Magneto
convection of rotating nanofluids in porous medium:
metals and semiconductors as nanoparticles
Jyoti Ahuja1, Urvashi Gupta2*
1Energy Research Centre, Panjab University, Chandigarh-160014, India
2Dr. S.S. Bhatnagar University Institute of Chemical Engineering
& Technology, Panjab University,
Chandigarh-160014, India
*Corresponding Author E-mail: dr_urvashi_gupta@yahoo.com,
urvashi@pu.ac.in
ABSTRACT:
Present paper investigates the onset of thermal convection of a porous nanofluid layer under the combined influence of rotation
and magnetic field using Darcy-Brinkman model which is the modification of the
Darcy model where in viscous shear effects and change in viscosity are
accounted in momentum equation.In the present
model, due to the presence of rotation Coriolis force
term and due to the presence of magnetic field Lorentz’s force term get
introduced in the conservation equations of momentum coupled with the Maxwell’s
equations. To investigate the combined effect of these forces on the thermal
convection of nanofluid layer normal mode
technique and Galerkin type weighted residual method
is applied. A comparative analysis of the thermal instability of metallic (Cu,
Ag) and semiconducting (TiO2, SiO2) nanofluids
is examined. It is observed that metals are more stable as compared
to semiconductors. Further, it is found that silver nanoparticles
stabilize the water based fluid more as compared to copper nanoparticles
and in semiconductors TiO2 nanoparticles
enhance the stability of the system more as compared to SiO2 nanoparticles. Stability of the system enhances with the
rise in Chandrasekhar number and Taylor number whereas it falls with the rise
in porosity. An additional parameter i.e. Darcy number is introduced due to the
consideration of Darcy Brinkman model which has a stabilizing effect on the nanofluid layer system.
KEYWORDS: Nanofluid, Brownian
motion, Thermophoresis, Darcy number, Chandrasekhar
number, Taylor number.
1. INTRODUCTION:
The concept of nanofluids has improvised the
heat transfer mechanism by replacing the suspension of micrometer sized
particles with nanometer sized particles in conventional fluids. These
nanometer sized particles are called as nanoparticles
which may be metals, metal oxides, carbides, nitrides and semiconductors. The
host liquids may be water, ethylene glycol and propylene glycol etc. The
magnificent idea of introducing nanofluids first came
into the mind of Choi [1] who claimed the enhanced
heat transfer with the addition of nanoparticles.
However this enhancement is very small with the low nanoparticle concentration
(Kim et al. [2]; Putnam et al., [3]; Witharana et al. [4].) All these reports motivated Buongiorno [5] to develop a system of conservation
equations for nanofluids with-in the effect of
Brownian motion and thermophoresis. He
concluded that effect of these forces result in decrease of viscosity of nanofluid which leads to the heat transfer enhancement. The
benchmarking exercise on the problem of thermal convection for nanofluids has been done by Kim et al. [6]. Tzou [7] studied the problem analytically and used eigen function expansion method to solve the conservation
equations given by Buongiorno and found that critical
Rayleigh number is reduced with the addition of nanoparticles.
By using single term Galerkin approximation Nield and Kuznetsov [8] found the
expression for thermal Rayleigh number and the condition of overstability
in porous medium. After concluding the results
of Darcy model Nield and Kuznetsov
[9] have taken up Darcy-Brinkman model for a nanofluid
layer in porous medium. Further, Bhadauria et al. [10] and
Yadav et al. [11] made an extension of the thermal
instability problem by introducing Coriolis force
term (rotation) in momentum equations for both porous/non-porous mediums and
concluded that addition of Coriolis force term in
momentum equation made the overall system more stable. Gupta et al. [12,13]
studied the effect of magnetic field and Hall currents, respectively, on a nanofluid layer for both free boundaries and have shown
that the critical wave number and the associated Rayleigh number undergo a
significant increase with the increase in Chandrasekhar number and decrease
with the increase in Hall parameter.
Considering the conflicting
tendencies of magnetic field and rotation while acting
simultaneously, we have examined the combined influence of rotation and
magnetic field on a nanofluid layer system. In
addition to the body and buoyancy forces; Coriolis
force term (with the inclusion of rotation) and Lorentz force term (with the
inclusion of magnetic field) are introduced. With the introduction of magnetic field
and rotation in the system and with the use of Darcy –Brinkman model,
Chandrasekhar number, Taylor number and Darcy number are introduced. Rotation and magnetic field usually have the effect of
inhibiting the onset of thermal instability while acting separately.
2. Governing equations in porous medium:
Here the system is comprised by taking a horizontal layer of nanofluid in porous medium which is heated underside. Porous nanofluid layer of porosity ε is bounded by two free
boundaries in x-y plane and z-axis is directed vertically upward. The nanofluid layer has attained the temperature at lower and upper boundaries respectively
while heating from the bottom. Nanoparticles are
distributed in such a way that concentration of nanoparticles
isat lower and upper boundaries respectively.
3. Numerical results and discussion:
Let us interpret the impact
of magnetic field, permeability and other nanofluid
parameters on the stability of the system. Stability of the system w.r.t. nanofluid parameters is
examined by analyzing the behavior of thermal Rayleigh number with the
variation in respective parameter. Numerical calculations are accomplished by
using Eq. (18) for stationary mode of heat transfer and Eq. (25) for
oscillatory mode of heat transfer respectively. Graphical interpretation is
carried out for metallic nanofluids (Cu, Ag) and
semiconductors (TiO2 and SiO2) with the help of Mathematica
software.
5.1. Metallic nanofluids:
Ultrafine metallic nanoparticles dispersed in
base fluids are known as metallic nanofluids. Thermal
conductivity of nanofluids gets increased by using nanoparticles of metallic substances due to their high
thermal conductivity. In the present paper, nanoparticles
of metals (Cu and Ag) are dispersed in the base fluid water for analyzing the
stability of metallic nanofluids. The physical properties of nanofluids
vary with the variation in shape, size and volumetric fraction of nanoparticles as shown by Yang et al. [15]. The thermophysical properties of the nanofluids,
considered in this study, are supposed to be constant except for the density
variation, which is determined based on the Boussinesq
approximation. The values of nanofluid parameters at (concentration of nanoparticles)
are for Cu-water nanofluid and for Ag-water nanofluid.
5.2. Semiconductors:
An electrical conductivity of a
semiconductor materials lies between the conductivity of a conductor (like
copper), and an insulator (like glass). The physical properties of
semiconductor materials are based on the quantum physics which explains the
movement of electrons and holes in a crystal lattice. The unique arrangement of
the crystal lattice makes silicon and titanium the most commonly used elements
in the preparation of semiconducting materials. The values of nanofluid parameters at (concentration of nanoparticles)
are for TiO2-water
nanofluid and for SiO2-water
nanofluid.
5.3. Comparative analysis
of thermal instability of metallic nanoparticles with
semiconductors:
After fixing the values of other parameters (like rotation and magnetic
field), a comparative study is carried out for different nanofluids
(metallic/semiconducting) by taking the variation in thermal Rayleigh number
with wave number.
For 0.1 % difference in volume fraction of nanoparticles,
the parametric values of different nanofluids are
calculated using the physical properties. In Fig. 2, thermal Rayleigh number Ra
is plotted with the wave number
Fig.2.
Comparison of metallic nanofluids and semiconductors
under the simultaneous influence of rotation and magnetic field
for different nanofluids under consideration.
It is observed that Ag-water nanofluid exhibits
highest stability as its curve holds higher values of among all other nanofluids whereas curve of SiO2-water nanofluid
lies at the bottom representing least stability. It is noticed that density of
different nanofluids follow the ordering as
Ag>Cu>TiO2>SiO2 which is the same as for the stabilizing influence of nanofluids in the presence of rotation and magnetic field.
Thus we may say that nanoparticles having high values
of density exhibit more stability.
5.4. Impact of
different nanofluid parameters:
Figures 3-10 show the impact
of different nanofluid parameters on the thermal
instability of the system under the simultaneous influence of rotation and
magnetic field. In order to examine the behavior of a particular nanofluid parameter on the thermal instability of the nanofluid, variation in that particular parameter is done
by fixing the other parameters as .
Figures 3-4 are plot of with the variation in Taylor number for the nanofluids with nanoparticles as
metals and semiconductors respectively. It is noticed from these graphs that
rise in the value of rotation parameter, the values of thermal Rayleigh number
get incremented for both types of convection; which establishes the stabilizing
effect of rotation. Also, in case of stationary convection; the curves showing
the effect of Taylor number for Ag–water nanofluid
lie above the curves for Cu-water nanofluid which
means that Ag-water nanofluid exhibits higher
stability as compared to Cu-water nanofluid. On the
other hand, if the case of semiconductors is discussed (Fig. 4), it is found
that TiO2-nanoparticles enhance the stability of nanofluid
more as compared to SiO2-nanoparticles with the increase in Taylor
number. While in the case of oscillatory motion, influence of Taylor number on
the thermal instability of different nanofluids
(considered here) is comparatively negligible. In oscillatory mode of
convection, values of thermal Rayleigh number for all the types of nanofluids approximately lie on the same curve for the same
value of Taylor number. It is also interpreted from the figures that metals
inhibit the onset of convection as compared to semiconductors under the
combined influence of magnetic field and rotation.
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Fig. 3. Impact of Taylor number on the thermal instability of Cu-water and Ag-water nanofluid. |
Fig.4. Impact of Taylor number on the thermal instability of TiO2-water and SiO2-water nanofluid. |
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Fig.5. Impact of Chandrasekhar number on the thermal instability of Cu-water and Ag-water nanofluid. |
Fig.6. Impact of Chandrasekhar number on the thermal instability of TiO2-water and SiO2-water nanofluid. |
Figures 5-6 signify the
impact of applied magnetic field on the thermal instability of nanofluids with nanoparticles as
metals and semiconductors respectively, for stationary as well as oscillatory
convections. It can be seen from the figures that stabilizing effect
increases as the magnitude of applied magnetic field gets increasesed.
Thus the vertical magnetic field enhances the stability of the system for both
types of convection. Also, by increasing the magnitude of magnetic field,
Ag-water and TiO2-water nanofluids
exhibits higher stability than Cu-water and SiO2-water nanofluids respectively. Further, these graphical
representations show that the heat transfer takes place through oscillatory
convection instead of stationary convection.
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Fig.7. Impact of porosity on the thermal instability of Cu-water and Ag-water nanofluid |
Fig.8. Impact of porosity on the thermal instability of TiO2-water and SiO2-water nanofluid. |
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Fig.9. Impact of Darcy number on the thermal instability of Cu-water and Ag-water nanofluid. |
Fig.10. Impact of Darcy number on the thermal instability of TiO2-water and SiO2-water nanofluid. |
In continuation to observe the impact of other parameters, now the
effect of Darcy number and porosity is interpreted in the Figs. 7-10 where it
is discovered that Darcy number enhances the stability of the system while the
porosity does the reverse by reducing the stability of the system. By
increasing the Darcy number and porosity of the medium, Ag-water and TiO2-water
nanofluids exhibits higher stability than Cu-water
and SiO2-water nanofluids respectively.
6. CONCLUSIONS:
In the present paper, magneto-convection of rotating nanofluid
layer in porous medium using Darcy-Brinkman model is investigated for both free
boundaries. The effects of various nanofluid
parameters on the stability of the basic flow are analysed with different types
of nanoparticles-metallic (copper (Cu) and silver
(Ag)) and semiconducting (Titanium dioxide (TiO2) and Silica (SiO2))
with water as the base fluid. The instability sets in through the mode of oscillatory
motions instead of stationary convection for the present configuration of nanoparticles. The existence of oscillatory motions in the
system is due to the occurrence of two
buoyancy forces occurring in the opposite directions i.e. density variation
(due to heating from the bottom) and density of nanoparticles
(at the bottom). Both the external forces; Lorentz force & Coriolis force enhance the stability of the system for both
types of convection: stationary as well as oscillatory motions while porosity
of the medium destabilizes the system. Thus magnetic field and rotation
postpone the onset of convection while porosity advances the same. With the
increase of the distribution of nanoparticles at the
lower boundary; thermal Rayleigh number increases i.e. stability of the system
enhances and the impact of Darcy number is to contribute towards the stability
of the system. Based upon the comparative study of thermal instability carried
out by taking metallic and semiconducting nanofluids
it is established that metallic nanofluids are more
stable than semiconducting nanofluids in the presence
of rotation and magnetic field. Also, Ag-water nanofluid
exhibit higher stability than Cu-water nanofluid in
metals and in semiconductors TiO2-water nanofluid
exhibit higher stability than SiO2-water nanofluid
under the simultaneous influence of magnetic field and rotation.
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ACKNOWLEDGEMENT:
One of the authors Prof. Urvashi Gupta thanks to Council of Scientific and
Industrial Research, New Delhi-110012, India for their financial assistance in
the form of Research and Development Project [Ref. No: 25(0247)/15/EMR-II].
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Received on 22.11.2016 Modified on 29.11.2016 Accepted on 04.12.2016 ©A&V Publications All right reserved DOI: 10.5958/2349-2988.2017.00022.5 Research J. Science and Tech. 2017; 9(1):135-142.
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