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Photonic crystals in biology - NanoTR-VI

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PPoster Session, Thursday, June 17Theme F686 - N1123Preparation of Anion Exchange Membrane and Its Characterization by AFM and EFM111UZeynep ÇolakoluUP P*, Nilay GizliP P, Mustafa DemircioluP1PDepartment of Chemical Eng<strong>in</strong>eer<strong>in</strong>g, Ege University, Bornova, 35100, zmir, TurkeyAbstract-For the selective removal of arsenic species from water, a heterogeneous anion exchange membrane was prepared onpolyethylene backbone conta<strong>in</strong><strong>in</strong>g quaternized immobilized N-methyl-D-glucam<strong>in</strong>e (NMDG). Surface characterization and electrostaticconductivity of this material were <strong>in</strong>vestigated by atomic force microscopy (AFM) and electrostatic force microscopy (EFM). Roughnessvalues show that materials have no porosity, while positive values of surface skewness (1.398) po<strong>in</strong>t to extreme peaks on the membranesurface and surface kurtosis (2.174) lower than 3.0 to broader height distributions. Characterization of materials by AFM and EFM servedfor both optimization of preparation conditions and improvement of material properties.Safety <strong>in</strong> dr<strong>in</strong>k<strong>in</strong>g water is a challenge by climate change.Arsenic is important due to high toxicity and its high levelssome cities <strong>in</strong> Turkey. Ma<strong>in</strong> forms of arsenic met <strong>in</strong> groundwaters are arsenite or arsenate anions. Therefore theseparation by ion exchange comes as the first alternativemethod for ground waters. Removal performance of arsenicmust be enhanced for a viable <strong>in</strong>dustrial application. The aimof this study is to produce the anion exchange membranesand to characterize them by us<strong>in</strong>g AFM and EFM. Recentstudies show hopeful results <strong>in</strong> the name of us<strong>in</strong>g anionexchange membranes for the purification of water sourcesfrom hazardous ions s<strong>in</strong>ce these membranes have excellentelectrochemical properties [1].In this study, membranes were prepared by aheterogeneous method, <strong>in</strong> which powdered ion exchangeres<strong>in</strong> of NMDG was comb<strong>in</strong>ed with polyethylene, pressedand heated up till 250°C and kept for 10 m<strong>in</strong>. Then themembrane was subjected to morphological andelectrochemical characterization. The surface structure ofmembranes was observed by multimode AFM (RT-SHPM,NanoMagnetics Instruments). The membrane surfaces werescanned by alum<strong>in</strong>ium reflex coated silicon probe (Tap300AI, NanoMagnetics Instruments) hav<strong>in</strong>g the spr<strong>in</strong>gconstant of 40 N/m and the resonance frequency of 300 kHz<strong>in</strong> dynamic mode. Scan area and speed were chosen as210x10 μmP Pand 5 μ/s, respectively.The roughness parameters such as root mean squareroughness (RMS), mean roughness (Ra), average meanheight (Hav), surface skewness (Ssk) and surface kurtosis(Sku) were obta<strong>in</strong>ed by us<strong>in</strong>g built-<strong>in</strong> software SPM 1.16.13.It’s found that surface skewness was positive 1.398 which isalso numerically greater than 1.0 <strong>in</strong>dicates that it has extremepeaks on the surface [2]. Surface Kurtosis was found as2.174 which is lower than 3.0, so the membrane showsbroader height distributions [3]. Imag<strong>in</strong>g by EFM, anotherAFM technique, is used to characterize materials forelectrical properties. In this technique, a conductive AFM tip<strong>in</strong>teracts with the sample through long-range Coulombicforces. These <strong>in</strong>teractions change both oscillation amplitudeand phase of AFM cantilever, which are monitored to createEFM phase image [4]. In this study, the voltage levels werechosen as -4V and +4V for forward and backward potentials.Scan speed of 8μm/s was applied for the samples with the2area of 30 x 30μmP P.Figure 1. AFM and EFM Phase views of membranes.The image at the left <strong>in</strong> Figure 1 is an AFM image onwhich lighter regions show peaks on the sample surface, onEFM image (to the right) lighter regions representconductive areas. Various properties were observed bychang<strong>in</strong>g the parameters such as area scanned, scan speed,applied voltage, head lift, ris<strong>in</strong>g and fall<strong>in</strong>g time <strong>in</strong> order todeterm<strong>in</strong>e the optimum conditions for measurement. As aresult, before delv<strong>in</strong>g <strong>in</strong>to experimental tests andperformance studies requir<strong>in</strong>g large amount of material andlaborious tasks <strong>in</strong> a separation process, characterization ofmaterials by AFM and EFM dur<strong>in</strong>g preparation phase ofthem helps both to screen the alternatives and to optimize thepreparation conditions for the development of novelselective materials and the improvement of their properties.*Correspond<strong>in</strong>g author: HTzeynepcolakoglu@hotmail.comT[1] Punita V. Vyas, B.G. Shah, G.S. Trivedi, P. Ray, S.K.Adhikary, R. Rangarajan, Characterization of heterogeneous anionexchangemembrane, Journal of Membrane Science 187 (2001)[2] J. F. Jørgensen, L. L. Madsen, J. Garnaes, K. Carneiro, K.Schaumburg, Calibration, drift elim<strong>in</strong>ation and molecular structureanalysis, JVST B, 12(3), 1698-1701 (1994)[3] J. F. Jørgensen, N. Schmeisser, J. Garnaes, L. L. Madsen, K.Schaumburg, L. Hansen, P. Sommer-Larsen. (1994) Dynamicsand structure of selfassembled organic molecules at the solidliquid<strong>in</strong>terface, Journal of Surface & Coat<strong>in</strong>g Technology 67, pp.201-11[4] F. M. Serry, K. Kjoller, J. T. Thornton, R. J. Tench, and D.Cook. Electric Force Microscopy, Surface Potential Imag<strong>in</strong>g, andSurface Electric Modification with the Atomic Force Microscope(AFM).6th Nanoscience and Nanotechnology Conference, zmir, 2010 674

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