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Photonic crystals in biology - NanoTR-VI

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P ionsPP haveP contactPoster Session, Thursday, June 17Theme F686 - N1123The Creation of Hydrophobic Clay Surfaces with Long Cha<strong>in</strong> Hydrocarbon111UH. Hasan YolcuUP P*, Ahmet GürsesP P, and Met<strong>in</strong> AçkyldzP P,1PAtaturk University, K.K. Education Faculty, Dep. of Chemistry, 25240 ErzurumAbstract- In this study, the presence of lotus effect for the clay modified by us<strong>in</strong>g long cha<strong>in</strong> hydrocarbon was <strong>in</strong>vestigated. It wasfound the powder sample comparison with pellet form exhibits super hydrophobic character. This may be attributed to the chang<strong>in</strong>g ofroughness on the surface of modified clay particles depend<strong>in</strong>g on press<strong>in</strong>g and to the creat<strong>in</strong>g of higher energy surface with the adsorption oflong cha<strong>in</strong> hydrocarbon onto <strong>in</strong>terlayer region of clay.Non wettable surfaces with high water contact angle(WCA) and facile slid<strong>in</strong>g of drops are called superhydrophobic surface. Superhydrophobic surfaces with0water contact angles larger than 150P received a lotof research attention, due to important applications rang<strong>in</strong>gfrom self clean<strong>in</strong>g materials to microfluidic devices [1, 2].Many surfaces <strong>in</strong> nature are highly hydrophobic and selfclean<strong>in</strong>g (e.g. lotus leaves). The design synthesis andapplication of new k<strong>in</strong>ds of super hydrophobic and selfclean<strong>in</strong>g organic or <strong>in</strong>organic material will be essential andimportant task to fulfill [3].The clay sample was purified by sedimentation, dried atvacuum oven and sieved to give a 38-85 m (>%92) sizefraction us<strong>in</strong>g ASTM Standard sieves. Different amountsof hydrocarbon (0.05-1.0 g) was mixed with 500 mLaqueous solutions of CTAB (100, 200, 240, 260, 300, and320 mg/L). The mixture was shaken at 293 K, for 30 m<strong>in</strong>sand 1g clay sample was added to this mixture and shakenfor 30 m<strong>in</strong>s <strong>in</strong> a thermostatic shaker at 200 rpm. Themodified clay samples which produced by aboveprocedure were filtered through filter paper of Whatman41 and dried at 383 K <strong>in</strong> a vacuum oven for 2 h.and water droplets leads to ga<strong>in</strong><strong>in</strong>g the hydrophobiccharacter of samples. But the powder organoclay hassuperhydrophobic character, probably due to lotus effect.The variation of <strong>in</strong>itial CTAB concentration doesn’tsignificantly affect the contact angles of the pellet andpowder samples (Figure 2).Figure 2. Effect of <strong>in</strong>itial CTAB concentration on the contactangleIntensity (counts)200016001200800Raw clay*Correspond<strong>in</strong>g author: HThasanyolcu@atauni.edu.trT[1] M. Ma and R. M. Hill. Curr. Op<strong>in</strong>. Colloid Interface Sci. 11,193-202 (2006).[2] A. Tuteja, et al. Science. 318, 1618 -1622 (2007).[3] X , Feng and L, Jiang,. Adv. Mater. 18, 3063-3078 (2006).[4] H.Y. Erbil et al, Science. 299, 1377 (2003).40002 12 22 322Theta (deg)Figure 1. X-ray diffraction spectrums for raw clay and producedorgano-clayThe XRD patterns shows the <strong>in</strong>tensities of peaks for theorgano-clay sample were significantly decreased withcompared the raw clay. This attributed to the presence ofexfoliated clay layers. It can be said that the basal spac<strong>in</strong>g<strong>in</strong>creases, depend<strong>in</strong>g on ion-exchange occurred between+CTAP bounded hydrocarbon and the cations <strong>in</strong> the<strong>in</strong>terlayer region of clay (Figure 1).In this work, the contact angles for the powderorganoclay sample and pellet form were compared. It was0found that powder samples have 146P angle<strong>in</strong>dicat<strong>in</strong>g the presence of lotus effect. On the other hand,the surface roughness of modified clay particles changesdepend<strong>in</strong>g on press<strong>in</strong>g and the contact angle values0measured on the pellet reduce to about 90 P P. This showsthat the effect of surface roughness on the hydrophobiccharacter is predom<strong>in</strong>ant comparison with surface energy.Water droplets cannot penetrate <strong>in</strong>to the pores of thehydrophobic surfaces due to the trapped air [4]. In the bothforms, the reduc<strong>in</strong>g of contact areas between the surface6th Nanoscience and Nanotechnology Conference, zmir, 2010 735

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