 Nano Idea
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Energy Transfer in Mixed Convection MHD Flow of Nanofluid Containing Different Shapes of Nanoparticles in a Channel Filled with Saturated Porous Medium
 Gul Aaiza^{1},
 Ilyas Khan^{2} and
 Sharidan Shafie^{1}Email author
Received: 20 July 2015
Accepted: 3 November 2015
Published: 23 December 2015
Abstract
Energy transfer in mixed convection unsteady magnetohydrodynamic (MHD) flow of an incompressible nanofluid inside a channel filled with saturated porous medium is investigated. The channel with nonuniform walls temperature is taken in a vertical direction under the influence of a transverse magnetic field. Based on the physical boundary conditions, three different flow situations are discussed. The problem is modelled in terms of partial differential equations with physical boundary conditions. Four different shapes of nanoparticles of equal volume fraction are used in conventional base fluids, ethylene glycol (EG) (C _{ 2 } H _{ 6 } O _{ 2 }) and water (H _{ 2 } O). Solutions for velocity and temperature are obtained discussed graphically in various plots. It is found that viscosity and thermal conductivity are the most prominent parameters responsible for different results of velocity and temperature. Due to higher viscosity and thermal conductivity, C _{ 2 } H _{ 6 } O _{ 2 } is regarded as better convectional base fluid compared to H _{ 2 } O.
Keywords
Introduction
Thermal conductivity plays a vital role in heat transfer enhancement. Conventional heat transfer fluids such as water, ethylene glycol (EG), kerosene oil and lubricant oils have poor thermal conductivities compared to solids. Solids particles on the other hand have higher thermal conductivities compared to conventional heat transfer fluids. Choi [1] in his pioneering work indicated that when a small amount of nanoparticles is added to common base fluids, it increases significantly the thermal conductivity of the base fluids as well as their convective heat transfer rate. This mixtures is known as nanofluids. More exactly, nanofluids are suspensions of nanosize particles in base fluids. Usually nanofluids contain different types of nanoparticles such as oxides, metals and carbides in commonly base fluids like water, EG, propylene glycol and kerosene oil. Some specific applications of nanofluids are found in various electronic equipment, energy supply, power generation, air conditioning and production. Vajjha and Das [2] for the first time used EG (60 %) and water (40 %) mixture as base fluid for the preparation of alumina (Al _{ 2 } O _{ 3 }), copper oxide (CuO) and zinc oxide (ZnO)nanofluids. At the same temperature and concentration, they found that CuO nanofluid posses high thermal conductivity compare to those of Al _{ 2 } O _{ 3 } and ZnO nanofluids. Naik and Sundar [3] took 70 % propylene glycol and 30 % water and prepared CuO nanofluid. As expected, they found that CuO nanofluid has better thermal conductivity and viscosity properties compare to base fluid. Recently, Mansur et al. [4] studied nanofluids for magnetohydrodynamic (MHD) stagnation point flow past a permeable sheet for stretching and shrinking cases. They obtained numerical solutions using bvp4c program in MATLAB and computed results for embedded parameters.
The ability of nanoparticles to enhance the thermal conductivity of base fluids together with numerous applications of nanofluids in industry has attracted the interest of researchers to conduct further studies. Amongst them, several are performing experimental work, some of them are using numerical computations, however very few studies are available on analytic side. Perhaps, it is due to the reason that analytic solutions are not always convenient. Among the various attempts are mention here those made in [5–15].
The quality of nanofluid not only depends on the type of nanoparticles but also their shapes. Researchers usually use nanoparticles of spherical shapes. However, in terms of applications and significance, spherical shaped nanoparticles are limited. Due to this reason nonspherical shaped nanoparticles are choose in this study. More exactly, this study incorporates four different types of nanoparticles namely cylinder, platelet, blade and brick. Furthermore, nanofluids literature reveals that nonspherical shaped nanoparticles carry a number of key desirable properties to be the main focus of current research especially in cancer therapy. Recently, investigation shows that cylindrical shaped nanoparticles are seven times more deadly than traditional spherical shaped nanoparticles in the delivery of drug to breast cancer cells. To the best of author knowledge, analytic studies on different shapes of nanoparticles contained in EG or water as the base fluids is not reported yet. Although, Timofeeva et al. [16] study the problem of Al _{ 2 } O _{ 3 } nanofluids containing different shaped nanoparticles but they conducted this study experimentally together with theoretical modelling. More exactly they investigated various shapes of Al _{ 2 } O _{ 3 } nanoparticles in a base fluid mixture of EG and water of equal volumes. By using Hamilton and Crosser model, they noted enough enhancements in the effective thermal conductivities due to particle shapes. Loganathan et al. [17] considered spherical nanoparticles and analyzed radiation effects on an unsteady natural convection flow of nanofluids past an infinite vertical plate. They concluded that spherical silver (Ag) nanofluids velocity is less than copper (Cu), titanium dioxide (TiO _{ 2 }) and Al _{ 2 } O _{ 3 } spherical nanofluids due to greater viscosity. Recently, Asma et al. [18] obtained exact solutions for free convection flow of nanofluids with ramped wall temperature by taking five different types of spherical shaped nanoparticles.
Heat transfer due to convection arises in many physical situations. Convection is of three types i.e. free convection, forced convection and mixed convection. The buoyancy induced convection is called free convection whereas forced convection causes due to external pressure gradient or object motion. Mixed convection induces only due to simultaneous occurrence of free and forced convection to transfer heat. The most typical and common situations where mixed convection is almost always realized is the flow in the channel due to the process on heating or cooling the channel walls. In such a flow situation, the buoyancy force causes free convection whereas the external pressure gradient or the non homogeneous boundary conditions on the velocity results forced convection. Sebdani et al. [19] studied heat transfer of Al _{ 2 } O _{ 3 } water nanofluid in mixed convection flow inside a square cavity. Fan et al. [20] investigated mixed convection heat transfer in a horizontal channel filled with nanofluids. Tiwari and Das [21] and Sheikhzadeh et al. [22] analyzed laminar mixed convection flow of a nanofluid in twosided liddriven enclosures. Further, magnetic field in nanofluids has its numerous applications such as in the polymer industry and metallurgy where hydromagnetic techniques are being used. Nadeem and Saleem [23] examined the unsteady flow of a rotating MHD nanofluid in a rotating cone in the presence of magnetic field. AlSalem et al. [24] investigated MHD mixed convection flow in a linearly heated cavity. The effects of variable viscosity and variable thermal conductivity on the MHD flow and heat transfer over a nonlinear stretching sheet was investigated by Prasad et al. [25]. The problem of Darcy Forchheimer mixed convection heat and mass transfer in fluidsaturated porous media in the presence of thermophoresis was presented by Rami et al. [26]. Effect of radiation and magnetic field on the mixed convection stagnationpoint flow over a vertical stretching sheet in a porous medium bounded by a stretching vertical plate was presented by Hayat et al. [27]. Few other studies on mixed convection and nanofluids are given in [28–38].
Based on above literature, the present investigation is concerned with the radiative heat transfer in mixed convection MHD flow of a different shapes of Al _{ 2 } O _{ 3 } in EGbased nanofluid in a channel filled with saturated porous medium. The focus in this work is the effect of different parameters on cylinder shape nanofluids. The fluid is assumed to be electrically conducting and the no slip condition is considered at the boundary of the channel. Three different flow situations are discussed. In the first case, both of the bounding walls of the channel are at rest. Fluid motion is originated due to buoyancy force together with external pressure gradient of oscillatory form applied in the flow direction. In the second case, the upper wall of the channel is set into oscillatory motion whereas the third case extends this idea when both of the channel walls are given oscillatory motions. Analytical solutions are obtained for velocity and temperature profile. The results for skin friction and Nusselt number are computed. Graphical results for velocity field and temperature distributions are displayed for various parameters of interest and discussed in details.
Formulation and Solution of the Problem
where u = u(y, t) denotes the fluid velocity in the x– direction, T = T(y, t) is the temperature, ρ _{ nf } is density of nanofluids, μ _{ nf } is the dynamic viscosity of nanofluid, σ is the electrical conductivity of the base fluid, k _{1} > 0 is the permeability of the porous medium (ρβ)_{ nf }, thermal expansion coefficient of nanofluids g, is the acceleration due to gravity (ρc _{ p })_{ nf }, is the heat capacitance of nanofluids, k _{ nf } is the thermal conductivity of nanofluid, q is the radiative heat flux in x– direction. The first term on the right denotes the externa l pressure gradient.
Constants a and b empirical shape factors
Model  Platelet  Blade  Cylinder  Brick 

a  37.1  14.6  13.5  1.9 
b  612.6  123.3  904.4  471.4 
Sphericity Ψ for different shapes nanoparticles
Model  Platelet  Blade  Cylinder  Brick 

Ψ  0.52  0.36  0.62  0.81 
Thermophysical properties of water and nanoparticles
Model  ρ(kgm ^{− 3})  c _{ P }(kg ^{− 1} K ^{− 1})  k(Wm ^{− 1} K ^{− 1})  β × 10^{− 5}(K ^{− 1}) 

H _{ 2 } O  997.1  4179  0.613  21 
C _{ 2 } H _{ 6 } O _{ 2 }  1.115  0.58  0.1490  6.5 
Cu  8933  385  401  1.67 
TiO _{ 2 }  4250  686.2  8.9528  0.9 
Ag  10500  235  429  1.89 
Al _{ 2 } O _{ 3 }  3970  765  40  0.85 
Fe _{ 3 } O _{ 4 }  5180  670  9.7  0.5 
where α is the radiation absorption coefficient.
where α is the mean radiation absorption coefficient.
In order to solve Eqs. (9) and (10), we consider the following three cases.
CaseI: Flow Inside a Channel with Stationary Walls
for velocity and temperature respectively.
Case2: Flow Inside a Channel with Oscillating Upper Plate
where H(t) is the Heaviside step function.
Case3: Flow Inside a Channel with Oscillating Upper and Lower Plates
Nusselt Number and Skinfriction
Graphical Results and Discussion
The influence of different shapes of Al _{2} O _{3} nanoparticles on the velocity of EGbased nanofluids is shown in Fig. 1. It can be seen from this figure that the blade shape Al _{2} O _{3} nanoparticles has the highest velocity followed by brick, platelet and cylinder shapes nanoparticles. The influence of the shapes on the velocity of nanofluids is due to the strong dependence of viscosity on particle shapes for the volume fraction ϕ < 0.1. The present results show that the elongated shape nanoparticles like cylinder and platelet have the highest viscosities as compared to square shape nanoparticles like brick and blade. The obtained results agree well with the experimental results predicted by Timofeeva et al. [16]. A very small deviation is observed in the present study, where the cylinder shape nanoparticles has the highest viscosity, whereas from the experimental results reported by Timofeeva et al. [16] the platelet has the highest viscosity. Timofeeva et al. [16] had compared their results with Hamilton and Crosser model [28] and found that their results are identical with Hamilton and Crosser model [28]. In the present work, we have used Hamilton and Crosser model [28] and found that our analytical results also match with the experimental results of Timofeeva at el. [16].
Figure 2 is plotted to examine the effect of different shapes of Al _{2} O _{3} nanoparticle on the velocity of water nanofluids. It is clearly seen that the cylinder shape Al _{2} O _{3} nanoparticles has the lowest velocity followed by platelet, brick and blade. Thus, according to Hamilton and Crosser model [28], suspension of elongated and thin shape particles (high shape factor n) should have higher thermal conductivities, if the ratio of k _{ nf }/k _{ f } is greater than 100. It is also mentioned by Colla et al. [32] that the thermal conductivity and viscosity increase with the increase of particle concentration due to which velocity decreases. Therefore, the cylinder shape Al _{2} O _{3} nanoparticles has the highest thermal conductivity followed by platelet, brick and blade. Timofeeva et al. [16] described the reason that when the sphericity of nanoparticles is below 0.6, the negative contribution of heat flow resistance at the solid–liquid interface increases much faster than the particle shape contribution. Thus, the overall thermal conductivity of suspension start decreasing below sphericity of 0.6 but it is increasing in case of Hamilton and Crosser model [28] due to the only contribution of particle shape parameter n. Furthermore, flow in this research is single phase, therefore the negative contribution of heat flow resistance is neglected. Timofeeva et al. [16] used the model \( {k}_{nf}/{k}_f=1+\left({c}_k^{shape}+{c}_k^{surface}\right)\;\phi \), for finding the thermal conductivity of nanoparticles. According to this model, \( {c}_k^{shape} \) and \( {c}_k^{surface} \) coefficients reflecting contributions to the effective thermal conductivity due to particle shape (positive effect) and due to surface resistance (negative effect) respectively. Particle shape coefficient \( {c}_k^{shape} \) was calculated by Hamilton and Crosser equation.
A comparison of EGbased nanofluid with waterbased nanofluid is made in Fig. 3. It is found that the velocity of waterbased nanofluid is greater than the velocity of EGbased nanofluid. The viscosity and thermal conductivity of EG and water base nanofluids are also predicted by Hamilton and Crosser model [28] for the same ϕ. This result shows that EG based nanofluid has greater viscosity and thermal conductivity compared to water based nanofluid.
The effect of different nanoparticles on the velocity of nanofluids is presented in Fig. 4. From this figure, it is noted that cylinder shape Al _{2} O _{3} nanofluid has the highest velocity followed by Fe _{3} O _{4}, TiO _{2}, Cu and silver nanofluids. This shows that cylinder shape silver nanofluids has the highest viscosity and thermal conductivity compared to Cu TiO _{2}, iron oxide Fe _{3} O _{4} and Al _{2} O _{3} nanofluids. One can see from this result that cylinder shape silver nanofluid has better quality fluids compared to magnetite cylinder shape Fe _{3} O _{4} nanofluid. This result is supported by Hamilton and Crosser model [28] that the viscosity and thermal conductivity of nanofluid are also affected by nanoparticles φ i.e. the viscosity and thermal conductivity increase with the increase of φ, therefore, velocity decreases with the increase of φ. This figure further shows that viscosity of Al _{2} O _{3} nanofluid at φ is less than 0.1 increases nonlinearly with nanoparticles concentration. This result is found identical with the experimental result reported by Colla et al. [32].
Different φ of cylinder shape Al _{2} O _{3} nanoparticles on the velocity of cylinder shape Al _{2} O _{3} nanofluid is shown in Fig. 5. It is clear from this figure that with the increase of φ velocity of nanofluids is decreased. This is due to the reason that the fluid becomes more viscous with the increase of φ which leads to decrease the velocity of nanofluids. The thermal conductivity of nanofluids also increase with the increase of φ. Experimentally by Colla et al. [32] also reported this behaviour. Results for different values of radiation parameter N are presented in Fig. 6. It is found that velocity increases with the increase of N. This result agrees well with the result obtained by Makinde and Mhone [31]. Physically, this means that with the increase of N, increases the amount of heat energy transfers to the fluid.
The graphical results of velocity for different values of magnetic parameter M are shown in Fig. 7. With increasing M, velocity of the nanofluid decreases. Increasing transverse magnetic field on the electrically conducting fluid gives rise to a resistive type force called Lorentz force which is similar to drag force and upon increasing the value of M, increases the drag force which has the tendency to slow down the fluid velocity. The drag force is maximum near the channel walls and minimum in the middle of the channel. Therefore, velocity is maximum in the middle of the channel and minimum at the boundaries.
The velocity profile for different value of Grashof number Gr is plotted in Fig. 8. It is found that an increase in Gr, leads to an increase in the velocity. Increase of Gr, increases temperature gradient which leads to an increase in the buoyancy force. Therefore, velocity increase occurs with Gr, is due to the enhancement of buoyancy force. Figure 9 is prepared for permeability parameter K. It is found that velocity increases with increasing K due to less friction force. More exactly, increasing K reduce fluid friction with channel wall and velocity enhances.
In the second case, Figs. 10, 11, 12, 13, 14, 15, 16, and 17 are plotted for the flow situation when the upper wall is oscillating and the lower wall is at rest. For the last case, when both boundaries are oscillating, Figs. 18, 19, 20, 22, 23, 24, and 25 are plotted. From all these graphs (Figs. 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 23, 24, and 25), we found that they are qualitatively similar but different quantitatively to Figs. 1, 2, 3, 4, 5, 6, 7,8, and 9.
The effect of different particle shapes on the temperature of the nanofluid is shown in Figs. 26 and 27. The temperature in the present work is different for different shapes due to different viscosity and thermal conductivity of different shapes of nanoparticles. It should be noted that the effect of thermal conductivity increases with the increase of temperature but the viscosity decreases with the increase of temperature. It is clear that elongated shape of nanoparticles like cylinder and platelet have minimum temperature because of the greater viscosity and thermal conductivity whereas blade has the highest temperature due to least viscosity and thermal conductivity. The brick shape is lowest in temperature range, although, it has low viscosity. This is due to the shear thinning behavior with temperature. Further, cylinder shape also show shear thinning behavior but the effect is less prominent here. All the other shapes like platelet and blade show Newtonian behavior and independence of viscosity on shear rate. This shear thinning behavior is also studied experimentally by Timofeeva et al. [16].
Figure 28 shows a comparison of water and EGbased nanofluids. It is evaluated that both are temperature dependent and the variation is observed at the same rate for both fluids. This means that the effect of temperature on the thermal conductivity and viscosity of different based nanofluids occur at the same rate. Figure 29 is plotted in order to see the effect of φ on the temperature of the EGbased nanofluid. It is observed that with the increase of φ temperature of the fluid increases due to the shear thinning behavior. The viscosity of cylinder shape nanoparticles show shear thinning behavior at the highest concentration. This was also experimentally shown by Timofeeva et al. [16]. The graphical results of temperature for different values of radiation parameter N are shown in Fig. 30. It is clear from this figure that temperature of the cylinder shape nanoparticles in EGbased nanofluid get more sinusoidal with the increase of N. The increasing N means cooler or dense fluid or decrease the effect of energy transport to the fluid. The cylinder shape nanofluid has temperature dependent viscosity due to shear thinning behavior.
Conclusions

The velocity of nanofluid decrease with the increase of volume fraction of nanoparticles due to increase of viscosity and thermal conductivity.

Velocity of EGbased nanofluid is concluded lower than waterbased nanofluid because the viscosity of base fluid effect the Brownian motion of the nanoparticles.

Elongated particles like cylinder and platelet shapes have lower velocity as compared to blade and brick shapes of nanoparticles due to higher viscosity.

The velocity of the nanofluid decrease with the increase of magnetic parameter due to increase of the drag force which has the tendency to slow down the motion of the fluid.

The velocity of the nanofluid also increase with the increase of thermal Grashof number. Increasing of thermal Grashof number, temperature gradient increases which leads to increase the buoyancy force.
Declarations
Acknowledgements
The authors are grateful to the reviewers for their excellent comments to improve the quality of the present article. The authors would also like to acknowledge the Research Management CenterUTM for the financial support through vote numbers 4 F109 and 03 J62 for this research.
Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
Authors’ Affiliations
References
 Choi SUS (1995) Enhancing thermal conductivity of fluids with nanoparticle, in: D.A. Siginer, H.P. Wang (Eds.), Developments and Applications of NonNewtonian Flows. ASME FED 66:99–105Google Scholar
 Vajjha RS, Das DK (2009) Experimental determination of thermal conductivity of three nanofluids and development of new correlations. Int J Heat Mass Transf 52:4675–4682View ArticleGoogle Scholar
 Naik MT, Sundar LS (2011) Investigation into thermophysical properties of glycol based CuO nanofluid for heat transfer applications. World Acad Science Engineer Technology 59:440–446Google Scholar
 Mansur S, Ishak A, Pop I (2015) The magnetohydrodynamic stagnation point flow of a nanofluid over a stretching/shrinking sheet with suction. PLoS One 10(3):e0117733View ArticleGoogle Scholar
 Ellahi R, Hassan M, Zeeshan A (2015) Shape effects of nanosize particles in CuH2O nanofluid on entropy generation. Int J Heat Mass Transf 81:449–456View ArticleGoogle Scholar
 Sheikholeslami M, Ganji DD, Javed MY (2015) R. Ellahi cEffect of thermal radiation on magnetohydrodynamics nanofluid flow and heat transfer by means of two phase model. J Magn Magn Mater 374:36–43View ArticleGoogle Scholar
 Rashidi S, Dehghan M, Ellahi R, Riaz M, JamalAbad MT (2015) Study of stream wise transverse magnetic fluid flow with heat transfer around an obstacle embedded in a porous medium. J Magn Magn Mater 378:128–137View ArticleGoogle Scholar
 Noreen SA, Raza M, Ellahi R (2014) Influence of heat generation and heat flux in peristalsis with interaction of nanoparticles. The European Physical Journal Plus 129:185View ArticleGoogle Scholar
 Ellahi R, Hassan M, Soleimani S (2014) A study of natural convection heat transfer in a nanofluid filled enclosure with elliptic inner cylinder. International Journal for Numerical Methods for Heat and Fluid Flow 24(8):1906–1927View ArticleGoogle Scholar
 Sheikholeslami M, Ellahi R, Ashorynejad HR, Domairry G, Hayat T (2014) Effects of heat transfer in flow of nanofluids over a permeable stretching wall in a porous medium. Computational and Theoretical Nanoscience 11(2):486–496View ArticleGoogle Scholar
 SheikholeslamI M, Bandpy MG, Ellahi R, Zeeshan A (2014) Simulation of CuOwater nanofluid flow and convective heat transfer considering Lorentz forces. J Magn Magn Mater 369:69–80View ArticleGoogle Scholar
 Noreen SA, Rahman SU, Ellahi R, Nadeem S (2014) Nano fluid flow in tapering stenosed arteries with permeable walls. Int J Therm Sci 85:54–61View ArticleGoogle Scholar
 Ellahi R (2013) The effects of MHD and temperature dependent viscosity on the flow of nonNewtonian nanofluid in a pipe: Analytical solutions. Applied Mathematical Modeling 37:1451–1467View ArticleGoogle Scholar
 Ellahi R, Raza M, Vafai K (2012) Series solutions of nonNewtonian nanofluids with Reynolds' model and Vogel's model by means of the homotopy analysis method. Math Comput Model 55:1876–1891View ArticleGoogle Scholar
 Wang XB, Zhou PL, Peng FX (2003) A fractal model for predicting the effective thermal conductivity of liquid with suspension of nanoparticles. Internation Journal of Heat and Mass Transfer 46(14):2665–2672View ArticleGoogle Scholar
 Timofeeva EV, Jules RL, Dileep S (2009) Particle shape effect on thermophysical properties of alumina nanofluids. J Appl Phys 106:014304View ArticleGoogle Scholar
 Loganathan P, Chand PN, Ganesan P (2013) Radiation effects on an unsteady natural convection flow of a nanofluids past an infinite vertical plate. NANO 08:1350001. doi:10.1142/S179329201350001X [10 pages]View ArticleGoogle Scholar
 Asma K, Khan I, Sharidan S (2015) Exact solutions for free convection flow of nanofluids with ramped wall temperatur. The European Physical Journal Plus 130:57–71View ArticleGoogle Scholar
 Sebdani S, Mahmoodi M, Hashemi S (2012) Effect of nanofluid variable properties on mixed convection in a square cavity. Int J Therm Sci 52:112–126View ArticleGoogle Scholar
 Fan T, XU H, Pop I (2013) Mixed convection heat transfer in horizontal channel filled with nanofluids. International Journal of springer plus 34:339–350Google Scholar
 Tiwari RK, Das MK (2007) Heat transfer augmentation in a twosided liddriven differentially heated square cavity utilizing nanofluids. Int J Heat Mass Transf 50:9–10View ArticleGoogle Scholar
 Sheikhzadeh GA, Hajialigol N, Qomi ME, Fattahi A (2012) Laminar mixed convection of Cuwater nanofluid in two sided liddriven enclosures. Journal of Nanostructures 1:44–53Google Scholar
 Nadeem S, Saleem S (2014) Unsteady mixed convection flow of nanofluid on a rotating cone with magnetic field. Apply Nanoscience 4:405–414View ArticleGoogle Scholar
 AlSalem K, Oztop HF, Pop I, Varol Y (2012) Effect of moving lid direction on MHD mixed convection in a linearly heated cavity. Int J Heat Mass Transf 55:1103–1112View ArticleGoogle Scholar
 Prasad KV, Vajravelu K, Datti PS (2010) The effect of variable fluid properties on the MHD flow and heat transfer over a nonlinear stretching sheet. International Journal of Thermal Science 49:603–610View ArticleGoogle Scholar
 Rami JY, Fawzi A, AbuAlRub F (2011) DarcyForchheimer mixed convection heat and mass transfer in fluid saturated porous media. International Journal of Numerical Methods for Heat & Fluid Flow 11:600–618Google Scholar
 Hayat T, Abbas Z, Pop I, Asghar S (2010) Effect of radiation and magnetic field on the mixed convection stagnationpoint flow over a vertical stretching sheet in a porous medium. Int J Heat Mass Transf 53:466–474View ArticleGoogle Scholar
 Hamilton RL, Crosser OK (1962) Thermal conductivity of heterogeneous twocomponent systems. Journal of Industrial & Engineering Chemistry Fundamentals 1:187–191View ArticleGoogle Scholar
 Turkyilmazoglu M (2014) Unsteady convection flow of some nanofluids past a moving vertical flat plate with heat transfer. J Heat Transf 136:031704–031711View ArticleGoogle Scholar
 Zeehan A, Ellahi R, Hassan M (2014) Magnetohydrodynamic flow of water/ethylene glycol based nanofluids with natural convection through porous medium. European Physical Journal Plus 129:261View ArticleGoogle Scholar
 Makinde OD, Mhone PY (2005) Heat transfer to MHD oscillatory flow in a channel filled with porous medium. Romanian Journal of Physics 50:931–938Google Scholar
 Colla L, Fedele L, Scattolini M, Bobbo S (2012) Waterbased Fe2O3 nanouid characterization: thermal conductivity and viscosity measurements and correlation. Advances in Mechanical Engineering Article ID 674947:8Google Scholar
 Noreen AS, Raza M, Ellahi R (2015) Influence of induced magnetic field and heat flux with the suspension of carbon nanotubes for the peristaltic flow in a permeable channel. J Magn Magn Mater 381:405–415View ArticleGoogle Scholar
 Ellahi R, Aziz S, Zeeshan A (2013) Non Newtonian nanofluids flow through a porous medium between two coaxial cylinders with heat transfer and variable viscosity. Journal of Porous Media 16(3):205–216View ArticleGoogle Scholar
 Noreen AS, Raza M, Ellahi R (2014) Interaction of nano particles for the peristaltic flow in an asymmetric channel with the induced magnetic field. The European Physical Journal  Plus 129:155–167View ArticleGoogle Scholar
 Sheikholeslami M, Ellahi R (2015) Three dimensional mesoscopic simulation of magnetic field effect on natural convection of nanofluid. Int J Heat Mass Transf 89:799–808View ArticleGoogle Scholar
 Ellahi R, Hassan M, Zeeshan A (2015) Study on magnetohydrodynamic nanofluid by means of single and multiwalled carbon nanotubes suspended in a salt water solution. IEEE Trans Nanotechnol 14(4):726–734View ArticleGoogle Scholar
 Sheikholeslami M, Ellahi R (2015) Simulation of ferrofluid flow for magnetic drug targeting using Lattice Boltzmann method. Journal of Zeitschrift Fur Naturforschung A, Verlag der Zeitschrift für Naturforschung 70:115–124Google Scholar