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Therefore, higher values of C, i.e., the boundary layer thickness, depict higher adsorption capacities (Table 8).
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Variation of radiation parameter R on the temperature (theta (eta )) and thermal boundary layer thickness is depicted in Figure 11.
It depicts that the velocity field and momentum boundary layer thickness increase by increasing mixed convection parameter as shown in Fig. 4a. Figure 4b illustrates that the solutal concentration profile and its boundary layer thickness are a decreasing function of mixed convection parameter.
It is depicted that the temperature field and the thermal boundary layer thickness increase with the increase in R. Figure 15 displays the effect of Prandtl number on the temperature profile.
The results also show that momentum boundary layer thickness decreases whereas thermal boundary layer thickness increases.
Figures depicted that increasing the suction parameter would cause a decrease in thermal boundary layer thickness and concentration profiles.
It was depicted that the k-Factor promotes with enhancement of viscosity due to growing of boundary layer thickness on the rotor surface.
Thermal boundary layer thickness reduction.
Consequently, the momentum boundary layer thickness reduces.
Therefore finally concentration boundary layer thickness is increases.
The constant I could be attributed to boundary layer thickness.
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