Please cite this article in press as: Mosayebidorcheh, S., et al. Analysis of turbulent MHD Couette nanofluid flow and heat transfer using
hybrid DTM–FDM. Particuology (2014), http://dx.doi.org/10.1016/j.partic.2014.07.004
ARTICLE IN PRESS
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PARTIC-726; No. of Pages 8
Particuology xxx (2014) xxx–xxx
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Particuology
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Analysis of turbulent MHD Couette nanofluid flow and heat transfer
using hybrid DTM–FDM
S. Mosayebidorcheh
a,∗
, M. Sheikholeslami
b
, M. Hatami
c
, D.D. Ganji
b
a
Young Researchers and Elite Club, Najafabad Branch, Islamic Azad University, Najafabad, Iran
b
Department of Mechanical Engineering, Babol University of Technology, Babol, Iran
c
Esfarayen University of Technology, Engineering and Technical College, Mechanical Engineering Department, Esfarayen, North Khorasan, Iran
a r t i c l e i n f o
Article history:
Received 8 June 2014
Received in revised form 21 July 2014
Accepted 27 July 2014
Keywords:
Turbulent
Hall effect
Hybrid DTM–FDM
Nanofluid
MHD Couette flow
a b s t r a c t
Unsteady turbulent nanofluid flow and heat transfer in the presence of a magnetic field is studied by
considering the Hall effect. The zero-equation turbulence model is used to simulate turbulent flow. The
modeling results obtained by applying the hybrid differential transformation method–finite difference
method (DTM–FDM) to solve this problem confirm its viability. An analytical procedure is used for various
values of active parameters. Results indicate that the Nusselt number over the lower plate depends linearly
on nanoparticle volume fraction, Hall parameter, Reynolds number, and turbulent Eckert number whereas
it is inversely proportional on the Hartmann number and the turbulent parameter.
© 2014 Chinese Society of Particuology and Institute of Process Engineering, Chinese Academy of
Sciences. Published by Elsevier B.V. All rights reserved.
Introduction
Algebraic turbulence models or zero-equation turbulence mod-
els are models that do not require the solutions of any additional
equations, and are calculated directly from the flow variables. As
a consequence, zero-equation models may not be able to properly
account for history effects on the turbulence, such as convection
and diffusion of turbulent energy. These models are often too
simple for use in general situations, but can be quite useful for
simpler flow geometries or in start-up situations (e.g., the initial
phases of a computation in which a more complicated model may
have difficulties). This method has several advantages such as ease
of implementation, fast calculation times, and good predictions
for simple flows where experimental correlations for the mixing
length exist (Biswas & Eswaran, 2002).
The differential transformation method (DTM) was introduced
by Zhou (1986) to solve some problems analytically. A hybrid
numerical technique that combines the DTM and finite differ-
ence method (FDM) is used in many studies (Gkdo˘ gan, Merdan,
& Yildirim, 2012; Odibat, Bertelle, Aziz-Alaoui, & Duchamp, 2010;
∗
Corresponding author. Tel.: +98 9358855140.
E-mail addresses: sobhanmosayebi@yahoo.com (S. Mosayebidorcheh),
mohsen.sheikholeslami@yahoo.com (M. Sheikholeslami),
m.Hatami2010@gmail.com (M. Hatami), ddg davood@yahoo.com (D.D. Ganji).
Rashidi, Chamkh, & Keimanesh, 2011). It is a suitable and efficient
method for solving the time-dependent problem in heat and mass
transfer subjects. For instance, Peng and Chen (2011) investigated
an annular fin with temperature-dependent thermal conductiv-
ity using this hybrid-DTM; also Chu and Lo (2007) developed the
hybrid differential transformation-finite difference method to ana-
lyze nonlinear transient heat conduction problems. Motivated by
the above-mentioned work, the main objective of our study is to
introduce the hybrid-DTM as a highly accurate and efficient method
for the unsteady magnetohydrodynamic (MHD) Couette fluid flow
between two parallel plates. Outcomes reveal that the hybrid-
DTM as an explicit method can overcome all nonlinearity terms of
the problem without needing linearization. Peng and Chen (2011)
showed that the convective heat transfer plays a dominant role in
the heat dissipation under convection-radiation conditions.
Nanofluids are produced by dispersing the nanometer-scale
solid particles into base liquids of low thermal conductivity
such as water, ethylene glycol, and oils. The term “nanofluid”
was first coined by Choi (1995) to describe this new class of
fluids. The presence of nanoparticles in the fluids noticeably
increases their effective thermal conductivity and consequently
enhances their heat transfer characteristics. Nanofluids as a pas-
sive method for enhancement heat transfer became popular in
the last decade (Domairry & Hatami, 2014; Hatami & Ganji, 2014;
Hatami, Sheikholeslami, & Ganji, 2014a, Hatami, Sheikholeslami,
& Ganji, 2014b; Sheikholeslami & Ganji, 2013, Sheikholeslami &
http://dx.doi.org/10.1016/j.partic.2014.07.004
1674-2001/© 2014 Chinese Society of Particuology and Institute of Process Engineering, Chinese Academy of Sciences. Published by Elsevier B.V. All rights reserved.