## 5 Comprehensive Analysis of Outcomes of Attached Parameters
A material's ability to transfer heat increases with the consideration of nanoparticles in the base fluid. Molecules collide more frequently due to a change in thermal conductivity, which increases the kinetic energy of the fluid's molecules and the temperature field. Figures 11-13 reveal the consequences of the attached parameters with the mass transportation field. Mass diffusivity is related to the Schmidt number, and due to this fact, the mass transportation becomes lower. The Schmidt number's role is the same for mass transportation as the Prandtl number is for heat transportation. The Schmidt number is the ratio of momentum diffusivity to mass diffusivity. A positive variation in _Sc_ magnifies the concentration of nanofluid, which provides a resistance-free motion to the mass transport and depreciates the concentration field. The Brownian motion parameter also results in a reduction of mass transportation. The temperature of the fluid is magnified by virtue of an amplification in _Nb_, which otherwise diminishes the concentration of fluid molecules and depreciates the concentration field. Note that a positive change in \(A\) encourages the fluid viscosity phenomenon, which amplifies the temperature and diminishes the concentration field phenomenon. Similarly, the unsteadiness parameter gives the same result as _Sc_ and _Nb_. Figure 10: Variations in temperature profiles owing to changes in \(\varepsilon\). Figures 14-19 discuss the impact of various dimensionless parameters on the surface drag coefficient. From the figures, it is crystal clear that a positive change in _We_, _Pr_ diminishes the surface drag coefficient, but surface drag phenomenon escalates as a result of magnifications in _Sc_, \(A\), \(M\) and \(\sigma\). From Figure 14, it is quite evident that a positive variation in the Weissenberg number _We_ depreciates the skin friction phenomenon. The Weissenberg number is directly related with the relaxation time. Relaxation time is the time needed by the fluid in order to regain its original shape. During this time, the fluid is allowed to relax, and its viscosity increases. Paint is an example of the Weissenberg phenomenon. The skin friction coefficient, also called drag friction, is the drag created by the friction of the fluid opposite to the object surface over which the fluid is moving. It is quite established that a positive variation in _We_ amplifies the fluid viscosity, which is responsible for a decrement in the fluid velocity and skin friction phenomenon. Figure 15 provides the statistical analysis of the power law index against the surface drag coefficient. The viscosity of the fluid solely depends on power law index n. The fluid behavior is shear thinning in the case of \(n<1\), Newtonian for \(n=1\) and shear thickening for \(n>1\). It is well established that the viscosity of fluid decreases by virtue of magnification in \(n\). Velocity is directly related with viscosity. The velocity of fluid topples the sheet velocity in the case of amplification n, which magnifies the skin friction phenomenon. Figure 14: Revealing the consequences of _We_ with the related skin friction coefficient. Figure 13: Variations in species concentration profiles owing to changes in \(A\). Figure 16: Revealing the consequences of \(Pr\) with the related skin friction coefficient. Figure 17: Revealing the consequences of \(A\) with the related skin friction coefficient. Figure 6.0 Revealing the consequences of \(n\) with the related skin friction coefficient. Figure 16 displays the impact of the Prandtl number \(Pr\) on the drag coefficient. The Prandtl number is the dimensionless quantity expressing the ratio of momentum diffusivity to the thermal diffusivity. Momentum diffusivity is the dynamic viscosity to fluid density ratio, and thermal diffusivity expresses the ratio of thermal conduction to density and specific heat. Viscosity is inversely related to temperature. A decrement in temperature depreciates thermal diffusivity and moreover strengthens the fluid viscosity and momentum diffusion phenomenon.