Int: J Food Eng; 2012 51 Chin NL, Chan SM, Yusof YA, Chuah TG,

Int: J Food Eng; 2012. 51. Chin NL, Chan SM, Yusof YA, Chuah TG, Talib RA: Modelling of rheological behaviour of pummelo juice concentrates using master-curve. J Food Eng 2009, 93:134–140.CrossRef NVP-HSP990 supplier 52. Larson RG: The Structure and Rheology of Complex Fluids. New York: Oxford University Press; 1999. 53. Timofeeva EV, Routbort JL, Singh D: Particle shape effects on thermophysical properties of alumina nanofluids. J App Phys 2009, 106:014304.CrossRef 54. Abdelhalim MAK, Mady MM, Ghannam MM: Rheological and dielectric

properties of different gold nanoparticle sizes. Lipids Health Dis 2011, 10:208.CrossRef 55. Pham KN, Petekidis G, Vlassopoulos D, Egelhaaf SU, Pusey PN, Poon WCK: Yielding of colloidal glasses. Europhys Lett 2006, 75:624–630.CrossRef 56. Tanaka H, Meunier J, Bonn D: Nonergodic states

of charged colloidal suspensions: repulsive and NU7026 attractive glasses and gels. Phys Rev E Stat Nonlin 2004, 69:031404.CrossRef 57. Cox WP, Merz EH: Correlation of dynamic and steady-flow viscosities. J Polym Sci 1958, 28:619–622.CrossRef 58. Haleem BA, Nott Transmembrane Transporters inhibitor PR: Rheology of particle-loaded semi-dilute polymer solutions. J Rheol 2009, 53:383–400.CrossRef Competing interests The authors declare that they have no competing interests. Authors’ contributions DC performed the nanofluid sample characterization and experimental measurements and participated in the redaction and the critical evaluation of experimental results. MJPG contributed with the selection of the optimal oxyclozanide experimental setting and type of tests to be performed.

CGF participated in the critical evaluation of experimental and theoretical results. MMP analyzed the data and participated in the structuring of the work. LL conceived the study, developed its design, and coordinated the redaction of the manuscript. All authors read and approved the final manuscript.”
“Background It was known that working frequency is moving to the gigahertz band region for applications such as magnetic recording heads, wireless inductor cores, and microwave noise filters [1]. It requires the development of a soft magnetic film with high resonance frequency and high permeability [2, 3]. In order to solve the expanded electromagnetic interference problems, many researchers begin to focus on the enhancement of microwave absorption [4]. Magnetic thin film application is based on the analysis of the dynamic magnetic or magnetization process, which is subjected to an effective magnetic anisotropy field H eff as given by the Landau-Lifshitz-Gilbert (LLG) equation [5] and resonance frequency f r[6] (1) (2) where M s represents saturation magnetization, H eff is the anisotropy effective field, γ is the gyromagnetic factor, and α is the damping constant. From Equations 1 and 2, it can be seen that magnetic anisotropy and saturation magnetization are the two key material parameters which determine the magnetic properties of the magnetic film.

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