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Photonic crystals in biology

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Poster Session, Tuesday, June 15<br />

Theme A1 - B702<br />

Synthesis and Characterization of Electrospun Ba 0.6 Sr 0.4 TiO 3 Nanofibers and 3-3 Nanocomposites<br />

Yahya Toprak, 1 Ebru Menur Alkoy 2 and Sedat Alkoy 1,*<br />

1 Department of Materials Science and Eng<strong>in</strong>eer<strong>in</strong>g, Gebze Institute of Technology, Kocaeli 41400, Turkey<br />

2 Faculty of Eng<strong>in</strong>eer<strong>in</strong>g, Maltepe University, Istanbul 34857, Turkey<br />

Abstract— Barium strontium titanate – Ba 0.6 Sr 0.4 TiO 3 (BST) nanofibers with diameters of 50–200 nm were prepared<br />

us<strong>in</strong>g electrospun BST/polyv<strong>in</strong>ylpyrrolidone (PVP) fibers by calc<strong>in</strong>ation for 1 h at temperatures <strong>in</strong> the range of 650–800ºC<br />

<strong>in</strong> air. The morphology and crystal structure of calc<strong>in</strong>ed BST/PVP nanofibers were characterized us<strong>in</strong>g SEM and XRD.<br />

Nanocomposites with 3-3 phase connectivity were prepared by <strong>in</strong>filtrat<strong>in</strong>g an epoxy matrix phase <strong>in</strong>to the nanofiber mats.<br />

Dielectric properties of the BST/epoxy nanocomposites were evaluated for tunable microwave dielelectric applications.<br />

BST powders were also prepared by gelation and dry<strong>in</strong>g of BST precursor sol-gel solutions. Dried gels were then<br />

calc<strong>in</strong>ed, ground, pressed and s<strong>in</strong>tered to obta<strong>in</strong> dense BST ceramics. Electrical properties of BST ceramics were<br />

determ<strong>in</strong>ed through dielectric and PE hysteresis measurements.<br />

Barium strontium titanate - Ba 1x Sr x TiO 3 (BST) is a<br />

perovskite type material with a ferroelectric-paraelectric<br />

transition temperature that can be tuned from 30 to 400 K by<br />

vary<strong>in</strong>g the Ba/Sr ratio [1]. Solid solutions with x = 0.2 to<br />

0.5 are normally used to shift the transition temperature to,<br />

or just below, room temperature. BST solid solutions have<br />

unique comb<strong>in</strong>ation of large dielectric constant, high<br />

tunability, low dc leakage, low loss tangent, and stable<br />

operation at high temperature [2]. With this comb<strong>in</strong>ation of<br />

favorable properties, BST f<strong>in</strong>ds niche <strong>in</strong> tunable microwave<br />

devices such as microwave tunable phase shifters, tunable<br />

filters, and high-Q resonators for radar and communication<br />

applications [3]. Fiberization of the functional ceramics<br />

expand their utility <strong>in</strong>to the micro and nanodevices, and<br />

<strong>in</strong>corporation of these fibers <strong>in</strong>to composite structures<br />

provides an added flexibility and mechanical <strong>in</strong>tegrity [4].<br />

Electrosp<strong>in</strong>n<strong>in</strong>g represents a simple and versatile method for<br />

prepar<strong>in</strong>g ceramic fibers <strong>in</strong> the nanoscale range [5].<br />

In the preparation of BST precursor sol-gel solution<br />

barium acetate, strontium acetate and titanium isopropoxide<br />

were used as source materials. A mixture of acetic acid and<br />

2-methoxyethanol with 1:2 mix ratio was used as solvent.<br />

Poly(v<strong>in</strong>ylpyrrolidone) (PVP) was used as the carrier<br />

polymer. The Ba:Sr molar ratio was 0.6:0.4 and the molarity<br />

of the f<strong>in</strong>al precursor solution was 0.27 M. Various PVP<br />

additions from 5 to 30 wt% were studied. The electric field<br />

dur<strong>in</strong>g the electrosp<strong>in</strong>n<strong>in</strong>g process was varied from 10 to 20<br />

kV/cm and the pump<strong>in</strong>g rate from 1 to 5 l/h.<br />

Electrospun BST/polyv<strong>in</strong>ylpyrrolidone (PVP) fibers were<br />

obta<strong>in</strong>d by calc<strong>in</strong>ation for 1 h at temperatures <strong>in</strong> the range of<br />

650–800ºC <strong>in</strong> air. The morphology and crystal structure of<br />

calc<strong>in</strong>ed BST/PVP nanofibers were characterized us<strong>in</strong>g<br />

SEM and XRD. Nanocomposites with 3-3 phase<br />

connectivity were prepared by <strong>in</strong>filtrat<strong>in</strong>g an epoxy matrix<br />

phase <strong>in</strong>to the nanofiber mats. Dielectric properties of the<br />

BST/epoxy nanocomposites were evaluated for tunable<br />

microwave dielelectric applications. BST powders were<br />

also prepared by gelation and dry<strong>in</strong>g of BST precursor solgel<br />

solutions. Dried gels were then calc<strong>in</strong>ed, ground, pressed<br />

and s<strong>in</strong>tered to obta<strong>in</strong> dense BST ceramics. Electrical<br />

properties of BST ceramics were determ<strong>in</strong>ed through<br />

dielectric and PE hysteresis measurements.<br />

X-ray diffraction patterns presented <strong>in</strong> Fig. 1 for calc<strong>in</strong>ed<br />

BST powders <strong>in</strong>dicate that a calc<strong>in</strong>ation temperature of<br />

700ºC was enough to obta<strong>in</strong> pure BST phase with perovskite<br />

structure. The scann<strong>in</strong>g electron micrograph shown <strong>in</strong> Fig.<br />

2 <strong>in</strong>dicates that nanofibers with diameters rang<strong>in</strong>g from 50<br />

to 200 nm can be obta<strong>in</strong>ed without the formation of<br />

undesired beads.<br />

Figure 1. XRD pattern of BST powders calc<strong>in</strong>ed at 700ºC-1 h.<br />

Figure 2. SEM micrograph of the as deposited BST/PVP<br />

nanofibers.<br />

The dielectric constant of the bulk BST ceramic pellets<br />

were as high as 2000 with a dielectric loss of less than 2%<br />

measured at room temperature at 100 kHz. The polarization<br />

vs. electric field hysteresis loops <strong>in</strong>dicates a ferroelectric<br />

behavior with a remnant polarization of 5 C/cm 2 and a<br />

coercive field of 15 kV/cm measured under an electric field<br />

of 50 kV/cm.<br />

*Correspond<strong>in</strong>g author: sedal@gyte.edu.tr<br />

[1] K.V. Saravanan et al., Mater. Chem. Phy. 105, 426 (2007).<br />

[2] S. Maensiri et al., J. Colloid Interface Sci. 297, 578 (2006).<br />

[3] D.Y. Lee et al., J Sol-Gel Sci Technol 53, 43 (2010).<br />

[4] E.M Alkoy et al., J. Amer. Ceram. Soc. 92, 2566 (2009).<br />

[5] R. Ramaseshan et al., J. Appl. Phys. 102, 111101 (2007).<br />

6th Nanoscience and Nanotechnology Conference, zmir, 2010 328

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