface of the sample must be constantly immersed in the distilled water for 24 days. The density of the glass has been measured at ambient temperature using the Archimedes method. The glass is immersed in a solution of diethyl orthophtalate density, depending on the temperature, is known. The precision is 0.05 g/cm<sup>3</sup>. The density of the glass is given by the following equation:</p><p>ρ = m glass [ m glass + ( m ortho − m ortho + glass ) ] ρ ortho</p><p>with:</p><p>ρ = Density</p><p>m<sub>air</sub> = Weight of glass measured in air</p><p>m<sub>ortho</sub> = Weight of diethyl orthophthalate only</p><p>m<sub> ortho+glass</sub> = Weight of glass immersed in diethyl orthophthalate</p><p>ρ<sub>ortho</sub> = 1.11422 g/cm<sup>3</sup></p><p>The infrared spectra of the phosphate glasses studied have been determined in the region between 1600 and 400 cm<sup>−</sup><sup>1</sup> with a resolution of 2 cm<sup>−</sup><sup>1</sup>. The samples were finely ground and mixed with KBr (potassium bromide), which is transparent in the infrared, and whose role was to serve as a matrix.</p><p>Chemical composition of the departure mixture and some characteristics of the quaternary glasses, are summarized in <xref ref-type="table" rid="table1">Table 1</xref>.</p></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Analysis of Chemical Durability of Series xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub></title><p>The chemical durability (D<sub>R</sub>) of the glass is strongly dependent on its composition, in the case of the glass of the xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> composition series, the approximate durability analysis is carried out by measuring the dissolution rate (D<sub>R</sub>), which is defined as the weight loss of the glasses in g・cm<sup>−</sup><sup>2</sup>・min<sup>−</sup><sup>1</sup>. The D<sub>R</sub> values shown in <xref ref-type="table" rid="table1">Table 1</xref> show a very low dissolution rate for low levels of chromium oxide (2 mol% of Cr<sub>2</sub>O<sub>3</sub>) introduced into the phosphate network to the detriment of PbO. The substitution of PbO by Cr<sub>2</sub>O<sub>3</sub> for more than 2 mol% becomes an unfavourable factor for D<sub>R</sub>. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the variation in the</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Compositions, density and chemical durability of xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> with (1 ≤ x ≤ 4; mol%)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Glass sample</th><th align="center" valign="middle"  colspan="3"  >Starting glass composition (mol%)</th><th align="center" valign="middle" >O/P ratio</th><th align="center" valign="middle" >(D<sub>R</sub>) (g・cm<sup>−</sup><sup>2</sup>・min<sup>−</sup><sup>1</sup>)</th><th align="center" valign="middle" >ρ (g/cm<sup>3</sup>)</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >Cr<sub>2</sub>O<sub>3</sub></td><td align="center" valign="middle" >PbO</td><td align="center" valign="middle" >P<sub>2</sub>O<sub>5</sub></td><td align="center" valign="middle" ></td><td align="center" valign="middle" >24 days</td><td align="center" valign="middle" >&#177;0.02</td></tr><tr><td align="center" valign="middle" >S<sub>1</sub></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >44</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >2.92</td><td align="center" valign="middle" >(1.07 &#177; 0.20) &#215; 10<sup>−6</sup></td><td align="center" valign="middle" >4.175</td></tr><tr><td align="center" valign="middle" >S<sub>2</sub></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >43</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >2.94</td><td align="center" valign="middle" >(5.79 &#177; 0.20) &#215; 10<sup>−8</sup></td><td align="center" valign="middle" >4.238</td></tr><tr><td align="center" valign="middle" >S<sub>3</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >42</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >2.96</td><td align="center" valign="middle" >(2.90 &#177; 0.20) &#215; 10<sup>−7</sup></td><td align="center" valign="middle" >4.134</td></tr><tr><td align="center" valign="middle" >S<sub>4</sub></td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >41</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >2.98</td><td align="center" valign="middle" >(2.02 &#177; 0.20) &#215; 10<sup>−7</sup></td><td align="center" valign="middle" >4.136</td></tr></tbody></table></table-wrap><p>dissolution rate of the glasses immersed in distilled water at 900˚C for 24 days [<xref ref-type="bibr" rid="scirp.85683-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref11">11</xref>]. A progressive improvement of D<sub>R</sub> from 1.07 &#215; 10<sup>−</sup><sup>6</sup> to 5.80 &#215; 10<sup>−</sup><sup>8</sup> (g・cm<sup>2</sup>・min) was noted when the Cr<sub>2</sub>O<sub>3</sub> content varied from 1 to 2 mol%, respectively. However, we noted an increase in the dissolution rate (D<sub>R</sub>) from 5.80 &#215; 10<sup>−</sup><sup>8</sup> to 2 &#215; 10<sup>−</sup><sup>7</sup> (g・cm<sup>−</sup><sup>2</sup>・min<sup>−</sup><sup>1</sup>) when the Cr<sub>2</sub>O<sub>3</sub> content varies from 2 to 4 mol%, respectively.</p></sec><sec id="s3_2"><title>3.2. Density and Molar Volumes</title><p>Density measurements allowed us to follow the evolution of the molar volume depending on the composition of the system xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub>. The density measurements were completed at room temperature. As can be observed from the <xref ref-type="fig" rid="fig2">Figure 2</xref>, the variation in density versus Cr<sub>2</sub>O<sub>3</sub> content (mol%) indicates a maximum value of x = 2. The molar volume of oxygen (V<sub>OM</sub>) and the radius of anions of oxygen r<sub>cal</sub>(O<sup>2−</sup>) in the glass have been determined from Equations (1) and (2), respectively</p><p>V O M = M / ρ N A N 0 ∗ (1)</p><p>r cal ( O 2 − ) = V O M 3 2 (2)</p><p>With M = molar mass, ρ = density, N<sub>A</sub> = Avogadro number; N 0 ∗ = number of oxygen atoms in the molecular formula. The value of the molar volume and the oxygen radius were calculated from the approximate hypothesis of close packing of oxygen anions O<sup>2−</sup>, having r(O<sup>2−</sup>) recapitulated for each composition in <xref ref-type="table" rid="table2">Table 2</xref> [<xref ref-type="bibr" rid="scirp.85683-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref15">15</xref>]. A detailed analysis of the data in <xref ref-type="table" rid="table2">Table 2</xref> shows that the molar volume passes through a minimum when the Cr<sub>2</sub>O<sub>3</sub> content reaches 2 mol%. However, the covalent radius value of the oxygen atom (O<sup>2−</sup>), calculated by the molar volume using the Equation (2) for each composition, seems to decrease slightly.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Density and molar volume of system xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub></title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Samples</th><th align="center" valign="middle" >Molar formula Oxygen/Mol (N<sub>O</sub>)</th><th align="center" valign="middle" >Molar mass (g/mol)</th><th align="center" valign="middle" >ρ (g/cm<sup>3</sup>)</th><th align="center" valign="middle" >Molar volume (nm)<sup>3</sup> V O M = M / ρ N A N 0 ∗ <sup> </sup></th><th align="center" valign="middle" >Calculated oxygen radius (nm) r<sub>cal</sub>(O<sup>2−</sup>)</th></tr></thead><tr><td align="center" valign="middle" >S1</td><td align="center" valign="middle" >1Cr<sub>2</sub>O<sub>3</sub>・44PbO・55P<sub>2</sub>O<sub>5</sub> (322)</td><td align="center" valign="middle" >17,782.8</td><td align="center" valign="middle" >4.175</td><td align="center" valign="middle" >0.0219</td><td align="center" valign="middle" >0.140</td></tr><tr><td align="center" valign="middle" >S2</td><td align="center" valign="middle" >2Cr<sub>2</sub>O<sub>3</sub>・43PbO・55P<sub>2</sub>O<sub>5</sub> (324)</td><td align="center" valign="middle" >17,711.6</td><td align="center" valign="middle" >4.238</td><td align="center" valign="middle" >0.0214</td><td align="center" valign="middle" >0.138</td></tr><tr><td align="center" valign="middle" >S3</td><td align="center" valign="middle" >3Cr<sub>2</sub>O<sub>3</sub>・42PbO・55P<sub>2</sub>O<sub>5</sub> (326)</td><td align="center" valign="middle" >17,640.4</td><td align="center" valign="middle" >4.134</td><td align="center" valign="middle" >0.0217</td><td align="center" valign="middle" >0.139</td></tr><tr><td align="center" valign="middle" >S4</td><td align="center" valign="middle" >4Cr<sub>2</sub>O<sub>3</sub>・41PbO・55P<sub>2</sub>O<sub>5</sub> (328)</td><td align="center" valign="middle" >17,569.2</td><td align="center" valign="middle" >4.136</td><td align="center" valign="middle" >0.0215</td><td align="center" valign="middle" >0.139</td></tr></tbody></table></table-wrap></sec><sec id="s3_3"><title>3.3. Structural Approach by Infrared Spectroscopy</title><p>The infrared spectra for the xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> glasses series (with 1 ≤ x ≤ 4) are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. As can be seen from this figure, all the phosphate vibration bands of the treated sample are presented in the frequency range between 1600 and 399 cm<sup>−1</sup> [<xref ref-type="bibr" rid="scirp.85683-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref17">17</xref>]. The band of approximately 1244 - 1228 cm<sup>−1</sup> is attributed to the asymmetric vibration modes uas (PO<sub>2</sub>) or the two non-bridging oxygen atoms linked to a phosphorus atom in the phosphate tetrahedron Q<sup>2</sup> [<xref ref-type="bibr" rid="scirp.85683-ref17">17</xref>]. The vibrations of the bands around 1070 - 1047 cm<sup>−1</sup> are characteristic of the stretching vibrations υasy (PO<sub>3</sub>) and the terminal groups υs (PO<sub>2</sub>) [<xref ref-type="bibr" rid="scirp.85683-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref18">18</xref>]. The band about 912 - 894 cm<sup>−1</sup> is attributed to the uasy P-O-P stretching vibrations [<xref ref-type="bibr" rid="scirp.85683-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref20">20</xref>] , while the band at 779 - 771</p><p>cm<sup>−1</sup> is assigned to the stretching vibration υ<sub>sy</sub> P-O-P band of the transition oxygen atoms of phosphorus to a phosphate tetrahedron Q<sup>1</sup> [<xref ref-type="bibr" rid="scirp.85683-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref21">21</xref>]. Bands that appear between 500 and 466 cm<sup>−1</sup> are attributed to the P-O-P vibration modes of the skeleton [<xref ref-type="bibr" rid="scirp.85683-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref19">19</xref>]. All characteristics of the phosphate vibrations show that the phosphate glasses of compositions xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> (with 1 ≤ x ≤ 4) may have chains or rings of the metaphosphate groups, with some traces of pyrophosphate groups. In fact, when the Cr<sub>2</sub>O<sub>3</sub> content (mol%) is equal to x = 2, the vibration bonds υas (PO<sub>2</sub>) assigned to metaphosphates groups tend to be the dominant characteristic of the spectrum. As shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>, the band becomes more intense.</p></sec><sec id="s3_4"><title>3.4. X-Ray Diffraction</title><p>The XRD pattern shown in the <xref ref-type="fig" rid="fig4">Figure 4</xref> indicates that the local structure of chromium-lead phosphate glasses, evolved from ultraphosptate (O/P = 2.93) to nearby chains (cyclic metaphosphate O/P = 3, isolated orthophosphates O/P = 4) structures Cr(PO<sub>3</sub>)<sub>3</sub>, Cr<sub>2</sub>(PO<sub>3</sub>)<sub>6</sub>, Pb(PO<sub>3</sub>)<sub>2</sub>, Pb<sub>2</sub>(PO<sub>3</sub>)<sub>4</sub>, Pb<sub>3</sub>(PO<sub>4</sub>)<sub>2</sub>, Pb<sub>9</sub>(PO<sub>4</sub>)<sub>6</sub>, Pb<sub>3</sub>Cr(PO<sub>4</sub>)<sub>3</sub> and some trace of Pb<sub>2</sub>P<sub>2</sub>O<sub>7</sub>. When the sample S<sub>1</sub> was thermally treated at 560˚C, the amorphous phase partially disappeared and major Cr (PO<sub>3</sub>)<sub>3</sub> [JCDDS FileN˚: 01-077-0672], Pb(PO<sub>3</sub>)<sub>2</sub> [JCDDS. File N˚: 00-043-0335], Pb<sub>2</sub>(PO<sub>3</sub>)<sub>4</sub> [JCDDS File N˚: 01-086-21] Phases occurred in the sample, with minor Pb<sub>3</sub>(PO<sub>4</sub>)<sub>2</sub> [JCDDS File N˚01-070-1790] and Pb<sub>9</sub>(PO<sub>4</sub>)<sub>6</sub> [JCDDS file N˚: 00033-0768] Phases. When the Cr<sub>2</sub>O<sub>3</sub> content increased in the glass (S<sub>2</sub>), the heat treatment caused an increase in crystallization temperature at 580˚C, which</p><p>resulted in the disappearance of isolated orthophosphate phase and the formation of CrPO<sub>3</sub>)<sub>3</sub>, Pb<sub>2</sub>(PO<sub>3</sub>)<sub>4</sub> and Pb(PO<sub>3</sub>)<sub>2</sub>. However, the S<sub>4</sub> sample thermally treated at 560˚C, indicate the formation of metaphosphate and/or rings of metaphosphate phase Cr(PO<sub>3</sub>)<sub>3</sub>, Pb<sub>2</sub>(PO<sub>3</sub>)<sub>4</sub> with the appearance of isolated orthophosphate phase Pb<sub>9</sub>(PO<sub>4</sub>)<sub>6</sub> and Pb<sub>3</sub>Cr(PO<sub>4</sub>)<sub>3</sub> [JCDDS File N˚: 00-047-0830] at the expense of metaphosphate phases [<xref ref-type="bibr" rid="scirp.85683-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref23">23</xref>].</p></sec><sec id="s3_5"><title>3.5. SEM Micrograph</title><p>SEM images in <xref ref-type="fig" rid="fig5">Figure 5</xref> illustrate the morphology of the glasses considered in</p><p>this work. The glass form of S<sub>2</sub>, shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a), exhibits two phases, a vitreous phase and a crystalline phase. This last one indicates the formation of crystalline agglomerates particle having ring form that indicate, the crystallisation tendency is enhanced and major Cr (PO<sub>3</sub>)<sub>3</sub> and Pb<sub>2</sub>(PO<sub>3</sub>)<sub>4</sub> phases are crystallised in these glasses. The presence of the crystalline phase seems to explain the increase in chemical durability [<xref ref-type="bibr" rid="scirp.85683-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref16">16</xref>]. The SEM micrograph for the sample S<sub>4</sub> indicates a radical change in the structure. There is formation of crystalline phase agglomerates of various sizes, ranging from some microns. This probably explains the structural change towards more short isolated orthophosphate chains as the Cr<sub>2</sub>O<sub>3</sub> content increases in the glass network.</p></sec></sec><sec id="s4"><title>4. Discussion</title><p>The structure and the chemical durability of the glasses series xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> (with 1 ≤ x ≤ 4; mol%) have been investigated using various techniques such as density, X-Ray diffraction and IR. The measured properties indicate that the glasses series chromium-lead-phosphorus-oxygen network become stronger for x = 2. X-ray diffraction indicates that the samples S<sub>1</sub>, S<sub>2</sub> and S<sub>4</sub>, respectively annealed at 560˚C and 580˚C for 72 h, contain metaphosphates, orthophosphates and certain traces of pyrophosphate phases in all the glasses. When the Cr<sub>2</sub>O<sub>3</sub> content is equal to 2 mol%, X ray diffraction and IR spectra, both, confirmed the predominance of metaphosphate groups most probably cyclic. The bands at 1244 - 1228 cm<sup>−</sup><sup>1</sup>, attributed to the asymmetric vibration modes νas (PO<sub>2</sub>), become more intense. The predominance of cyclic metaphosphate chains as Cr (PO<sub>3</sub>)<sub>3</sub> and Pb<sub>2</sub>(PO<sub>3</sub>)<sub>4</sub> have led to maximum chemical durability. Analysis of the density values also showed a maximum density for x = 2 mol%. The covalent radius values of oxygen calculated from Equation (2) indicate that the minimum value rcal (O<sup>2</sup><sup>−</sup>) is observed for x = 2 mol% and therefore a relatively high reinforcement of the metal-oxygen-phosphorus (Cr-O-P) bond. Additionally, because of the big stability of the energy of field of ligand of d<sup>3</sup>systems in octahedral symmetry, the ions Cr<sup>3+</sup> occupy almost exclusively the sites having this symmetry type [<xref ref-type="bibr" rid="scirp.85683-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref24">24</xref>] , while the Pb is estimated to be in the tetrahedral site forming PbO<sub>4</sub> pyramids which are connected in phosphate tetrahedron by covalent links P-O-Pb [<xref ref-type="bibr" rid="scirp.85683-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref26">26</xref>]. Above 2 mol% Cr<sub>2</sub>O<sub>3</sub>, the glass structure changes relatively, it is found that the DRX spectra intensity of the ring metaphosphate phases decreases, whereas the appearance of the isolated orthophosphate phase becomes important when the Cr<sub>2</sub>O<sub>3</sub> content reaches 4 mol%. The substitution of PbO with chromium oxide by more than 2 mol% in the vitreous lattice appears to be an unfavorable factor for chemical durability. The origin of this phenomenon is explained almost probably by the approach of the boundary zone between the crystal and the glass by the continuous formation of groups of isolated phosphate PO 4 3 − [<xref ref-type="bibr" rid="scirp.85683-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref19">19</xref>]. The decrease of chemical durability observed, can be also explained by the existence of the critical concentrations between the cation ions beyond which each ion seeks, by competition, to have a site that is appropriate to it by moving away from the other. This behavior leads to an increase in the glass volume and a relaxation of the structure [<xref ref-type="bibr" rid="scirp.85683-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.85683-ref28">28</xref>] and consequently a decrease in density and chemical durability. On the other hand, the PbO oxide have &#224; low melting temperature and can participated with P<sub>2</sub>O<sub>5</sub> Oxyde, basis glass matrix, in the extend of the area glass. That explains probably the non evidence of the attributed band of orthophosphate isolated units in the IR spectra beside the X-ray diffraction spectra. Added, the elaboration method of the glasses (melting temperature, tempering speed, etc.) remains a significant factor in the deep understanding of the phenomenon [<xref ref-type="bibr" rid="scirp.85683-ref29">29</xref>].</p></sec><sec id="s5"><title>5. Conclusion</title><p>The structure and the chemical durability of chromium lead phosphate glasses of composition xCr<sub>2</sub>O<sub>3</sub>-(45-x)PbO-55P<sub>2</sub>O<sub>5</sub> avec (1 ≤ x ≤ 4; mol%) have been investigated using various techniques such IR, X-ray diffraction, density and SEM micrograph. The study of the dissolution rate carried out on the glasses, immersed in distilled water at 90˚C for 24 days, indicates a maximum chemical durability when the level of chromium oxide passes through 2 mol%. The analysis of the values of the density also showed a maximum density for x = 2 mol%. The covalent radius values of the oxygen indicate that the minimum values are observed for x = 2 mol%, and therefore, a relatively high reinforcement of the metal-oxygen-phosphorus (Cr-O-P) bonds. However, the increase in the Cr<sub>2</sub>O<sub>3</sub> content in the vitreous network to the detriment of PbO beyond 2 mol%, is an unfavourable factor for both chemical durability and density. The increase in the Cr + Pb/P ratio leads to an increase in the number of metal-O-P bonds which cause a high tendency for crystallisation and confirms that the dissolution rate (D<sub>R</sub>) of the analyzed compounds is comparable to the values of borosilicate glasses and 40 times less than BaBal glasses which are used as alternative materials for the immobilisation of nuclear waste substances.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors wish to thank National Center for Scientific and Technical Research [Division of Technical Support Unit for Scientific Research (TSUSR) Rabat, Morocco] for their assistance to the realization of this work.</p></sec><sec id="s7"><title>Cite this paper</title><p>Makhlouk, R., Beloued, N. and Aqdim, S. (2018) Study of Chromium-Lead-Phosphate Glasses by XRD, IR, Density and Chemical Durability. 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