<?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">JWARP</journal-id><journal-title-group><journal-title>Journal of Water Resource and Protection</journal-title></journal-title-group><issn pub-type="epub">1945-3094</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jwarp.2016.810075</article-id><article-id pub-id-type="publisher-id">JWARP-70878</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Separation of Benzene, Toluene, Ethylbenzene and P-Xylene from Aqueous Solutions by Carbon Nanotubes/Polyvinylidene Fluoride Nanocomposite Membrane
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fengsheng</surname><given-names>Su</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Chungsying</surname><given-names>Lu</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>Jie-Huei</surname><given-names>Tai</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Environmental Engineering, National Chung Hsing University, Taiwan</addr-line></aff><aff id="aff1"><addr-line>Department of Safety, Health and Engineering, Ming Chi University of Technology, Taiwan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>sfs0331@gmail.com(FS)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>08</month><year>2016</year></pub-date><volume>08</volume><issue>10</issue><fpage>913</fpage><lpage>928</lpage><history><date date-type="received"><day>August</day>	<month>15,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>September</month>	<year>23,</year>	</date><date date-type="accepted"><day>September</day>	<month>27,</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>
 
 
  Carbon nanotubes/polyvinylidene fluoride (PVDF) nanocomposite membranes (abbreviated as CPMs) were fabricated to study their physicochemical property and separation efficiency of organic pollutants such as benzene, toluene, ethylbenzene and methylbenzene (abbreviated as BTEX) from aqueous solutions. The rejection coeffi-cients (
  R) of BTEX depend on the CNT content of CPM, pore size of membrane, molecule size of BTEX, permeation pressure (
  P), feed concentration (
  C
  <sub>f</sub>) and temperature. The CNT contents were 5%, 10% and 15% in CPM have been conducted. The 10% CNT content of CPM (10-CPM) has not only higher water flux but also the relatively higher 
  R as comparing of 5% and 15% CNT of CPM. The 
  R decreased with increasing 
  P, 
  C<sub>f</sub> and temperature but has no significant influence on ionic strength (
  μ). The R of BTEX were found in the order as B &lt; T &lt; E 
  ≈
   X which revealed the major mechanism of BTEX separation with CPM was related to molecule size of BTEX (B &lt; T &lt; E 
  ≈
   X). It exhibits that the size exclusion plays the important role in BTEX separation. According to the result of separation of BTEX by 10-CPM, the R of BTEX not only have above 80% with relative lower pressure but also have higher water flux as compared of other nano-filtration. This suggests that the 10-CPMs possess good potential for BTEX removal in wastewater treatment.
 
</p></abstract><kwd-group><kwd>CNT Membrane</kwd><kwd> BTEX</kwd><kwd> Nanofiltration</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The BTEX, volatile organic compounds, which are benzene (B), toluene (T), ethylben- zene (E) and p-xylene (X) are commonly used as solvents in industrial field. The waste- water containing of BTEX is usually discharged into environment from manufacturing, transportation and purposeful disposal sources. The BTEX are toxic and carcinogenic substances, while the presence of excessive amounts of BTEX in aqueous system may have an adverse impact on water quality or them volatized into ambient atmosphere thus endanger public health. It is clear that sustainable, cost effective and efficient wastewater treatment for BTEX is needed. The development of a cost-effective waste- water treatment process for BTEX removal before releasing into the environment is needed in order to meet the growing demand for cleaner water. Membrane filtration process has been employed for this purpose [<xref ref-type="bibr" rid="scirp.70878-ref1">1</xref>] .</p><p>Carbon nanotubes (CNT) are unique, one-dimensional macromolecules that possess outstanding gas and water permeability, nanofluidics and molecular transport at nano- scales [<xref ref-type="bibr" rid="scirp.70878-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.70878-ref5">5</xref>] . Literatures have demonstrated that the CNT membrane has extremely high transport rates of water and gas due to its unique nano-fluidic system [<xref ref-type="bibr" rid="scirp.70878-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.70878-ref14">14</xref>] . These properties lead membrane filtration to high flux and low operation pressure and thus directly benefit the fields of water and wastewater treatment, desalination, gas pollution control, gas/chemical separations and drug delivery [<xref ref-type="bibr" rid="scirp.70878-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.70878-ref19">19</xref>] . However, to the knowledge of the authors, filtration of BTEX from aqueous solutions by CNT/ polymer nanocomposite membrane is still limited in the literature.</p><p>This article fabricated the CNT/polyvinylidene fluoride (PVDF) nanocomposite membranes (CPMs) to study their physicochemical properties and separation perfor- mance of BTEX from aqueous solutions.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Preparation of Carbon Nanotubes Membranes</title><p>Commercially available multiwalled CNTs (C<sub>Tube</sub>-100, CNT Co. Ltd., Korea) with outer diameter of 10 - 40 nm and length of 1 - 25 mm were used to make CNT nanocomposite membranes which has 3.16 nm as average pore diameter. The CPMs were prepared by dissolving CNTs into 16 mL of N, N-dimethylformide (DMF, 99.8% purity, Sigma Aldrich Corp., Mo, USA) at 25˚C and sonicating for 1 h. The PVDF (Sigma-Aldrich Corp, Mo, USA) was added into the mixture in a CNT/PVDF ratio of 5 - 15 wt% and then was stirred at 400 rpm and heated to 180˚C for 24 h to make sure complete dissolution of the polymer. The CNT/PVDF solution was uniformly casted on a glass plate by means of a hand-casting knife with a knife gap set at 300 μm and then subsequently immersed in a deionized water bath to preserve the membrane (wet phase inversion method). The CPMs were trimmed to a circle shape with a diameter of 7 cm. The PVDF membrane (PM) was also prepared using the same procedure with the exception of CNTs addition.</p></sec><sec id="s2_2"><title>2.2. Pollutants</title><p>The employed B, T, E and X were analytical grade with &gt;99% purity and purchased from Merck (Darmstadt, Germany for B and T; Hohenbrunn, Germany for E and X). These chemical agents were diluted using deionized H<sub>2</sub>O to the desired concentrations in enclosed bottles. The molecule diameters of B, T, E and X are respectively 0.58, 0.6, 0.63 and 0.63 nm [<xref ref-type="bibr" rid="scirp.70878-ref20">20</xref>] .</p></sec><sec id="s2_3"><title>2.3. Filtration Experiments</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the membrane filtration experiment setup. It was conducted by using a crossflow filtration system, which equipped with a pressure vessel containing the mem- brane module, pressurization tank, a temperature control box and a digital analytical balance. The BTEX containing solution was pressured by compressed air from the tank to the membrane cell within a stainless steel disk, which has inner diameter of 5 cm and an active area of 19.63 cm<sup>2</sup>. The permeation was analyzed for the BTEX concentration and weight to measure the permeation volume. The rejection coefficient of the BTEX concentration, R, was calculated as:</p><disp-formula id="scirp.70878-formula1474"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9402980x2.png"  xlink:type="simple"/></disp-formula><p>where C<sub>f</sub> and C<sub>p</sub> are the BTEX concentrations in the feed and permeate, respectively. The membrane is completely permeable when R reaches zero while the membrane is completely impermeable when R achieves unity.</p></sec><sec id="s2_4"><title>2.4. Analytic Methods</title><p>The concentrations of BTEX were determined by a gas chromatograph and flame ionization detection (GC-FID, Model Shimadzu 2010, Shimadzu Instruments, CA, USA). The BTEX samples were collected to 5 ml from filter and then injected to purge and trap concentrator (Stratum PTC, Teledyne Tekmar, OH, USA) under trap adsorption temperature at 25˚C and trap desorption temperature at 250˚C with N<sub>2</sub> as purge gas, then the gaseous BTEX were injected to GC-FID for analysis at detector temperature of 200˚C.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Membrane filtration setup</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x4.png"/></fig><p>The CNT content of CPMs was determined by a thermo gravimetric analyzer (TGA I 1000, Instrument Specialists Incorporated, Twin Lakes, WI, USA) at a heating rate of 2˚C/min from 25˚C - 800˚C.</p><p>The morphologies of the PM and CPMs were investigated by a field emission scanning electron microscope (FE-SEM, Ultra Plus, Carl Zeiss SMT AG, Germany). Repres- entative samples of the membranes were cut into 1 - 2 mm<sup>2</sup>, attached with carbon tape to aluminum stabs, and shadowed with platinum prior to the SEM measurements.</p><p>Membrane surface topography was determined by atomic force microscope (AFM, SPA 400, Seiko Instruments Inc., Japan) image and analysis. Topographic imaging was performed in dynamic force mode with noncontact silicon cantilevers (NSC15/AIBS, spring const. = 20 N/m, Mikromasch, Estonia). The surface roughness of membrane (abbreviated as R<sub>RMS</sub>) that was typically used to quantify variations in surface elevation was determined directly from the height data by root-mean-square roughness calculation.</p><p>The pore properties of the membrane were determined by N<sub>2</sub> adsorption/desorption at 77 K via Micromeritics ASAP 2020 volumetric sorption analyzer (Norcross, GA, USA). The N<sub>2</sub> adsorption/desorption isotherms were measured at a relative pressure range of 0.0001 - 0.99 and then employed to determine specific pore volume and average pore diameter via the micropore (MP) method for pore sizes below 1.7 nm and the Barrett-Johner-Halenda (BJH) method for pore sizes 1.7 - 300 nm.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Characterization of the Membrane</title><sec id="s3_1_1"><title>3.1.1. TGA</title><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the TG curves of PM and 5% - 15% of CNT content CPMs. There are two temperatures for the start of rapid weight loss, named as T<sub>1</sub> and T<sub>2</sub>, which were</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> TG curves of PM and various CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x5.png"/></fig><p>ascribed to initial temperatures for thermal decomposition of PVDF and CNTs/ash,<sub> </sub>respectively [<xref ref-type="bibr" rid="scirp.70878-ref21">21</xref>] . The T<sub>1</sub> of PM, 5-CPM, 10-CPM and 15-CPM were in the range of 362˚C - 390˚C and T<sub>2</sub> of them was 510˚C. The CNTs starts thermal decomposition since T<sub>2</sub> and the weight remained at T<sub>2</sub> can explain to percentage of CNTs content in membrane. The remaining weight of 5, 10, 15-CPMs at T<sub>2</sub> was about 5.1, 9.4 and 14.7 wt%, respectively, which reveals that the real CNTs content in CPMs has well controlled in this research. The residue material at 800˚C about 1.0 wt% could be attributed to ash and metallic catalytic from CNTs [<xref ref-type="bibr" rid="scirp.70878-ref22">22</xref>] .</p></sec><sec id="s3_1_2"><title>3.1.2. Pore Size Distribution</title><p><xref ref-type="fig" rid="fig3">Figure 3</xref> displays the pore size distributions of membranes with micropores (&lt;2 nm), mesopores (2 - 50 nm) and macropores (50 - 300 nm). It can be seen that the PM has narrow micropores at 0.42 nm and has lower amount in mesopores/macropores volume. After adding CNTs into PM, the micropore size range has increased wider to 0.4 - 0.46 nm which can be attributed to the CNTs provided more pores from space of graphite interlayers in the range of 0.3 - 0.4 nm [<xref ref-type="bibr" rid="scirp.70878-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.70878-ref24">24</xref>] . The mesocopore/macropore volume of PM and CPMs were tenth of magnitude lower than micropore volumes of that. The CNTs content could effects mesocopore/macropore volume of CPM that has increased among of 5 - 70 nm with rising of CNT contents. It can be explained that the CNTs have a number of CNT cavity pores (10 nm) and aggregated pores (40 - 60 nm) which creating the pores in CPMs [<xref ref-type="bibr" rid="scirp.70878-ref25">25</xref>] .</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Pore size distributions of PM and various CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x6.png"/></fig></sec><sec id="s3_1_3"><title>3.1.3. FE-SEM</title><p>Figures 4(a)-(d) show the FE-SEM images of PM and CPMs surfaces. The PM surface can be seen smoother than CPMs surfaces. While the CNTs added into membranes, the membrane surface became rougher and created few surface macropores. The surface of all CPMs have obviously rugae-like structure that has space below 3 nm can be seen in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b-1). The surface macropores were in the range of 10 - 25 nm for 5-CPM, 10 - 35 nm for 10-CPMs and 10 - 130 nm for 15-CPMs, respectively, which can prove the CNT content effects on pore size of CPMs. The surface macropore quantity was increased with increasing CNT contents, which can be attributed to the CNTs has aggregated structure and the remained air bubbles in the aggregated pores during CPMs fabrication.</p></sec><sec id="s3_1_4"><title>3.1.4. Membrane Surface Roughness (R<sub>RMS</sub>)</title><p>R<sub>RMS</sub> was measured by atomic force microscopy (AFM) which can explain the surface roughness of membrane and its relation of water permeation. The higher value of R<sub>RMS</sub> reveals the membrane surface is rougher, more hydrophilic, more pore density and more pore volume that are related to filtration performance of membrane [<xref ref-type="bibr" rid="scirp.70878-ref26">26</xref>] . <xref ref-type="table" rid="table1">Table 1</xref> shows the R<sub>RMS</sub> roughness for PM and 5 - 15 CPMs membranes. The R<sub>RMS</sub> of PM was 35.6 nm which is lower than that of all CPMs. It’s the fact that increasing the addition of CNTs in polymer membrane can greater the surface roughness and thus changed the filtration performance.</p></sec><sec id="s3_1_5"><title>3.1.5. Optical Contact Angle of Membranes (θ)</title><p><xref ref-type="table" rid="table2">Table 2</xref> shows the optical contact angle (θ) of PM and CPMs. The θ of PM was less</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> SEM images of PM and various CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x7.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Surface roughness of membranes</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Membranes</th><th align="center" valign="middle" >R<sub>RMS</sub> (nm)</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >35.6</td></tr><tr><td align="center" valign="middle" >5-CPM</td><td align="center" valign="middle" >43.5</td></tr><tr><td align="center" valign="middle" >10-CPM</td><td align="center" valign="middle" >58.8</td></tr><tr><td align="center" valign="middle" >15-CPM</td><td align="center" valign="middle" >78.9</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Optical contact angle of membranes</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Membrane</th><th align="center" valign="middle" >θ (˚)</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >83.75 &#177; 2.36</td></tr><tr><td align="center" valign="middle" >5-CPM</td><td align="center" valign="middle" >76.07 &#177; 0.7</td></tr><tr><td align="center" valign="middle" >10-CPM</td><td align="center" valign="middle" >71.78 &#177; 2.03</td></tr><tr><td align="center" valign="middle" >15-CPM</td><td align="center" valign="middle" >59.95 &#177; 1.46</td></tr></tbody></table></table-wrap><p>than 90˚ which reveals the PM has the hydrophilic surface and has good affinity for water [<xref ref-type="bibr" rid="scirp.70878-ref27">27</xref>] . The θ of CPM were decreased with increasing CNT content and R<sub>RMS</sub>. It is the fact that the addition of CNT into membrane can enhance the hydrophilicity and roughness for membrane thus increasing the water permeation.</p></sec></sec><sec id="s3_2"><title>3.2. Effect of CNTs Content on Water Permeation</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> displays the water permeation flux (J<sub>v</sub>) of PM and all CPMs with operation time under permeation pressure 10 psi. The J<sub>v</sub> of PM and 5-CPM have stable J<sub>v</sub> from 10 to 420 min, but that of 10-CPMs and 15-CPMs have decreased then reached equilibrium after 300 min and 420 min, respectively. The decrease of J<sub>v</sub> for 10-CPM and 15-CPM are the conventional trend which relating to pore structure of membrane. The large pore size and larger R<sub>RMS</sub> could cause the water molecular accumulated on membrane and thus reducing the J<sub>v</sub>. The similar finding was reported in literatures [<xref ref-type="bibr" rid="scirp.70878-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.70878-ref29">29</xref>] . The J<sub>v</sub> at equilibrium time for PM, 5, 10, 15-CPMs are 2.0, 3.3, 4.6 and 7.1 L/m<sup>2</sup>∙h, respectively. It shows that all CPMs have greater J<sub>v</sub> than that of PM, which is a fact that more CNTs content can enhance more water permeability for membrane.</p></sec><sec id="s3_3"><title>3.3. Separation of BTEX</title><sec id="s3_3_1"><title>3.3.1. BTEX Removal<sup> </sup></title><p><xref ref-type="fig" rid="fig6">Figure 6</xref> exhibits the R of PM and all CPMs at a C<sub>f</sub> of 80 mg/L under pressure 10 psi. The R of 5-CPM was slightly lower than that of PM for BTEX. The R of PM and 5-CPM were respectively 97.4%, 94.3%, 82.6% and 73.8% for B, 99.9%, 97.6%, 87.2% and 79.8% for T, 99%, 97.9%, 89.6% and 85.0% for E, 99.2%, 97.7%, 90.7% and 84.7% for X at the equilibrium time 330 min. It can be seen that the membranes follow the order of PM &gt; 5-CPM &gt; 10-CPM &gt; 15-CPM for BTEX and PM, 5-CPM and 10-CPM have R above 80% but 15-CPM. This could be attributed to the increases of mesopoers/macropores from CNTs in 15-CPM resulting some BTEX molecules have penetrated through mem-</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Water flux of PM and CPMs at 10 psi permeate pressure</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x8.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> R of BTEX with PM and CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x9.png"/></fig><p>brane and make higher CNT content membrane have lower BTEX rejection. The 10-CPM is not only has R above 80% for BTEX, but also has greater J<sub>v</sub> than 5-CPM. Therefore, 10-CPM has been chosen to exam the following membrane studies.</p></sec><sec id="s3_3_2"><title>3.3.2. Effect of Permeation Pressure</title><p><xref ref-type="fig" rid="fig7">Figure 7</xref> shows the R and J<sub>v</sub> of 10-CPM under various permeation pressure (P) from 5 - 40 psi with C<sub>f</sub> = 80 mg/L of BTEX. The R<sub>j</sub> of BTEX has significant decreases with increasing of P, but J<sub>v</sub> of BTEX has increased with rising of P. The R of BTEX were more than 90% while P was less than 10 psi. Therefore, the P at 10 psi was optimal pressure for membrane operation above 90% of R for BTEX. The R of B, T, E, X were 90.7%, 93.4%, 95.1% and 95.4%, respectively. This shows the order of R for BTEX was B &lt; T &lt; E ≈ X that is consistent with the order of molecular weight and molecular size. It indicates that the separation performance of the BTEX from aqueous solutions with CPM is dependent on molecular physical property.</p></sec><sec id="s3_3_3"><title>3.3.3. Effect of Feed BTEX Concentrations</title><p><xref ref-type="fig" rid="fig8">Figure 8</xref> displays the effect of C<sub>f</sub> in 40, 80 and 120 mg/L with 10-CPM on 10 psi. The R of BTEX C<sub>f</sub> in 40, 80 and 120 mg/L at 180 min were 87.3%, 80.3% and 68.3% for B, 92.6%, 84.7% and 76.3% for T, 95.0%, 88.5% and 83.9% for E, 96.5%, 90.0% and 85.4%</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> R and Jv of BTEX for 10-CPMs under various permeation pressures</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x10.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Effect of BTEX initial concentration on R with 10-CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x11.png"/></fig><p>for X, respectively. The result shows that the R of BTEX were decreased with increasing C<sub>f</sub> of BTEX. The reason is that the higher C<sub>f</sub> can enhance the diffusion force and cause the BTEX molecular to diffuse into membrane. The R of BTEX have also decreased with filtration time, which can be attributed to the concentration accumulated on retentate side with time and then enhanced the diffusion force on membrane, thus reduced R. The R has significant decrease in filtration of B and T as compared with E and X which reveals that the B and T have smaller molecular size and diffused into membrane easier.</p></sec><sec id="s3_3_4"><title>3.3.4. Effect of Solution Ionic Strength</title><p>The μ, which is a general property of the solution affecting the affinity between the solute and the aqueous solution, was adjusted using NaCl solution. The polar solutes can be affected by μ and adsorbed on membrane surface to become electrical double layer, which could increase the penetration of solutes [<xref ref-type="bibr" rid="scirp.70878-ref30">30</xref>] . <xref ref-type="fig" rid="fig9">Figure 9</xref> exhibits the effects of solution ionic strength (μ) on the R of 10-CPM at a C<sub>f</sub> of 80 mg/L and P of 10 psi. The R of BTEX with μ in 0, 10, 100 mM at 180 min were 80.3%, 80.3% and 72.6% for B, 84.7%, 84.0% and 77.4% for T, 88.5%, 88.2% and 78.1% for E, 89.9%, 87.2% and 80% for X, respectively. It is apparent that the R with 10 mM has similar result with that without μ, but R with 100 mM was slightly lower (&lt;10%) than that without μ. The result shows that the effect of μ on the R was not significant for the μ below 100 mM.</p></sec><sec id="s3_3_5"><title>3.3.5. Effect of Solution Temperature</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref>0 exhibits the effects of solution temperature on the R of 10-CPM at a C<sub>f</sub> of 80 mg/L and P of 10 psi. The R of BTEX with temperature at 10˚C, 20˚C, 30˚C at 180 min</p><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Effect of μ on R of BTEX with 10-CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x12.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Effect of solution temperature on R with 10-CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x13.png"/></fig><p>were 89.4%, 80.3% and 75.0% for B, 92.4%, 84.7% and 79.9% for T, 94.1%, 88.5% and 83.8% for E, 95.2%, 90.0% and 80.9% for X, respectively. It’s obviously that the R of BTEX were decreased with increasing temperature, which is due to the thermal expansion of membrane that resultant the pore size enlarger in membrane thus reducing the R of BTEX [<xref ref-type="bibr" rid="scirp.70878-ref31">31</xref>] .</p></sec></sec><sec id="s3_4"><title>3.4. Separation of Mixed BTEX</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref>1 exhibits the R of mixed BTEX at a C<sub>f</sub> of 20 and 80 mg/L with 10-CPM at 10 psi. The R of mixed B, T, E, X at 180 min were respectively 74.5%, 77.3%, 80.2% and 80.3% for C<sub>f</sub> of 20 mg/L and 80.2%, 83.6%, 88.0% and 87.2% for C<sub>f</sub> of 80 mg/L. While the C<sub>f</sub> is 80 mg/L, the R of mixed BTEX is similar to that of individual BTEX (section 3.2.3) and following the same order (B &lt; T &lt; E ≈ X) which indicating that the separation mechanism of BTEX can be assigned to size exclusion. The J<sub>v</sub> of mixed BTEX at a C<sub>f</sub> of 20 and 80 mg/L on 180 min were decreased 21.4% and 34.7%, respectively. It is the fact that the fouling has taken place by concentration on membrane surface and thus decreased the water flux.</p></sec><sec id="s3_5"><title>3.5. Separation Mechanism</title><p>It is observed that the order of R with CPMs was in order of 5-CPM &gt; 10-CPM &gt; 15-CPM is consistent with pore size and specific pore volume. The R of BTEX have effected by permeation pressure, inlet concentration and temperature but not influenced by ionic strength. This indicates that the separation performance of the BTEX from aqueous solutions with CPMs is dependent on size exclusion. The diagram of nanofluid in CPMs and major mechanism for rejecting BTEX from aqueous solutions is graphically presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>2. The water molecules penetrate through the CPMs with</p><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Filtration of mixed BTEX with CPMs</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x14.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> Schematic diagram of nanofluid in CPMs and major mechanism for rejecting BTEX from aqueous solutions</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9402980x15.png"/></fig><p>four possible pathways including transport along CNT surface, direct permeation through membrane pores, transport through the cavity pores of CNTs, transport through the aggregated pores and hydrophobic effect [<xref ref-type="bibr" rid="scirp.70878-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.70878-ref32">32</xref>] . The BTEX were rejected by pore due to size exclusion to reject and thus make the fast separation of BTEX from aqueous solutions. These results reflect that the 10-CPMs possess good potential applications in the separation of the BTEX form aqueous solutions.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>This article studied the characteristics of PM and CPMs and their separation performance of BTEX from aqueous solutions. The rejection coefficients (R) of BTEX were dependent of the CNT content of CPM, pore size of membrane, molecule size of BTEX, permeation pressure (P), feed concentration (C<sub>f</sub>) and temperature, but has no significant influence on ionic strength (μ). The size exclusion plays the important roles on BTEX separation by CPMs. It reveals that the higher molecule size, the higher rejection. The 10-CPM behaved the better separation performance of BTEX with removal efficiencies of 80.3%, 84.7%, 88.5% and 90.0%, respectively, under the relatively lower pressure 10 psi. It has not only higher water flux but also the relatively higher R as comparing of 5% and 15% CNT of CPM. The majority pore size of 10-CPM was &lt;0.4 nm that is capable for removing BTEX which have molecule size &lt; 0.58 nm. This suggests that the 10-CPMs possess good potential for BTEX removal in wastewater treatment.</p></sec><sec id="s5"><title>Acknowledgements</title><p>Support from the National Science Council, Taiwan, under a contract no. of NSC97- 2221-E-005-036-MY3 is gratefully acknowledged.</p></sec><sec id="s6"><title>Cite this paper</title><p>Su, F.S., Lu, C. and Tai, J.-H. (2016) Separation of Benzene, Toluene, Ethylbenzene and P-Xylene from Aqueous Solutions by Carbon Nanotubes/ Polyvinylidene Fluoride Nanocomposite Mem- brane. 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