<?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">JBM</journal-id><journal-title-group><journal-title>Journal of Biosciences and Medicines</journal-title></journal-title-group><issn pub-type="epub">2327-5081</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbm.2016.412019</article-id><article-id pub-id-type="publisher-id">JBM-72802</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Water Efflux in Red Blood Cells of Sickle Cell Patients under Spontaneous Deoxygenation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Manuel</surname><given-names>Arsenio Lores Guevara</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>Yulianela</surname><given-names>Mengana Torres</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>Juan</surname><given-names>Carlos García Naranjo</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>Andrés</surname><given-names>Ramírez Aguilera</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>María</surname><given-names>Altagracia Marichal Felue</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Teresa</surname><given-names>Simón Brada</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jan</surname><given-names>Philippé</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lidia</surname><given-names>Clara Suárez Beyrio</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Hospital General “Juan Bruno Zayas Alfonso”, Santiago de Cuba, Cuba</addr-line></aff><aff id="aff1"><addr-line>Centro de Biof&amp;amp;iacute;sica M&amp;amp;eacute;dica, Santiago de Cuba, Cuba</addr-line></aff><aff id="aff3"><addr-line>Department of Clinical Chemistry, Immunology and Microbiology, Ghent University, Ghent, Belgium</addr-line></aff><pub-date pub-type="epub"><day>01</day><month>12</month><year>2016</year></pub-date><volume>04</volume><issue>12</issue><fpage>152</fpage><lpage>161</lpage><history><date date-type="received"><day>October</day>	<month>14,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>December</month>	<year>13,</year>	</date><date date-type="accepted"><day>December</day>	<month>16,</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The water transport through Red Blood Cells (RBC) membrane has been previously studied in Sickle Cell Disease (SCD) using oxygenated RBC or under complete deoxygenation. In this work, the water efflux in RBC of sickle cell patients was studied under spontaneous deoxygenation conditions. With that purpose, a magnetic resonance method was used to evaluate the water exchange time (
  <em>τ</em>
  <em style="line-height:1.5;"><sub>e</sub></em>
  ) and the permeability through the erythrocyte membrane (
  <em style="line-height:1.5;">P</em>
  ) measuring the spin-spin relaxation time (
  <em style="line-height:1.5;">T<sub>2</sub></em>
  ) in doped and non-doped RBC. Carr-Purcell-Meiboon-Gill (CPMG) pulse sequence was used to measure <em>T<sub>2</sub></em><sub> </sub>in a magnetic resonance console coupled to one homogeneous magnet system (0.095 T). An increase of the water transport in RBC from sickle cell patients was observed and characterized with a <em style="font-family:宋体;font-size:14.399999618530273px;line-height:16.799999237060547px;white-space:normal;">τ</em><em><sub>e</sub></em> value of 15.2 &#177; 0.8 ms. The abnormal activation of the 
  <em style="line-height:1.5;">P</em>
  <sub><em>sickl</em><em>e</em></sub>
  , Gardos, and potassium chloride cotransporter channels starting from deoxygenation, as well as, the possible appearance of 
  new pores due to the increase of the hemoglobin-membrane interaction, are suggested to explain this abnormal transport phenotype. The change of the water volume to surface ratio (V/S) in the sickle cells is also suggested to be considered in <em>P</em> calculation under deoxygenation. The results obtained in this work increase the fundamental knowledge about molecular mechanism involved in SCD and could be useful in the development of new methods for diagnostic and treatment evaluation.
 
</p></abstract><kwd-group><kwd>Red Blood Cells</kwd><kwd> Water Permeability</kwd><kwd> Nuclear Magnetic Relaxation</kwd><kwd> Sickle Cell Disease</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>After one century, SCD is still an important worldwide health problem without a final solution [<xref ref-type="bibr" rid="scirp.72802-ref1">1</xref>] . Its complexity, genetic origin [<xref ref-type="bibr" rid="scirp.72802-ref2">2</xref>] and the different molecular processes involved in its pathophysiology [<xref ref-type="bibr" rid="scirp.72802-ref3">3</xref>] have contributed to this situation. The presence of an abnormal hemoglobin (HbS) inside the RBC, causing a polymerization process under deoxygenation, is recognized as the molecular process contributing most to the pathogenesis of SCD [<xref ref-type="bibr" rid="scirp.72802-ref4">4</xref>] , and for this reason many efforts have been made in relation to its study [<xref ref-type="bibr" rid="scirp.72802-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref9">9</xref>] . Nevertheless, the deoxygenation also causes cell damage, dehydration and shrinking [<xref ref-type="bibr" rid="scirp.72802-ref10">10</xref>] .</p><p>Different membrane abnormalities have been documented in RBC from sickle cell patients [<xref ref-type="bibr" rid="scirp.72802-ref11">11</xref>] : loss of lipid bilayer asymmetry, altered rate of phosphatidylcholine flip- flop, abnormal spectrin-actin skeleton, as well as, defective association between ankyrin and spectrin in situ on sickle cell inside out vesicles. These cause functional abnormalities as an abnormal transport phenotype [<xref ref-type="bibr" rid="scirp.72802-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref12">12</xref>] : increased influx of calcium, reduced efflux permeability to non-electrolytes as glycerol and ethylene glycol and net loss of monovalent cations. Specially, the net loss of monovalent cations has been directly related with direct cellular dehydration because of the cellular response to maintain the osmotic equilibrium [<xref ref-type="bibr" rid="scirp.72802-ref12">12</xref>] .</p><p>The water transport in RBC has been widely studied before [<xref ref-type="bibr" rid="scirp.72802-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.72802-ref18">18</xref>] . Especially, the water efflux and influx through the membrane of RBC from sickle cell patients has been studied in oxygenated erythrocytes [<xref ref-type="bibr" rid="scirp.72802-ref19">19</xref>] and in cells under total deoxygenation [<xref ref-type="bibr" rid="scirp.72802-ref20">20</xref>] , however, no studies under spontaneous deoxygenation have been performed. On the other hand, after deoxygenation, no values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x2.png" xlink:type="simple"/></inline-formula> and no proper values of P have been reported.</p><p>The deoxygenation pattern (deoxygenation % and speed) defines the HbS polymerization, as well as, the RBC shape change [<xref ref-type="bibr" rid="scirp.72802-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref4">4</xref>] . In this work, we study <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x3.png" xlink:type="simple"/></inline-formula> after HbS polymerization under spontaneous deoxygenation conditions. Different molecular mechanisms are considered to explain the observed behaviour, and the necessity of an adequate evaluation of the V/S to calculate P in sickle cells, after deoxygenation, is discussed.</p></sec><sec id="s2"><title>2. Materials and Methods</title><p>After the approval of the hospital ethical committee, and the obtaining of the informed consent, samples of RBCA (containing adult normal hemoglobin, HbA) and RBCS (containing HbS) were obtained [<xref ref-type="bibr" rid="scirp.72802-ref5">5</xref>] . Whole blood samples were obtained by venipuncture and immediately heparinized. After removing the plasma and leukocytes, RBC were washed three times with phosphate buffered saline (PBS, pH 7.4, Sigma Chemicals Co.) [<xref ref-type="bibr" rid="scirp.72802-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref9">9</xref>] . Supernatants were removed by centrifugation (500 g, 10 min) and decanting. The obtained washed RBC were resuspended (Hematocrit 45%, PBS (pH 7.4), 0.5% of BSA) and one portion was centrifuged (1000 g, 30 min, 25˚C) eliminating the supernatant to obtain packed RBC. 500 μl of packed RBC were taken and T<sub>2</sub> for this sample was measured (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x4.png" xlink:type="simple"/></inline-formula>).</p><p>300 μl of resuspended RBC were mixed with 600 μl of the manganese chloride stock solution (MnCl<sub>2</sub>(aq)) to obtain a final concentration of 2.5 mM. 500 μl of doped RBC were taken and T<sub>2</sub> for this sample was measured (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x5.png" xlink:type="simple"/></inline-formula>).</p><p>Starting from the measured values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x6.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x7.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x8.png" xlink:type="simple"/></inline-formula>and P were calculated as follows [<xref ref-type="bibr" rid="scirp.72802-ref13">13</xref>] :</p><disp-formula id="scirp.72802-formula147"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2150299x9.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72802-formula148"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2150299x10.png"  xlink:type="simple"/></disp-formula><p>where V (0.63 &#215; 10<sup>−10</sup> cm<sup>3</sup>) and S (1.42 &#215; 10<sup>−6</sup> cm<sup>2</sup>) are the water volume inside the RBC and the surface of the RBC, respectively. V/S = 4.4 &#215; 10<sup>−5</sup> cm.</p><p>The magnetic resonance measurements were performed in a magnetic resonance console (MARAN DRX, Oxford Instruments, UK). T<sub>2</sub> was measured using CPMG pulse sequence with a resonance frequency of 4.0353 MHz (homogeneous permanent magnet, B<sub>0</sub> = 0.095 T), 10 and 20 &#181;s for 90˚ and 180˚ pulses respectively, 128 scans, 50% for the RF power amplifier and the receiver gains, 3 s of relaxation delay and echo time of 0.2 ms (doped RBC) and 2 ms (packed RBC).</p><p>A student’s test (t-test) was performed to compare main values with α = 0.05.</p></sec><sec id="s3"><title>3. Results and Discussion.</title><p>The values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x11.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x12.png" xlink:type="simple"/></inline-formula>and P in oxygenated RBCA were measured for two temperature values (25˚C and 29˚C) (see <xref ref-type="table" rid="table1">Table 1</xref>).</p><p>The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x13.png" xlink:type="simple"/></inline-formula> and P values for RBCA water efflux, shown in <xref ref-type="table" rid="table1">Table 1</xref>, are coherent with previous reports in the literature (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x14.png" xlink:type="simple"/></inline-formula>= (9.8 - 14.0) ms; P = (3.3 - 4.7) &#215; 10<sup>−3</sup> cms<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.72802-ref16">16</xref>] . The independence with the temperature is due to the activation energy characterizing</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x15.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x16.png" xlink:type="simple"/></inline-formula>and P values corresponding to oxygenated RBCA for two temperature values (25˚C &#177; 1˚C and 29˚C &#177; 1˚C)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Individuals</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x17.png" xlink:type="simple"/></inline-formula>(ms)</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x18.png" xlink:type="simple"/></inline-formula>(ms)</th><th align="center" valign="middle" >P (10<sup>−3</sup> cms<sup>−1</sup>)</th><th align="center" valign="middle" >T (˚C)</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >9.93 &#177; 0.53</td><td align="center" valign="middle" >12.00 &#177; 0.23</td><td align="center" valign="middle" >3.70 &#177; 0.18</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >11.67 &#177; 0.76</td><td align="center" valign="middle" >13.00 &#177; 0.46</td><td align="center" valign="middle" >3.30 &#177; 0.16</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >11.89 &#177; 0.94</td><td align="center" valign="middle" >13.7 &#177; 1.2</td><td align="center" valign="middle" >3.25 &#177; 0.29</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >10.60 &#177; 0.50</td><td align="center" valign="middle" >11.30 &#177; 0.67</td><td align="center" valign="middle" >3.92 &#177; 0.20</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >11.83 &#177; 0.63</td><td align="center" valign="middle" >12.80 &#177; 0.84</td><td align="center" valign="middle" >3.40 &#177; 0.22</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >11.02 &#177; 0.80</td><td align="center" valign="middle" >12.19 &#177; 0.75</td><td align="center" valign="middle" >3.60 &#177; 0.18</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >14.75 &#177; 0.69</td><td align="center" valign="middle" >16.30 &#177; 0.84</td><td align="center" valign="middle" >2.68 &#177; 0.13</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >12.87 &#177; 0.50</td><td align="center" valign="middle" >13.93 &#177; 0.58</td><td align="center" valign="middle" >3.16 &#177; 0.13</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >13.71 &#177; 0.96</td><td align="center" valign="middle" >15.0 &#177; 1.1</td><td align="center" valign="middle" >2.94 &#177; 0.21</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >11.28 &#177; 0.40</td><td align="center" valign="middle" >11.99 &#177; 0.42</td><td align="center" valign="middle" >3.67 &#177; 0.13</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >12.16 &#177; 0.55</td><td align="center" valign="middle" >13.32 &#177; 0.66</td><td align="center" valign="middle" >3.31 &#177; 0.16</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >14.98 &#177; 0.43</td><td align="center" valign="middle" >16.47 &#177; 0.53</td><td align="center" valign="middle" >2.67 &#177; 0.01</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >14.14 &#177; 0.60</td><td align="center" valign="middle" >15.21 &#177; 0.53</td><td align="center" valign="middle" >2.89 &#177; 0.10</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >Main values</td><td align="center" valign="middle" >12.37 &#177; 1.60</td><td align="center" valign="middle" >13.6 &#177; 1.6</td><td align="center" valign="middle" >3.27 &#177; 0.39</td><td align="center" valign="middle" >-</td></tr></tbody></table></table-wrap><p>the process (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x19.png" xlink:type="simple"/></inline-formula>= 26 kJ∙mol<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.72802-ref18">18</xref>] and its influence in Equation (3).</p><disp-formula id="scirp.72802-formula149"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2150299x20.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x21.png" xlink:type="simple"/></inline-formula>, T and K are the initial water exchange time, the absolute temperature and the Boltzman constant, respectively.</p><p>The P values in oxygenated and spontaneously deoxygenated RBCA (24 h, 36˚C, 50% of deoxygenation) are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Because of the deoxygenation inhibits the KCC (K<sup>+</sup> and Cl<sup>−</sup> cotransporter) channel activation in RBCA [<xref ref-type="bibr" rid="scirp.72802-ref12">12</xref>] , causing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x22.png" xlink:type="simple"/></inline-formula> increases, these cells have a reduced P values after spontaneous deoxygenation. It was not taken into account and/or discussed in previous results [<xref ref-type="bibr" rid="scirp.72802-ref20">20</xref>] .</p><p>The values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x23.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x24.png" xlink:type="simple"/></inline-formula>and P in oxygenated RBCS are summarized in <xref ref-type="table" rid="table2">Table 2</xref>. P</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Efflux water permeability in oxygenated (100% of oxygenation) and spontaneously deoxygenated (50% of deoxygenation) RBC from healthy individuals. Red blood cells have intracellular concentrations and P was determined starting from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x26.png" xlink:type="simple"/></inline-formula> and V/S ratio (Equation (2)). <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x27.png" xlink:type="simple"/></inline-formula>was measured using the T<sub>2</sub> values of doped (2.5 mM MnCl<sub>2(aq)</sub>) and not doped RBC samples (Equation (1)). T<sub>2</sub> was measured using CPMG</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2150299x25.png"/></fig><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x28.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x29.png" xlink:type="simple"/></inline-formula>and P values in oxygenated RBCS</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sickle Cell patient</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x30.png" xlink:type="simple"/></inline-formula>(ms)</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x31.png" xlink:type="simple"/></inline-formula>(ms)</th><th align="center" valign="middle" >P (10<sup>−3</sup> cms<sup>−1</sup>)</th><th align="center" valign="middle" >T (˚C)</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >16.01 &#177; 0.80</td><td align="center" valign="middle" >18.7 &#177; 1.2</td><td align="center" valign="middle" >2.35 &#177; 0.16</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >17.34 &#177; 0.30</td><td align="center" valign="middle" >20.3 &#177; 1.1</td><td align="center" valign="middle" >2.16 &#177; 0.15</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >21.71 &#177; 0.70</td><td align="center" valign="middle" >26 &#177; 1</td><td align="center" valign="middle" >1.69 &#177; 0.12</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >17.16 &#177; 0.96</td><td align="center" valign="middle" >20.3 &#177; 1.3</td><td align="center" valign="middle" >2.17 &#177; 0.14</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >16.27 &#177; 0.96</td><td align="center" valign="middle" >19.5 &#177; 1.3</td><td align="center" valign="middle" >2.26 &#177; 0.16</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >18.84 &#177; 0.88</td><td align="center" valign="middle" >23.2 &#177; 1.3</td><td align="center" valign="middle" >1.89 &#177; 0.11</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >15.4 &#177; 1.1</td><td align="center" valign="middle" >18.2 &#177; 1.5</td><td align="center" valign="middle" >2.43 &#177; 0.21</td><td align="center" valign="middle" >29 &#177; 1</td></tr><tr><td align="center" valign="middle" >Main values</td><td align="center" valign="middle" >17.5 &#177; 2.1</td><td align="center" valign="middle" >20.8 &#177; 2.7</td><td align="center" valign="middle" >2.13 &#177; 0.26</td><td align="center" valign="middle" >29 &#177; 1</td></tr></tbody></table></table-wrap><p>decreases ((2.13 &#177; 0.26) &#215; 10<sup>−3</sup> cms<sup>−1</sup>) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x32.png" xlink:type="simple"/></inline-formula> increases (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x33.png" xlink:type="simple"/></inline-formula>= 20.89 &#177; 2.77 ms) if compared with the values obtained for healthy individuals (P = (3.27 &#177; 0.39) &#215; 10<sup>−3</sup> cms<sup>−1</sup> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x34.png" xlink:type="simple"/></inline-formula> = 13.63 &#177; 1.67 ms) (see <xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>The increase in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x35.png" xlink:type="simple"/></inline-formula> and P reduction in oxygenated RBCS, compared with healthy individuals, match with previous reports (P = (1.61 &#177; 0.39) &#215; 10<sup>−3</sup> cms<sup>−1</sup> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x36.png" xlink:type="simple"/></inline-formula> = 29.2 &#177; 7.3 ms) [<xref ref-type="bibr" rid="scirp.72802-ref19">19</xref>] , and are closely related to:</p><p>・ The lipid peroxidation in the lipid bilayer.</p><p>・ The hemoglobin interaction with membrane Band 3 protein.</p><p>・ The oxidation of Band 3 sulfhydryl groups in the 15 kDa transmembrane fragment.</p><p>Because of simple diffusion only supports the 10% of the water transport through RBC membrane, the lipid peroxidation in the lipid bilayer cannot explain the observed P reduction in 34%. The sulfhydryl group oxidation is caused by the spontaneous generation of oxygen radicals and has been considered as the main contribution to P reduction [<xref ref-type="bibr" rid="scirp.72802-ref19">19</xref>] . The hemoglobin-membrane interaction is established with the Band 3 protein, at the same position as the main pore (4.5 &#197;) for water transport in RBC membrane; and, therefore, could cause an occlusion of this channel [<xref ref-type="bibr" rid="scirp.72802-ref20">20</xref>] . It has been demonstrated that this interaction is stronger in oxygenated sickle cell patient RBC than in cells from healthy controls [<xref ref-type="bibr" rid="scirp.72802-ref21">21</xref>] . As a consequence, the occlusion could contribute to the observed P reduction in oxygenated RBCS.</p><p>The values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x37.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x38.png" xlink:type="simple"/></inline-formula> in RBCS, under spontaneous deoxygenation, are summarized in <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>The spontaneous deoxygenation decreases <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x39.png" xlink:type="simple"/></inline-formula> values (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x40.png" xlink:type="simple"/></inline-formula>=15.2 &#177; 1.0 ms) of the RBCS compared with the results obtained before deoxygenation (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x41.png" xlink:type="simple"/></inline-formula>= 20.8 &#177; 2.7 ms)</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Efflux water permeability in oxygenated (100% of oxygenation) RBC from healthy individuals and sickle cell patients. Red blood cells have intracellular concentrations and P was determined starting from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x43.png" xlink:type="simple"/></inline-formula><sub> </sub>and V/S ratio (Equation (2)). <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x44.png" xlink:type="simple"/></inline-formula>was measured using the T<sub>2</sub> values of doped (2.5 mM MnCl<sub>2(aq)</sub>) and not doped RBC samples (Equation (1)). T<sub>2</sub> was measured using CPMG</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2150299x42.png"/></fig><p>(see <xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>Even though it is possible to find reports of the water transport for deoxygenated RBCS (P = (1.58 &#177; 0.06) &#215; 10<sup>−2</sup> cms<sup>−1</sup>) [<xref ref-type="bibr" rid="scirp.72802-ref20">20</xref>] , it does not affect the novelty of our results because in these experiments:</p><p>・ The reported experimental values of efflux water permeability were 10 times higher than the established values for human RBC [<xref ref-type="bibr" rid="scirp.72802-ref16">16</xref>] .</p><p>・ Induced complete deoxygenation was employed to provoke the HbS polymerization (0.5 mM, sodium dithionite).</p><p>・ The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x45.png" xlink:type="simple"/></inline-formula> values are not reported.</p><p>The explanation of decreased<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x46.png" xlink:type="simple"/></inline-formula>, as a consequence of the spontaneous deoxygenation, is related with the hemoglobin-membrane interaction and the activation of the P<sub>sickle</sub>,</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x47.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x48.png" xlink:type="simple"/></inline-formula> in RBCS under spontaneous deoxygenation</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Sickle Cell patient</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x49.png" xlink:type="simple"/></inline-formula>(ms)</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x50.png" xlink:type="simple"/></inline-formula>(ms)</th><th align="center" valign="middle" >T (˚C)</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >11.69 &#177; 0.11</td><td align="center" valign="middle" >14.63 &#177; 0.17</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >11.32 &#177; 0.24</td><td align="center" valign="middle" >13.47 &#177; 0.34</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >13.04 &#177; 0.25</td><td align="center" valign="middle" >16.04 &#177; 0.39</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >13.26 &#177; 0.49</td><td align="center" valign="middle" >16.58 &#177; 0.77</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >12.17 &#177; 0.50</td><td align="center" valign="middle" >14.92 &#177; 0.76</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >12.57 &#177; 0.16</td><td align="center" valign="middle" >15.51 &#177; 0.24</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >11.83 &#177; 0.45</td><td align="center" valign="middle" >14.39 &#177; 0.67</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >13.3 &#177; 2.1</td><td align="center" valign="middle" >16 &#177; 3</td><td align="center" valign="middle" >25 &#177; 1</td></tr><tr><td align="center" valign="middle" >Main values</td><td align="center" valign="middle" >12.41 &#177; 0.77</td><td align="center" valign="middle" >15.2 &#177; 1.0</td><td align="center" valign="middle" >25 &#177; 1</td></tr></tbody></table></table-wrap><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Water exchange time in oxygenated (100% of oxygenation) and spontaneously deoxygenated (50% of deoxygenation) RBC from sickle cell patients. Red blood cells have intracellular concentrations and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x52.png" xlink:type="simple"/></inline-formula> was measured using the T<sub>2</sub> values of doped (2.5 mM MnCl<sub>2(aq)</sub>) and not doped RBC samples (Equation (1)). T<sub>2</sub> was measured using CPMG</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-2150299x51.png"/></fig><p>Gardos, and KCC channels. The hemoglobin-membrane interaction could cause the appearance of pores starting from high order structure of the Band 3 protein [<xref ref-type="bibr" rid="scirp.72802-ref20">20</xref>] . We have previously demonstrated the increase of hemoglobin-membrane interaction with HbS polymerization under spontaneous deoxygenation conditions [<xref ref-type="bibr" rid="scirp.72802-ref22">22</xref>] . Now, we are strongly suggesting this increase could provoke the opening of new pores for the water efflux, which could explain the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x53.png" xlink:type="simple"/></inline-formula> decrease after the agglutination process.</p><p>In RBCS, decreased oxygen partial pressure (PO<sub>2</sub>) provokes the P<sub>sickle</sub> activation, causing a K<sup>+</sup> efflux, as well as, Na<sup>+</sup> and Ca<sup>2+</sup> influx. When the Ca<sup>2+</sup> concentration reaches a threshold, the Gardos Channels (about 150 per cells) are activated causing a fast K<sup>+</sup> and Cl<sup>−</sup> efflux [<xref ref-type="bibr" rid="scirp.72802-ref12">12</xref>] . As a difference with RBCA, in the RBCS the deoxygenation inhibits the KCC channel until PO<sub>2</sub> = 40 mmHg, provoking it increases again when PO<sub>2</sub> &lt; 40 mmHg [<xref ref-type="bibr" rid="scirp.72802-ref12">12</xref>] . After 24 h of spontaneous deoxygenation (PO<sub>2</sub> &lt; 40 mmHg [<xref ref-type="bibr" rid="scirp.72802-ref23">23</xref>] , 50% of deoxygenation) KCC is reactivated in our experiments contributing to the net ions loss. The efflux of ions is coupled with a water efflux to maintain the osmotic equilibrium. The cellular dehydration increases the HbS concentration, which facilitates the HbS polymerization, the increase in the hemoglobin-membrane interaction, and the RBC shrinking.</p><p>On the other hand, it is important to consider that we are determining P (Equation (2)) for RBCA and RBCS using the same V/S ratio, as usual in the literature [<xref ref-type="bibr" rid="scirp.72802-ref19">19</xref>] . We consider this is an adequate procedure in oxygenated RBCS taking into account that: the Mean Corpuscular Volume (MCV) and Surface Area (S) do not have a statistically significant variation in these cells [<xref ref-type="bibr" rid="scirp.72802-ref24">24</xref>] - [<xref ref-type="bibr" rid="scirp.72802-ref29">29</xref>] . For deoxygenated RBCS is reported a MCV decreasing [<xref ref-type="bibr" rid="scirp.72802-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref34">34</xref>] and S remains constant [<xref ref-type="bibr" rid="scirp.72802-ref31">31</xref>] , which could change the V/S ratio and affect the P values. For this reason, in this work we are only reporting the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x54.png" xlink:type="simple"/></inline-formula> values after deoxygenation for RBCS. To evaluate P, it is necessary to determine the V/S behavior in RBCS after deoxygenation. It could be done by performing a magnetic resonance experiment which includes a magnetic field gradient, studying the water self- diffusion coefficient behavior for short interpulse delay time in CPMG or stimulated echo pulse sequences [<xref ref-type="bibr" rid="scirp.72802-ref35">35</xref>] . Another way to measure P is starting from the effective water self-diffusion coefficient measured in the RBC, as well as, in the extracellular and intracellular medium [<xref ref-type="bibr" rid="scirp.72802-ref35">35</xref>] . Starting from this last determination and measuring, in the same sample, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x55.png" xlink:type="simple"/></inline-formula> values using the method described in this work, it is also possible to determine V/S using Equation (2). It will be the subject of forthcoming works.</p><p>Not separated variations in water transport have been found in density-separated cell fractions of RBCS [<xref ref-type="bibr" rid="scirp.72802-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.72802-ref20">20</xref>] , for that reason our study has not considered it.</p></sec><sec id="s4"><title>4. Conclusion</title><p>The HbS polymerization process, under spontaneous deoxygenation conditions, leads to an increase in the water transport through the RBC membrane from sickle cell patients, characterized by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2150299x56.png" xlink:type="simple"/></inline-formula> values of 15.2 &#177; 0.8 ms. The abnormal activation of the P<sub>sickle</sub>, Gardos, and KCC channels starting from deoxygenation, as well as, the possible appearance of new pores due to the increased hemoglobin-membrane interaction could explain this abnormal transport phenotype. The results obtained in this work increase the fundamental knowledge about molecular mechanism involved in SCD and could be useful in the development of new methods for diagnostic and treatment evaluation.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work has been supported by the Belgian Development Cooperation through VLIR- UOS (Flemish Interuniversity Council-University Cooperation for Development) in the context of the Institutional University Cooperation program with Universidad de Oriente. The authors also want to thank the MRI RESEARCH CENTRE of the University of New Brunswick, Fredericton, Canada, for all the support received to finalize this work.</p></sec><sec id="s6"><title>Cite this paper</title><p>Guevara, M.A.L., Torres, Y.M., Naranjo, J.C.G., Aguilera, A.R., Beyrio, L.C.S., Felue, M.A.M., Brada, T.S. and Philipp&#233;, J. (2016) Water Efflux in Red Blood Cells of Sickle Cell Patients under Spontaneous Deoxygenation. 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