The Synthesis of Solvent-Free TiO2 Nanofluids through Surface Modification
P. Y. Yu, Y. P. Zheng, L. Lan
Northwestern Polytechnical University.
DOI: 10.4236/snl.2011.12008   PDF    HTML   XML   5,907 Downloads   11,998 Views   Citations

Abstract

TiO2 nanoparticles with surface hydroxyl groups are treated by trimethoxysilane (CH3O)3Si(CH2)3O(CH2CH2O)6-9CH3 and a inorganic core/organic shell hybridmaterials, which shows itself a yellow viscous fluid, is obtained. We call it solvent-free TiO2 nanofliuds. Transmission electron microscopy (TEM), Fourier transform infrared spectrum (FTIR), differential scanning calorimetry (DSC), thermogravimetric analysis (TGA) and rheometer are adopted to characterize the product. As a result, the content of TiO2 nanoparticles in the nanofliuds is about 5.5wt%, the functionalized TiO2 nanoparticles possess better dispersion, very low viscosity and an obvious liquid-like behavior at room temperature in absence of solvent.

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Yu, P. , Zheng, Y. and Lan, L. (2011) The Synthesis of Solvent-Free TiO2 Nanofluids through Surface Modification. Soft Nanoscience Letters, 1, 46-50. doi: 10.4236/snl.2011.12008.

1. Introduction

Nanoparticles have many unique mechanical, magnetic, thermal, optical, catalytic properties, but its agglomeration due to high surface energy and surface activity hinders their application [1,2].

A method for solving this problem is to disperse nanoparticles in a base fluid, known as nanofluids, is studied for many years. The nanofluids is composed of two parts, including solvents and nanoparticles. The solvents of nanofluids are always water, oil, acetone, decene and ethylene glycol, and the nanoparticles used are usually metallic particles [3,4], metallic and nonmetallic oxides [5-7], carbon nanotube [8], etc. These conventional nanofluids improve the dispersion of nanoparticles to a certain extent, but the system is a kind of suspension and unstable, nanoparticles in the nanofluids may aggregate and settle down [9]. The factors influencing the stability and properties of nanofluids include the nanoparticle’s concentration, dispersant, viscosity of system [10], moreover, the variety, diameter [11,12], density of nanoparticle and ultrasonic vibration are not be ignored [13].

Recently, some researchers synthesize a new series of nanofluids which can flow at low temperature in absence of solvent (liquid) by surface modification. These solvent-free nanofluids involve SiO2 [14,15], TiO2 [16], CaCO3, C60 [17], ZnO [18], carbon naotube [19-21], etc. By the chemical reactions between active groups on the nanoparticles’ surface (always hydroxyl groups) and the organic modifier, an organic soft shell forms on the surface of nanoparticles, it can not only reduce the agglomeration of nanoparticles, but also impart new properties to them.

Actually, another method is to introduce the nanoparticle into block copolymer nanostructures. Prof. Ruckenstein and co-worker have been identified it [22,23].

In this paper, we select the organic reagent (CH3O)3 Si(CH2)3O(CH2CH2O)6–9CH3 to modify TiO2 nanoparticles, which is synthesized by sol-gel method. The silanol groups in the modifier can interact with hydroxyl groups on the surface of nanostructures, after a long reaction process, TiO2 nanoparticles are coated by a mass of organic molecular and a core-shell structure forms. The new system possesses much better dispersion and can flow at the room temperature.

2. Materials and Methods

2.1. Raw Materials

Tetra-n-butyl titanate was purchased from TianJing KeMiou Chemical Company. Methanol (CH3OH, 99.5%), ethanol, HCl (36% - 38%), ammonia(NH4OH) and tetrahydrofuran were purchased as analytical grade reagents from Fuchen Chemical Ind., Ltd., and used without further purification. Deionized water was made in lab. (CH3O)3Si(CH2)3N+(CH3)(C10H21)2Clin methanol (40%) was from Gelest. C9H19-C6H4-(OCH2-CH2)20(CH2)3K+ was from Sigma-aldrich.

2.2. Synthesis of TiO2 Nanoparticles

TiO2 nanoparticles were prepared by a sol-gel method through Tetrabutyl titanate hydrolysis. 17mL of Tetrabutyl titanate was mixed with 15mL of ethanol. The mixture was called as solution A. Solution B was prepared by mixing 15mL of ethanol, 2 mL of 5.5 mol/L hydrochloric acid solution, and1mL of deionized water. Then trickled solution B slowly to solution A with stiring constantly, and stop the experiment after the formation of gel. The gel was aged for 6 h at room temperature and carefully grinded after drying at 65˚C.

2.3. Synthesis of TiO2 Nanofluids

For the TiO2 nanofluids, 0.5 g of TiO2 powder was dispersed in 10mL of ammonia (pH 10), the suspension was treated with ultrasonic for 30 min, then 2.5 g (CH3O)3 Si(CH2)3O(CH2CH2O)6–9CH3 was added. The mixture was placed in a sealed single-mouth flask and treated at 70˚C for 24 h. The final solution was extracted with toluene three times, the aqueous layer was collected and dried at 65˚C. The dried material was dispersed in 20mL of deionized water and extracted with toluene three times again. After collecting the aqueous layer, the solution was dried at 65˚C. Subsequently, the material was dispersed in 20 mL of the acetone, after centrifugation, the transparent sol was dried at 65˚C. The product is a yellow transparent liquid.

2.4. Characterizations

The structure of the TiO2 nanofluids was investigated by Fourier transform-infrared (FTIR) spectrometer analysis (WQF-310, Beijing Second Optical Instruments Factory) using KBr pellets. Transmission electron microscope (TEM) images were obtained on a Hitachi H-800 instrument at an accelerating voltage of 200 kV, placing a few drops of the dispersion on a copper grid, and evaporating them prior to observation. The thermogravimeric analysis (TGA) measurements were taken under N2 flow by using TA TGAQ50 instrument. Differential scanning calorimetry (DSC) traces were recorded collected on a TA Q1000 Instruments, heating rate of 10˚C/min, from −60˚C to 60˚C. Rheological properties were studied by using the rheometer of TA AR-G2 instrument, heating rate of 5˚C/min.

3. Results and Discussion

The FTIR spectra of the TiO2 nanofluids are presented in Figure 1. The figure shows that they all have peak(s) at 450 cm−1 - 700 cm−1 which is the location of characteristic peaks of titania. The TiO2 nanofluids also have many new absorption peaks of organic groups compared with pure TiO2 nanoparticles. In theory, the reaction between TiO2 nanoparticles and (CH3O)3Si(CH2)3O(CH2CH2O)6–9 CH3 can yield Ti-O-Si, Si-O-Si bonds, from the spectra, their peaks are found at 944 cm-1 and 1110 cm-1 respectively [24]. In addition, the peak of stretching vibration of polyoxyethene is also observed at 1110 cm-1 overlapping with Si-O-Si. The strong peak at 3459 cm-1 is attributed to the presence of remaining hydroxyl groups on the TiO2 nanoparticles. The results prove that the modifier has been grafted on the surface of TiO2 nanoparticles.

The microstructure of the pure TiO2 nanoparticals and TiO2 nanofluids could be clearly observed from the TEM images (Figure 2). As shown in Figure 2, the pure TiO2 nanoparticals have serious phenomenon of agglomeration, its dispersion is significantly improved after modification. The modifier protects TiO2 nanoparticles from agglomeration and probably can improve its compatibility with organic materials.

Figure 3 is the DSC curve of the modifier (CH3O)3 Si(CH2)3O(CH2CH2O)6–9CH3 and the TiO2 nanofluids. In the heating process, both the modifier and TiO2 nanofluids show a second order transition at −50˚C, corresponding to the glass transition temperature (Tg). The first order transition of the modifier occurs at −0.4˚C, corresponding to the melting temperature (Tm). Differently, the TiO2 nanofluids has two first order transition at −27˚C and −3.6˚C, this may be the result of oligomeric siloxane of different molecular weight produced during the modification [22]. The two possess the same Tg (−50˚C), the

Conflicts of Interest

The authors declare no conflicts of interest.

References

[1] Z. X. Yan, J. Deng and Z. M. Luo, “A Comparison Study of the Agglomeration Mechanism of Nano and Micrometer Aluminum Particles,” Materials Characterization, Vol. 61, No. 2, 2010, pp. 198-205. doi:10.1016/j.matchar.2009.11.010
[2] S. L. Kuo, Y. C. Chen, M. D. Ger and W. H. Hwu, “Nano-Particles Dispersion Effect on Ni/Al2O3 Composite Coatings,” Materials Chemistry and Physics, Vol. 86, No. 1, 2004, pp. 5-10. doi:10.1016/j.matchemphys.2003.11.040
[3] C. Y. Tsai, H. T. Chien, P. P. Ding, B. Chan, T. Y. Luh and P. H. Chen, “Effect of Structural Character of Gold Nanoparticles in Nanofluid on Heat Pipe Thermal Performance,” Material Letters, Vol 58, No. 9, 2004, pp. 1461-1465. doi:10.1016/j.matlet.2003.10.009
[4] D. W. Zhou, “Heat Transfer Enhancement of Copper Nano?uid with Acoustic Cavitation,” International Journal of Heat and Mass Transfer, Vol. 47, No. 14-16, 2004, pp. 3109-3117. doi:10.1016/j.ijheatmasstransfer.2004.02.018
[5] W. Yu, H. Q. Xie, L. F. Chen and Y. Li, “Investigation of Thermal Conductivity and Viscosity of Ethylene Glycol Based Zno Nano?uid,” Thermochimica Acta, Vol 491, No. 1-2, 2009, pp. 92-96. doi:10.1016/j.tca.2009.03.007
[6] C. T. Nguyen, G. Roy, C. Gauthier and N. Galanis, “Heat Transfer Enhancement Using Al2O3–Water Nano?uid for an Electronic Liquid Cooling System,” Applied Thermal Engineering, Vol. 27, No. 8-9, 2007, pp. 1501-1506. doi:10.1016/j.applthermaleng.2006.09.028
[7] D. Milanova and R. Kumar, “Heat Transfer Behavior of Silica Nanoparticles in Pool Boiling Experiment,” Journal of Heat Transfer, Vol. 130, No. 4, 2008, pp. 042401- 042407. doi:10.1115/1.2787020
[8] M. E. Meibodi, M. Vafaie-Sefti, A. M. Rashidi, A. Amrollahi, M. Tabasi and H. S. Kalal, “The Role of Different Parameters on The Stability and Thermal Conductivity of Carbon Nanotube/Water Nano?uids,” International Communications in Heat and Mass Transfer, Vol. 37, No. 3, 2010, pp. 319-323. doi:10.1016/j.icheatmasstransfer.2009.10.004
[9] W. T. Jiang, G. L. Ding, H. Peng and H. T. Hu, “Modeling of Nanoparticles’ Aggregation and Sedimentation in Nano?uid,” Current Applied Physics, Vol. 10, No. 3, 2010, pp. 934-941. doi:10.1016/j.cap.2009.11.076
[10] A. N. Eiyad, “Effects of variable viscosity and thermal conductivity of Al2O3–water nano?uid on heat transfer enhancement in natural convection,” Inernational Journal of Heat Fluid Flow, Vol. 30, No. 4, 2009, pp. 679-690.
[11] T. P. Teng, Y. H. Hung, T. C. Teng, H. E. Mo and H. G. Hsu, “The Effect of Alumina/Water Nano?uid Particle Size on Thermal Conductivity,” Applied Thermal Engineering, Vol. 30, No. 14-15, 2010, pp. 2213-2218. doi:10.1016/j.applthermaleng.2010.05.036
[12] K. B. Anoop, T. Sundararajan and S. K. Das, “Effect of Particle Size on the Convective Heat Transfer in Nano?uid in the Developing Region,” International Journal of Heat and Mass Transfer, Vol. 52, No. 9-10, 2009, pp. 2189-2195. doi:10.1016/j.ijheatmasstransfer.2007.11.063
[13] Y. J. Li, J. E. Zhou, S. Tung and E. Schneider, S. Q. Xi, “A Review on Development of Nano?uid Preparation and Characterization,” Powder Technology, Vol. 196, No. 2, 2009, pp. 89-101. doi:10.1016/j.powtec.2009.07.025
[14] A. B. Bourlinos, S. R. Chowdhury, D. D. Jiang and Q. Zhang, “Weakly Solvated PEG-Functionalized Silica Nanoparticles with Liquid-Like Behavior,” Journal of Materials Science, Vol. 40, No. 18, 2005, pp. 5095-5097. doi:10.1007/s10853-005-1301-8
[15] A. B. Bourlinos, R. Herrera, N. Chalkias, D. D. Jiang, Q. Zhang, L. A. Archer and E. P. Giannelis, “Surface-Func- Tionalized Nanoparticals with Liquid-Like Behavior,”Advanced Materials, Vol. 17, No. 2, 2005, pp. 234-237. doi:10.1002/adma.200401060
[16] A. B. Bourlinos, S. R. Chowdhury, R. Herrera, D. D. Jiang, Q. Zhang, L. A. Archer and E. P. Giannelis, “Functionalized Nanostructures with Liquid-Like Behavior: Expanding the Gallery of Available Nanostructures,” Advanced Functional Materials, Vol. 15, No. 8, 2005, pp. 1285-1290. doi:10.1002/adfm.200500076
[17] T. Michinobu, T. Nakanishi, J. P. Hill, M. Funahashi and K. Ariga, “Room Temperature Liquid Fullerenes: An Uncommon Morphology of C60 Derivatives,” Journal of the American Chemical Society, Vol. 128, No. 32, 2006, pp. 10384-10385. doi:10.1021/ja063866z
[18] A. B. Bourlinos, A. Stassinopoulos, D. Anglos, R. Herrera, S. H. Anastasiadis, D. Petridis and E. P. Giannelis, “Functionalized Zno Nanoparticals with Liquidlike Behavior and Their Photoluminescence Properties,” Small. Vol. 2, 2006, p. 513. doi:10.1002/smll.200500411
[19] J. X. Zhang, Y. P. Zheng, P. Y. Yu, S. Mo and R. M. Wang, “Modified Carbon Nanotubes with Liquid-Like Behavior At 45?C,” Carbon. Vol. 47, No. 12, 2009, p. 2776. doi:10.1016/j.carbon.2009.05.036
[20] J. X. Zhang, Y. P. Zheng, P. Y. Yu, S. Mo and R. M. Wang, “The Synthesis of Functionalized Carbon Nanotubes by Hyperbranched Poly (Amine-Ester) with Liquid-Like Behavior at Room Temperature,” Polymer. Vol. 50, No. 13, 2009, p. 2953. doi:10.1016/j.polymer.2009.04.042
[21] J. X. Zhang, Y. P. Zheng, L. Lan, S. Mo, P. Y. Yu, W. Shi and R. M. Wang, “Direct Synthesis of Solvent-Free Multiwall Carbon Nanotubes/Silica Nonionic Nano?uid Hybrid Material,” Acs Nano, Vol. 3, No. 8, 2009, p. 2185. doi:10.1021/nn900557y
[22] H. Y. Chen and E. Ruckenstein, “Structure and Particle Aggregation in Block Copolymer-Binary Nanoparticle Com- Posites,” Polymer, Vol. 51, No. 24, 2010, p. 5869. doi:10.1016/j.polymer.2010.10.011
[23] H. Y. Chen and E. Ruckenstein, “Nanoparticle aggregation in the presence of a block copolymer,” Journal of Chemical Physics, Vol. 131, No. 24, 2009, article ID 244904. doi:10.1063/1.3280064
[24] S. Q. Huang, Z. G. Sun and S. B. Li, “New Silicone Polymer,” in Chinese, Chemical Industry Press, Beijing, 2004.

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