• No se han encontrado resultados

Localización y características

3. MATERIALES Y METODOS

3.1. EXPERIMENTO A

3.1.1. Localización y características

In this chapter we describe the alignment kinetics of an assembly of non- interacting magnetic nanorods suspended in different fluid.

We first studied an assembly of magnetic nanorods suspended in a Newtonian fluid with constant viscosity  and subject to an external magnetic field B. It has been shown that the alignment kinetics is controlled by a single parameter β. We theoretically predicted and experimentally confirmed that one can control the alignment of an assembly of nanorods by choosing the parameter β and time of application of the external field. Experiments with nickel nanorods covered with PVP in a glycerol–water mixture supported the theory.

Next, we describe we theoretically studied the kinetics of ordering of an assembly of nanorods suspended in a solidifying liquid film. The process of solidification was

104

modeled by assuming that the film viscosity increases with time exponentially fast and nanorods are randomly distributed in the films prior to the application of external magnetic field. We showed that the nanorods would not always align parallel to the external magnetic field; some of them will be quenched halfway to the equilibrium orientation prior to the film solidification. Different regimes of ordering were revealed and classified and the time required for the nanorods to align along the field direction was analyzed depending on the physical parameters of the liquids and nanorod materials. Fortunately, all physical parameters were collapsed in a single dimensionless parameter

U0 defined by eq.(4.15). This parameter controls the alignment kinetics and limiting distribution of nanorods in the film and resulting magnetization of the film. We introduced a criterion of the nanorod ordering and constructed phase diagrams shown in Figure 4.16. These phase diagrams predict the physical conditions ensuring the complete order of nanorods in the film providing maximum possible magnetization.

4.6 References

1. Song, S.Q., Bohuslav, G., Capitano, A., Du, J., Taniguchi, K., Cai, Z.H., and Sun, L. (2012). Experimental characterization of electrochemical synthesized Fe nanowires for biomedical applications. J Appl Phys 111.

2. Salem, A.K., Hung, C.F., Kim, T.W., Wu, T.C., Searson, P.C., and Leong, K.W. (2005). Multi-component nanorods for vaccination applications. Nanotechnology

16, 484-487.

3. Wanekaya, A.K., Chen, W., Myung, N.V., and Mulchandani, A. (2006). Nanowire-based electrochemical biosensors. Electroanal 18, 533-550.

4. McGary, P.D., Tan, L.W., Zou, J., Stadler, B.J.H., Downey, P.R., and Flatau, A.B. (2006). Magnetic nanowires for acoustic sensors (invited). J Appl Phys 99.

5. Tokarev, A., Rubin, B., Bedford, M., and Kornev, K.G. (2010). Magnetic Nanorods for Optofluidic Applications. Aip Conf Proc 1311, 204-209.

6. Kayani, A.A., Khoshmanesh, K., Ward, S.A., Mitchell, A., and Kalantar-Zadeh, K. (2012). Optofluidics incorporating actively controlled micro- and nano- particles. Biomicrofluidics 6.

105

7. Wilhelm, C., Gazeau, F., and Bacri, J.C. (2003). Rotational magnetic endosome microrheology: Viscoelastic architecture inside living cells. Phys Rev E 67. 8. Tokarev, A., Luzinov, I., Owens, J.R., and Kornev, K.G. (2012). Magnetic

Rotational Spectroscopy with Nanorods to Probe Time-Dependent Rheology of Microdroplets. Langmuir 28, 10064-10071.

9. Celedon, A., Hale, C.M., and Wirtz, D. (2011). Magnetic Manipulation of Nanorods in the Nucleus of Living Cells. Biophys J 101, 1880-1886.

10. Tokarev, A., Kaufman, B., Gu, Y., Andrukh, T., Adler, P.H., and Kornev, K.G. (2013). Probing viscosity of nanoliter droplets of butterfly saliva by magnetic rotational spectroscopy. Appl. Phys. Lett. 102.

11. Nikitin, L.V., Mironova, L.S., Kornev, K.G., and Stepanov, G.V. (2004). The magnetic, elastic, structural, and magnetodeformational properties of magnetoelastics. Polym. Sci. Ser. A 46, 301-309.

12. Filipcsei, G., Csetneki, I., Szilagyi, A., and Zrinyi, M. (2007). Magnetic field- responsive smart polymer composites. Advances in Polymer Science 206, 137- 189.

13. Erb, R.M., Libanori, R., Rothfuchs, N., and Studart, A.R. (2012). Composites Reinforced in Three Dimensions by Using Low Magnetic Fields. Science 335, 199-204.

14. Itoh, K., Ishida, S., Hamada, M., and Ogawa, S. (1979). Super - alignment of magnetic particles on coated disks and its effects on the recording characteristics. J Appl Phys 50, 2396-2398.

15. Chou, T.-W. (1992). Microstructural Design of Fiber Composites, (Cambridge, UK Cambridge University Press).

16. Richter, H.J. (1993). Media Requirements and Recording Physics for High- Density Magnetic Recording. Ieee Transactions on Magnetics 29, 2185-2201. 17. Richter, H.J. (1999). Recent advances in the recording physics of thin-film media.

Journal of Physics D-Applied Physics 32, R147-R168.

18. Eiling, A. (1987). High-density magnetic recording - theory and practical considerations. J Appl Phys 62, 2404-2418.

19. Doi, M., and Edwards, S.F. (1988). The theory of polymer dynamics, Paperback, with corrections. Edition, (Oxford: Clarendon Press).

20. Newman, J.J., and Yarbroug.Rb (1968). Motions of a magnetic particle in a viscous medium J Appl Phys 39, 5566-&.

21. Tirado, M.M., and Garciadelatorre, J. (1980). Rotational-Dynamics of Rigid, Symmetric Top Macromolecules - Application to Circular-Cylinders. J Chem Phys 73, 1986-1993.

22. Blums, E., Cebers, A., and Maiorov, M.M. (1997). Magnetic fluids, (New York: Walter de Gruyter ).

23. Ghosh, A., Mandal, P., Karmakar, S., and Ghosh, A. (2013). Analytical theory and stability analysis of an elongated nanoscale object under external torque. Physical Chemistry Chemical Physics 15, 10817-10823.

24. Perlov, C.M., and Middleman, S. (1987). Dynamics of orientation in particulate madia. J Appl Phys 61, 3892-3894.

106

25. Courant, R., and Hilbert, D. (1989). Methods of mathematical physics, (New York: Interscience Publishers).

26. Gupta, M.K., Kulkarni, D.D., Geryak, R., Naik, S., and Tsukruk, V.V. (2013). A Robust and Facile Approach To Assembling Mobile and Highly-Open Unfrustrated Triangular Lattices from Ferromagnetic Nanorods. Nano Lett 13, 36- 42.

27. Association, G.P. (1963). Physical Properties of Glycerine and Its Solutions, (Glycerine Producers' Association).

28. Onsager, L. (1949). The effects of shape on the interaction of colloidal particles. Annals of the New York Academy of Sciences 51, 627-659.

29. Kayser, R.F., and Raveche, H.J. (1978). Bifurcation in Onsager Model of Isotropic-Nematic Transition. Phys Rev A 17, 2067-2072.

30. Cheng, N.S. (2008). Formula for the viscosity of a glycerol-water mixture. Ind Eng Chem Res 47, 3285-3288.

31. Brinker, C.J., and Scherer, G.W. (1990). Sol-Gel Science: The Physics and Chemistry of Sol-Gel Processing, (New York: Academic Press;).

32. Larson, R.G. (1999). The structure and rheology of complex fluids, (New York: Oxford University Press).

33. Coey, J.M.D. (2010). Magnetism and magnetic materials, (Cambridge: Cambridge University Press).

107

CHAPTER V

5

VISCOSITY CHANGE OF MULLITE PRECURSOR DURING

EVAPORATION

As shown in the previous chapter, the alignment of magnetic nanorods in a solidifying film significantly depends on the fluid viscosity. In the composite processing when the solvent evaporates, viscosity changes significantly. Therefore, in order to control the nanorod alignment during solvent evaporation it is crucial to understand the effect of evaporation on viscosity. In this chapter, we will first study the evaporation kinetics of the mullite precursor droplet and then use the magnetic rotational spectroscopy (MRS) to measure the time-dependent viscosity. A correlation between the viscosity and concentration of mullite in the precursor drop was analized in detail and the Eyiring model was employed to explain the observed dependency.

Documento similar