Nowadays, nanofluid (colloidal suspension) gains a lot of interest among various scientists and researchers in different countries due to its vast applications as heat transfer fluid [1], transportation [2, 3], bio-fluid [4], micro-heat sinks [5], micro-transformer [6], etc. Many experiments had been conducted to explore the tremendous heat transfer efficiency of nanofluid (metal and nonmetal nanoparticles) at Argonne National Laboratory, Chicago. The Argonne scientist team revealed that silicon carbide nanoparticles in ethylene glycol/ water carry heat away approximately 15 times more than conventional fluid. The development of nanofluids was focused on the basis of working of whole nanofluid system rather than individual properties (size, shape, conductivity, etc.) of the nanoparticles. Thus, the concentration and particle size were key to designing such systems. In 2006, Buongiorno [7] discussed the twocomponent modeling of nanofluid flow based on seven slip mechanism. He concluded that Brownian motion and thermophoresis are mainly responsible for anomalous heat transfer in nanofluids. Later, the extension of the Buongiorno's model was reported in vertical plate problem [8], Cheng-Minkowycz problem [9], linear and nonlinearly stretching sheet problem [10, 11], Hiemenz flow problem [12], Falkner-Skan problem [13], nonequilibrium model [14], double-diffusive problem [15, 16], non-Newtonian problem [17], and others. Recently, Kuznetsov and Nield [18, 19] revised their earlier published with new no-flux boundary conditions. Due to these boundary conditions, the impact of Brownian motion on heat transfer is now insignificant. Thenafter, many researchers tried to implement such boundary conditions in different flow regimes [20-27].