<?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">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2018.98048</article-id><article-id pub-id-type="publisher-id">MSA-85842</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></subj-group></article-categories><title-group><article-title>
 
 
  The Roles of Acidity on Sono-Electrodeposition of Silver Nanoparticles
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kareem</surname><given-names>N. Abed</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>Ahmed</surname><given-names>Q. Abdullah</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abdulkareem</surname><given-names>M. A. Alsammarraie</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Department of Chemistry, College of Science, University of Baghdad, Baghdad, Iraq</addr-line></aff><aff id="aff2"><addr-line>1Physics Department, College of Science, University of Baghdad, Baghdad, Iraq</addr-line></aff><aff id="aff1"><addr-line>Physics Department, College of Science, University of Baghdad, Baghdad, Iraq</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>samuraee2000@hotmail.com(AMAA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>06</day><month>07</month><year>2018</year></pub-date><volume>09</volume><issue>08</issue><fpage>671</fpage><lpage>678</lpage><history><date date-type="received"><day>31,</day>	<month>March</month>	<year>2018</year></date><date date-type="rev-recd"><day>3,</day>	<month>July</month>	<year>2018</year>	</date><date date-type="accepted"><day>6,</day>	<month>July</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>
 
 
  The Ag NPs were produced by sonicat the electrochemical cell that the titanium horn serves as cathode and the anode was high purity silver foil, while the electrolyte in all experiments was (0.2 g Ag in 250 ml deionized water), the pH was varied between 2 to 8 using sulfuric acid and sodium bicarbonate diluted solutions, the current density was maintained at 5mA/cm. The quality of the products was extensively examined using: SEM, TEM, AFM, XRD, UV-visible and EDX techniques. The results reflected a clear fact that the more acidic electrolyte (lower pH value) has produced distorted spherical larger AgNPs, with a narrow particles size distribution, while decreasing the acidity (higher pH value) led to smaller particle size, and wider size distribution spectrum.
 
</p></abstract><kwd-group><kwd>Silver Sulfate</kwd><kwd> Silver Nanoparticles</kwd><kwd> Sonoelectrodeposition</kwd><kwd> AFM</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Sonoelectrochemistry is the coupling of ultrasonic vibration to an electrochemical system. The term “sonoelectrochemistry” appeared at 1990 [<xref ref-type="bibr" rid="scirp.85842-ref1">1</xref>] . Recently there is a growing interest of the application of the sonoelectrochemistry in the preparation of nanopowders [<xref ref-type="bibr" rid="scirp.85842-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.85842-ref3">3</xref>] due to it is environmental friendly and cost effectiveness method compared to most of other methods including radiation, thermal decomposition, and vapor deposition, reduction in microemulsions and chemical reduction [<xref ref-type="bibr" rid="scirp.85842-ref4">4</xref>] . Ultrasound has been applied in the fields of electroplating, electroorganic synthesis, electropolymerisation, electroanalytical chemistry and for the electrochemical production of nanoparticles [<xref ref-type="bibr" rid="scirp.85842-ref5">5</xref>] . Sonoelectrochemical formation of nanoscale metals was accomplished by applying an electric current pulse for electrodeposition, followed by a burst of ultrasonic energy that removes the particles from the son electrode [<xref ref-type="bibr" rid="scirp.85842-ref6">6</xref>] . The propagation of pressure waves in a fluid causes the formation of cavitation bubbles. At low irradiation intensity, these bubbles oscillate none linearly in the acoustic field. Above a threshold, called the transient cavitation threshold, the number of bubbles increases intensely. The collapse of these bubbles, described as an implosion in the hot-spot theory, or described as a fragmentation in the electrical theory, is at the origin of extreme local conditions: high temperature and high pressure following the hot-spot theory, high electrical fields following the electrical theory [<xref ref-type="bibr" rid="scirp.85842-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.85842-ref8">8</xref>] . When the irradiation intensity is higher than the threshold intensity, the collapse of the bubbles is also associated with shock waves and microstreaming. Mechanical effects including erosion of solids, fragmentation of solid particles in suspension and emulsification of non-miscible liquids can occur. Under the influence of these extreme local conditions and also of these mechanical effects, sonochemistry takes place. Sonochemistry, which is thus defined as chemistry induced by sound and ultrasound, is a fast developing field. It is well know that the final application highly depends on the particle size, in this work the particle size of Ag NPs was tuned by variation of the pH of the Ag<sub>2</sub>SO<sub>4</sub> electrolyte.</p></sec><sec id="s2"><title>2. Experimental</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> show the experimental set-up used. In these experiments titanium probe (20 kHz) acts both as a cathode and an ultrasound emitter. The electroactive part of the sonoelectrode is the planar circular surface at the bottom of the horn and the immersed cylindrical part into the electrolyte is covered by an isolating plastic jacket.</p><p>The ultrasound probe is connected to a power supply using a pulse driver. The system used the simplest configuration of a two-electrode cell, where the silver sheet used as anode. Before each experiment, the titanium sonoelectrode have been polished [<xref ref-type="bibr" rid="scirp.85842-ref9">9</xref>] . The electrochemical processes were performed at (20˚C), the temperature of the electrolyte maintained to within &#177;1˚C with cooling and</p><p>heating water bath circulator. The distance between the anode and cathode was (30 mm). The working time of 1min was chosen, the electrolyte was (0.2 gm Ag<sub>2</sub>SO<sub>4</sub>, from Nanjing Chemical Reagent Co. in 250 ml DI) and some drops of H<sub>2</sub>SO<sub>4</sub>, 30 W/cm<sup>2</sup> ultrasound intensity and varying of pH value (2, 4, and 8). The silver foil was immersed in solution and using ultrasonic to obtaining silver nanoparticles. The produced AgNPs washed with distilled water and collected by Millipore nanofilter paper the characterized by atomic force microscopy (AFM), UV-visible spectra (UV-vis),Transmission electron microscopy (TEM) and X-ray diffraction (XRD) techniques.</p><p>The electroactive part of the sonoelectrode is the planar circular surface with an area of 7 cm<sup>2</sup> at the bottom of the horn. The immersed cylindrical part is covered by an isolating plastic jacket. A silver sheet (2.0 cm &#215; 2.0 cm) is used as a counter electrode.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>SEM images in <xref ref-type="fig" rid="fig2">Figure 2</xref>, AFM images in <xref ref-type="fig" rid="fig3">Figure 3</xref>, and TEM images in <xref ref-type="fig" rid="fig4">Figure 4</xref> reflected the effect of the electrolyte acidity (pH) on the morphologies of the Ag NPs produced at current density of (5 mA/cm<sup>2</sup>). These SEM and AFM images</p><p>reflected a clear fact that the more acidic electrolyte (lower pH value) have produced distorted spherical larger AgNPs (around 73 nm), with a narrow particles size distribution, while decreasing the acidity (higher pH value) led to smaller particle size (63 nm at pH5, and 48 nm at pH8), and wider size distribution spectrum. This manner may attributed to the lower repulsing forces between</p><p>partially positive charged Ag particles because of the more numbers of free cations in the more acidic electrolyte [<xref ref-type="bibr" rid="scirp.85842-ref9">9</xref>] .</p><p>The decreasing of the particle size follows the order: pH2 (73 nm) &gt; pH5 (63 nm) &gt; pH8 (48 nm).</p><p>The particle surface roughness (SR) according to the AFM analyses shows unorganized manner, the lowest (SR) was recorded at pH5 (1.2 nm) then at pH8 (2.8 nm), the higher value of (SR) was at pH2 (4.46 nm).</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows UV-Visible absorption spectrum of the aqueous solution of the produced Ag NPs at different pH values, the peak at 400 nm is a specific peak of Ag-NPs, and can therefore confirm the formation of NPs in the solution due to the surface Plasmon resonance (SPR) of Ag NPs, the smaller size is, the broader the absorption band will be [<xref ref-type="bibr" rid="scirp.85842-ref10">10</xref>] . By increasing the pH value the absorbance peaks shift to higher wavelength (red shift) meaning lower energies, the absorbance vs wavelength has a red shift for smaller particles.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> represent a typical XRD pattern of the produced silver nanoparticles</p><p>shows the presence of the diffraction peaks located at 38.35˚, 44.58˚ and 64.8729˚ corresponding to (111), (200) and (220) planes and identical with face centered cubic (fcc) structure (Card No. 96-901-3047) [<xref ref-type="bibr" rid="scirp.85842-ref11">11</xref>] . The peaks being broad, i.e. the crystalline size decrease, with decreasing electrolyte acidity (higher pH) as shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>By comparing the grain size deduced from SEM and AFM images, with the crystallite size calculated from XRD spectrums using, Sheerer equation, the number of crystal in grain can be represented as the ratio between these two values [<xref ref-type="bibr" rid="scirp.85842-ref12">12</xref>] , and the results are as follow: at pH2 = 73/37.7 = 2, at pH5 = 63/16.1 = 4, and at pH8= 48/13.2 = 3.63.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> XRD parameters of the Ag NPs synthesized by sonoelectrochemical method at different pH values. (a) pH2; (b) pH5; (c) pH8</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >pH</th><th align="center" valign="middle" >2θ (Deg.)</th><th align="center" valign="middle" >FWHM (Deg.)</th><th align="center" valign="middle" >d<sub>hkl</sub> Exp. (&#197;)</th><th align="center" valign="middle" >Crystallite Size (nm)</th><th align="center" valign="middle" >d<sub>hkl</sub> Std.(&#197;)</th><th align="center" valign="middle" >hkl</th><th align="center" valign="middle" >card No.</th></tr></thead><tr><td align="center" valign="middle"  rowspan="2"  >2</td><td align="center" valign="middle" >37.9746</td><td align="center" valign="middle" >0.2230</td><td align="center" valign="middle" >2.3675</td><td align="center" valign="middle" >37.7</td><td align="center" valign="middle" >2.3723</td><td align="center" valign="middle" >(111)</td><td align="center" valign="middle" >96-901-3047</td></tr><tr><td align="center" valign="middle" >44.1780</td><td align="center" valign="middle" >0.3559</td><td align="center" valign="middle" >2.0484</td><td align="center" valign="middle" >24.1</td><td align="center" valign="middle" >2.0545</td><td align="center" valign="middle" >(200)</td><td align="center" valign="middle" >96-901-3047</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >5</td><td align="center" valign="middle" >37.8220</td><td align="center" valign="middle" >0.2990</td><td align="center" valign="middle" >2.3767</td><td align="center" valign="middle" >28.1</td><td align="center" valign="middle" >2.3723</td><td align="center" valign="middle" >(111)</td><td align="center" valign="middle" >96-901-3047</td></tr><tr><td align="center" valign="middle" >44.0508</td><td align="center" valign="middle" >0.5339</td><td align="center" valign="middle" >2.0540</td><td align="center" valign="middle" >16.1</td><td align="center" valign="middle" >2.0545</td><td align="center" valign="middle" >(200)</td><td align="center" valign="middle" >96-901-3047</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >38.3559</td><td align="center" valign="middle" >0.6356</td><td align="center" valign="middle" >2.3449</td><td align="center" valign="middle" >13.2</td><td align="center" valign="middle" >2.3723</td><td align="center" valign="middle" >(111)</td><td align="center" valign="middle" >96-901-3047</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >44.5847</td><td align="center" valign="middle" >0.5339</td><td align="center" valign="middle" >2.0307</td><td align="center" valign="middle" >16.1</td><td align="center" valign="middle" >2.0545</td><td align="center" valign="middle" >(200)</td><td align="center" valign="middle" >96-901-3047</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >64.8729</td><td align="center" valign="middle" >0.5593</td><td align="center" valign="middle" >1.4362</td><td align="center" valign="middle" >16.8</td><td align="center" valign="middle" >1.4528</td><td align="center" valign="middle" >(220)</td><td align="center" valign="middle" >96-901-3047</td></tr></tbody></table></table-wrap></sec><sec id="s4"><title>4. Conclusion</title><p>Sono-electrodeposition of AgNPs was succeeded using Ag<sub>2</sub>SO<sub>4</sub> electrolyte, decreasing the acidity of the electrolyte (higher pH) in the range pH2 to 8 produced lower particle size of AgNPs.</p></sec><sec id="s5"><title>Cite this paper</title><p>Abed, K.N., Abdullah, A.Q. and Alsammarraie, A.M.A. (2018) The Roles of Acidity on Sono-Electrodeposition of Silver Nanoparticles. Materials Sciences and Applications, 9, 671-678. https://doi.org/10.4236/msa.2018.98048</p></sec></body><back><ref-list><title>References</title><ref id="scirp.85842-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mason, T.J. and Lorimer, J.P. (2002) Applied Sonochemistry: The Uses of Power Ultrasound in Chemistry and Processing. 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