**4. Tables' Discussion**

This section is devoted to comparing the results of this study to the work published and the computation of various quantities of engineering interest with the changing values of the associated parameters. The comparison is carried out in Tables 1–3. The quantities of engineering interest are computed in Tables 4 and 5. The comparison is made with the research work already carried out in ref. [75] as in the following:

The comparison of the skin friction values with varying and *We* is shown in Table 1. The *Rd*, *Sr*, *Du*, *M*, and *Sc* values are taken as 0. We see complete agreement between the results of our work and the already published work.


**Table 1.** Computation of *Cf x* for changing and *We*, for *Rd* = *Sr* = *M* = *Du* = *Sc* = 0.

Table 2 shows the comparison of Nusselt number (*Nux*) for the varying *We, n,* , and *Pr*, whereas *Rd*, *Sr*, *Du*, *M*, and *Sc* are taken as 0. The value of *χ*<sup>1</sup> is taken as 0.2. Again both results are in tremendous agreement.


**Table 2.** Computation of *Nux*, when *Rd* = *Sr* = *M* = *Sc* = *Du* = 0.

Table 3 compares the present and published results for *Shx* (local Sherwood number) for changing *Sr*. We used *Du* = *We* = 0. The values of the parameters *n*, *Rd*, *Pr*, and *M* are kept fixed in computing the values of *Shx*. The comparison proves that both computations are in agreement with each other.

**Table 3.** Computation of *Shx*, for *Du* = *We* = 0.


The computation of *Cf x* and *Cf z* with the changing values of *M*, *m*, *χ*1, and *We* for suction case is tabulated in Table 4. It is found that *Cf x* first reduces and then increases with rising magnetic parameter (*M*). The skin friction *Cf x* drops with the augmenting values of *m*, *χ*<sup>1</sup> and *We*. The other skin friction component *Cf z* augments (drops) with the rising values of *M*, *χ*<sup>1</sup> and *We* (*m*).


**Table 4.** Computation of *Cf x* and *Cf z* in the suction case.

The variation of *Nux* and *Shx* with the augmenting *M*, *n*, *Sr*, *Du*, *Rd*, and *χ*<sup>1</sup> in the blowing case is shown in Table 5. It is clear that both *Nux* and *Shx* drop and then enhance with enhancing *M*. The Nusselt number first increases and then decreases, whereas the Sherwood number enhances with the higher *n*. Furthermore the Nusselt number enhances with the augmenting values of all the remaining parameters, that is *Sr*, *Du*, *Rd* and *χ*1. The Sherwood number rises (declines) with the increasing values of *Du* and *Rd* (*Sr* and *χ*1).


**Table 5.** *Nux*, and *Shx* in the case of blowing.
