The Blasius boundary-layer flow of a micropolar fluid

Rees, D. Andrew S.; Bassom, Andrew P.

doi:10.1016/0020-7225(95)00058-5

Cited by 147 publications

(101 citation statements)

References 11 publications

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“…The x axis is measured along the stretching surface in the direction of the motion and the y axis is perpendicular to it. Under the boundary layer assumptions and considering the mathematical nanofluid model proposed by Tiwari and Das [8] the basic equations of this problem can be written as (see Rees and Bassom [18]…”

Section: Mathematical Modelmentioning

confidence: 99%

See 1 more Smart Citation

Flow over a permeable stretching sheet in micropolar nanofluids with suction

Fauzi

Ahmad

Pop

2014

AIP Conference Proceedings

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Section: Mathematical Modelmentioning

confidence: 99%

“…Relation (5) was established by Ahmadi [19] and Kline [20] and it has been used by many researchers, for example, Rees and Bassom [18], Rees and Pop [21], and Nazar et al [16]. The thermophysical properties of the nanofluid can be seen from Oztop and Abu-Nada [22].…”

Section: Mathematical Modelmentioning

confidence: 99%

Flow over a permeable stretching sheet in micropolar nanofluids with suction

Fauzi

Ahmad

Pop

2014

AIP Conference Proceedings

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“…The theory of micropolar fluid was first proposed by Eringen [1]. Extensive review of the theory and applications can be found in the review article by Ariman et al [2] and quite recent papers by Rees and Bassom [3], Pop et al [4], Nazar et al [5][6][7][8], and so forth. This clearly shows the fast development of the theory of micropolar fluid.…”

Section: Introductionmentioning

confidence: 99%

Mixed Convection Boundary Layer Flow from a Solid Sphere with Newtonian Heating in a Micropolar Fluid

Salleh

Pop

2010

SRX Physics

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The steady mixed convection boundary layer flow from a solid sphere in a micropolar fluid, generated by Newtonian heating in which the heat transfer from the surface is proportional to the local surface temperature, is considered. The governing boundary layer equations are first transformed into a system of nondimensional equations via the non-dimensional variables, and then into nonsimilar equations before they are solved numerically using an implicit finite-difference scheme known as the Keller-box method. Numerical solutions are obtained for the skin friction coefficient, wall temperature and heat transfer coefficient, as well as the velocity and temperature profiles with several parameters considered, namely the mixed convection parameter, the material or micropolar parameter, and the Prandtl number.

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“…Many authors have assumed that special class of fluids, see Kline and Allen [9], Ahmadi [11], Allen and Kline [12], and Rees and Bassom [13].…”

Section: Solution Methodologymentioning

confidence: 99%