Anuar Ishak

Prof. Anuar Ishak

Universiti Kebangsaan Malaysia
orcid

Research Focus & Metrics

Academic Career Length

21Years (2006-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 June 2019 in International Journal of Heat and Mass Transfer
Verified
Journal Article
Closed access
IWIskandar Waini
Iskandar Waini
Anuar IshakAnuar Ishak
Anuar Ishak
IPIoan Pop
Ioan Pop

1 September 2010 in International Journal of Thermal Sciences
Verified
Journal Article
Closed access
NBNorfifah Bachok
Norfifah Bachok
Anuar IshakAnuar Ishak
Anuar Ishak
IPIoan Pop
Ioan Pop

21 October 2008 in Meccanica
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Journal Article
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PDF file
Anuar IshakAnuar Ishak
Anuar Ishak
RNRoslinda Nazar
Roslinda Nazar
IPIoan Pop
Ioan Pop

1 February 2011 in International Journal of Thermal Sciences
Verified
Journal Article
Closed access
NYNor Azizah Yacob
Nor Azizah Yacob
Anuar IshakAnuar Ishak
Anuar Ishak
IPIoan Pop
Ioan Pop

1 April 2011 in Physica B: Condensed Matter
Verified
Journal Article
Closed access
NBNorfifah Bachok
Norfifah Bachok
Anuar IshakAnuar Ishak
Anuar Ishak
IPIoan Pop
Ioan Pop

24 October 2006 in Meccanica
Verified
Journal Article
Open access
PDF file
Anuar IshakAnuar Ishak
Anuar Ishak
RNR. Nazar
R. Nazar
IPI. Pop
I. Pop
An analysis is made for the steady mixed convection boundary layer flow near the two-dimensional stagnation-point flow of an incompressible viscous fluid over a stretching vertical sheet in its own plane. The stretching velocity and the surface temperature are assumed to vary linearly with the distance from the stagnation-point. Two equal and opposite forces are impulsively applied along the x-axis so that the wall is stretched, keeping the origin fixed in a viscous fluid of constant ambient temperature. The transformed ordinary differential equations are solved numerically for some values of the parameters involved using a very efficient numerical scheme known as the Keller-box method. The features of the flow and heat transfer characteristics are analyzed and discussed in detail. Both cases of assisting and opposing flows are considered. It is observed that, for assisting flow, both the skin friction coefficient and the local Nusselt number increase as the buoyancy parameter increases, while only the local Nusselt number increases but the skin friction coefficient decreases as the Prandtl number increases. For opposing flow, both the skin friction coefficient and the local Nusselt number decrease as the buoyancy parameter increases, but both increase as Pr increases. Comparison with known results is excellent.