﻿Dufour Effects on Unsteady Hydromagnetic Radiative Fluid Flow past a Vertical Plate through Porous Medium

Open Journal of Fluid Dynamics
Vol.2 No.4(2012), Article ID:25721,13 pages DOI:10.4236/ojfd.2012.24017

Dufour Effects on Unsteady Hydromagnetic Radiative Fluid Flow past a Vertical Plate through Porous Medium

Jagdish Prakash1*, Avula Golla Vijaya Kumar2, Desu Bhanumathi3, Sibyala Vijaya Kumar Varma3

1Department of Mathematics, University of Botswana, Gaborone, Botswana

2Department of Mathematics, Sree Vidyanikethan Engineering College (Autonomous), Tirupati, India

3Department of Mathematics, S.V. University, Tirupati, India

Email: *prakashj@mopipi.ub.bw, agvijaykumar1729@gmail.com, svijayakumarvarma@yahoo.co.in

Received July 23, 2012; revised September 1, 2012; accepted September 9, 2012

Keywords: MHD; Heat and Mass Transfer; Diffusion-Thermo (Dufour Number); Vertical Plate; Porous Medium

ABSTRACT

The objective of the present study is to investigate diffusion-thermo (Dufour effect) and radiation effects on unsteady MHD free convection flow past an impulsively started infinite vertical plate with variable temperature and uniform mass diffusion in the presence of transverse applied magnetic field through porous medium. At time t > 0, the plate is given an impulsive motion with constant velocity in the vertical upward direction against to the gravitational field. At the same time the plate temperature is raised linearly with time t and the level of concentration near the plate is raised to. A magnetic field of uniform strength is applied normal to the direction to the flow. The dimensionless governing equations are solved in closed form by Laplace-transform technique. The effect of flow parameters on velocity, temperature, concentration, the rate of heat transfer and the rate of mass transfer are shown through graphs.

1. Introduction

In nature, there exist flows which are caused not only by the temperature differences but also the concentration differences. These mass transfer differences do affect the rate of heat transfer. In industries, many transport processes exist in which heat and mass transfer takes place simultaneously as a result of combined buoyancy effect in the presence of thermal radiation. Hence, radiative heat and mass transfer play an important role in manufacturing industries for the design of fins, steel rolling, nuclear power plants, gas turbines and various propulsion device for aircraft, missiles, satellites, combustion and furnace design, materials processing, energy utilization, temperature measurements, remote sensing for astronomy and space exploration, food processing and cryogenic engineering, as well as numerous agricultural, health and military applications. If the temperature of surrounding fluid is rather high, radiation effects play an important role and this situation does exist in space technology. In such cases, one has to take into account the combined effect of thermal radiation and mass diffusion.

Boundary layer flow on moving horizontal surfaces was studied by Sakiadis [1]. The effects of transversely applied magnetic field on the flow of an electrically conducting fluid past an impulsively started isothermal vertical plate were studied by Soundalgekar et al. [2]. MHD effects on impulsively started vertical infinite plate with variable temperature in the presence of transverse applied magnetic field were studied by Soundalgekar et al. [3]. The dimensionless governing equations were solved using Laplace transform technique. Kumari and Nath [4] studied the development of the asymmetric flow of a viscous electrically conducting fluid in the forward stagnation point of a two-dimensional body and over a stretching surface with an applied magnetic field. The governing equations were solved using Laplace transform technique.

England and Emery [5] studied the thermal radiation effects of an optically thin gray gas bounded by a stationary vertical plate. Soundalgekar and Takhar [6] considered the radiation free convection flow of an optically thin gray gas past a semi-infinite vertical plate. Radiation effects on mixed convection along isothermal vertical plate were studied by Hossain and Takhar [7]. In all above studies, the stationary vertical plate is considered. Raptis and Perdikis [8] studied the effects of thermal radiation and free convection flow past a moving vertical plate. The governing equations were solved analytically. Das et al. [9] analyzed radiation effects on flow past an impulsively started infinite isothermal vertical plate. The governing equations were solved by the Laplace transform technique. Muthucumaraswamy et al. [10] and Rajesh and Varma [11] studied radiation and mass transfer effects on exponentially accelerated isothermal vertical plate. Recently, Kumar and Varma [12] studied thermal radiation and mass transfer effects on MHD flow past an impulsively started exponentially accelerated vertical plate with variable temperature and mass diffusion.

Free convection flows that occurs in nature and in engineering practice is very large and has been extensively considered by many authors. When heat and mass transfer occurs simultaneously between the fluxes the driving potentials are more intricate in nature. An energy flux is generated not only by temperature gradients but by composition gradients as well. Temperature gradients can also create mass fluxes and this is the Soret or Thermal-diffusion effect. Generally, the thermal-diffusion and diffusion-thermo effects of smaller order magnitude than the effects prescribed by Fourier’s or Fick’s laws and are often neglected in heat and mass transfer processes. Due to the importance of thermal-diffusion and diffusionthermo effects for the fluids with very light molecular weight as well as medium molecular weight many investtigators have studied and reported results for these flows and the contributors such as Eckert and Drake [13], Dursunkaya and Worek [14], Anghel et al. [15], Postenlnicu [16] are worth mentioning. Alam and Rahman [17] studied the Dufour and soret effects on steady MHD free convective heat and mass transfer flow past a vertical porous plate embedded in a porous medium. Alam et al. [18] investigated the Dufour and Soret effects on unsteady free convection and mass transfer flow past an impulsively started infinite vertical plate embedded in a porous medium under the influence of transverse magnetic field.

In this paper, it is proposed to study diffusion-thermo and radiation effects on MHD free convection flow past an impulsively started infinite vertical plate with variable temperature through porous medium in the presence of transverse applied magnetic field. The dimensionless governing equations are solved using Laplace transform technique. And the solutions are expressed in terms of exponential and complementary error functions.

2. Mathematical Formulation

Diffusion-thermo and radiation effects on unsteady MHD free convection of flow of a viscous incompressible, electrically, conducting, radiating fluid past an impulsively started infinite vertical plate with variable temperature and uniform mass diffusion in the presence of transverse applied magnetic field through porous medium have been studied. The -axis is taken along the plate in vertical upward direction and -axis is taken normal to it in the direction of applied transverse magnetic field. Initially, it is assumed that the plate and surrounding fluid are at the same temperature and concentration in stationary condition for all the points in entire flow region. At time, the plate is given an impulsive motion with constant velocity. At the same time, the plate temperature is raised linearly with time t and the concentration levels near the plate are raised to. A magnetic field of uniform strength is assumed to be applied normal to the flow. For free convection flow, it is also assumed that1) The induced magnetic field is assumed to be negligible as the magnetic Reynolds number of the flow is taken to be very small.

2) The viscous dissipation is neglected in the energy equation.

3) The effects of variation in density  with temperature and species concentration are considered only on the body force term, in accordance with usual Boussinesq approximation.

4) The fluid considered here is gray, absorbing/emitting radiation but a non-scattering medium.

5) Since the flow of the fluid is assumed to be in the direction of axis, so the physical quantities are functions of the space co-ordinate and  only.

Then by usual Boussinesq’s approximation, the flow is governed by the following equations.

(1)

(2)

(3)

with the following initial and boundary conditions

(4)

where The local radiant for the case of an optically thin gray gas is expressed by

(5)

It is assumed that the temperature differences within the flow are sufficiently small and that may be expressed as a linear function of the temperature. This is obtained by expanding in a Taylor series about and neglecting the higher order terms, thus we get

(6)

From Equations (5) and (6), Equation (2) reduces to

(7)

On introducing the following non-dimensional quantities

(8)

We get the following governing equations which are dimensionless

(9)

(10)

(11)

The initial and boundary conditions in dimensionless form are as follows:

(12)

3. Solution of the Problem

The appeared physical parameters are defined in the nomenclature. The dimensionless governing equations from (9) to (11), subject to the boundary conditions (12) are solved by usual Laplace transform technique and the solutions are expressed in terms of exponential and complementary error functions.

(13)

(14)

(15)

,

4. Nusselt Number

From temperature field, now we study Nusselt number (rate of change of heat transfer) which is given in nondimensional form as

(16)

From Equations (14) and (16), we get Nusselt number as follows:

5. Sherwood Number

From concentration field, now we study Sherwood number (rate of change of mass transfer) which is given in non-dimensional form as

(17)

From Equations (13) and (17), we get Sherwood number as follows:

6. Results and Discussions

In order to get a clear insight of the physical problem the velocity, temperature, concentration, the rate of heat transfer and the rate of mass transfer have been discussed by assigning numerical values to the parameters like radiation parameter (R), magnetic parameter (M), Schmidt parameter (Sc), Prandtl number (Pr), Dufour number (Du), thermal Grashof number (Gr), mass Grashof number (Gm) and time t from Figures 1-13 for the cases of cooling (Gr > 0, Gm >0) and heating (Gr < 0, Gm < 0) of plate. The heating and cooling takes place by setting up free convection currents due to temperature and concentration gradient.

Figure 1 depicts the effect of magnetic field parameter on the fluid velocity and we observed that an increase in magnetic field parameter the velocity decreases in case of cooling of the plate while it increases in case of heating. Figures 2-4 show the effects of R, Du, Gr and Gm on the velocity field u. From these figures, it is observed that the velocity u increases as the radiation parameter R or Dufour number Du or thermal Grashof number Gr or mass Grashof number Gm increases in case of cooling of the plate and a reverse effect is noticed in the case of heating. The velocity profiles for different values of Schmidt number are shown in Figure 5. From this it is seen that the velocity decreases with increasing values of Schmidt number in the case of cooling of the plate but increases in the case of heating of the plate. Figure 6 reveals the velocity variation with time t for the cases of both cooling and heating. From this we observed that the velocity increases as time t increases for the case of cooling and the trend is just reversed for the case of heating of the plate. The effect of permeability parameter k on the velocity field is shown in Figure 7. It is seen from this figure that the velocity increases with increase of permeability parameter k in both cases of cooling and heating of the plate.

The influence of various flow parameters on the fluid temperature are illustrated in Figures 8-10. Figure 8 depicts that the effects of the Dufour number on the fluid temperature. It can be clear seen from this figure that the diffusion thermal effects slightly affect the fluid temperature. As the values of Dufour number increase, the fluid temperature is also increases. The effect of thermal radiation R on the temperature field is illustrated in Figure 9. It is obvious that the radiation parameter restricts the fluid temperature. Therefore, using radiation we can control the fluid temperature. In , we depict the

Figure 1. Velocity profiles when Sc = 2.01, Pr = 0.71, R = 10, k = 5, Du = 0.03 & t = 0.4.

Figure 2. Velocity profiles when Sc = 2.01, Pr = 0.71, M = 3, k = 5, Du = 0.03 & t = 0.4.

Figure 3. Velocity profiles when Sc = 2.01, Pr = 0.71, R = 10, k = 5, M = 3 & t = 0.4.

Figure 4. Velocity profiles when M = 3, Pr = 0.71, Sc = 2.01, R = 10, k = 5, Du = 0.03 & t = 0.4.

Figure 5. Velocity profiles when M = 4, Pr = 0.71, R = 10, k = 5, Du = 0.03 & t = 0.4.

Figure 6. Velocity profiles when Sc = 2.01, M = 3, Pr = 0.71, R = 10, k = 5, Du = 0.03.

Figure 7. Velocity profiles when Sc = 2.01, Pr = 0.71, R = 10, M = 3, Du = 0.03 & t = 0.4.

Figure 8. Temperature profiles when R = 4, Pr = 0.71 & Sc = 2.01.

Figure 9. Temperature profiles when Du = 0.03, Pr = 0.71 & Sc = 2.01.

. Temperature profiles when R = 4, Du = 0.03 & Sc = 2.01.

. Concentration profiles.

. Nusselt number.

. Sherwood number.

effects of Prandtl number Pr on the temperature field. It is observed that an increase in the Prandtl number leads to decrease in the fluid temperature. It is due to the fact that thermal conductivity of the fluid decreases with increasing Pr, resulting a decrease in thermal boundary layer thickness.

The concentration profiles for different values of Schmidt number (Sc) and time t are presented in . From this figure it is seen that the concentration decreases with increase in Sc while it increases with time t. reveals the rate of heat transfer coefficient in terms of Nusselt number for different values of radiation parameter R, Prandtl number Pr and Dufour number Dr respectively. It is observed that Nusselt number increases with increasing values of R or Pr but decreases as Du increases. Finally, from it is seen that Sherwood number increases with increase of Sc.

REFERENCES

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Nomenclature

Absorption coefficient

External magnetic field

Species concentration

Concentration of the plate

Concentration of the fluid far away from the plate

Dimensionless concentration

Specific heat at constant pressure

Concentration susceptibility

Acceleration due to gravity

Thermal Grashof number

Mass Grashof number

Magnetic field parameter

Nusselt number

Prandtl number

Radiative heat flux in the y-direction

Coefficient of mass diffusivity

Schmidt number

Temperature of the fluid near the plate

Temperature of the plate

Temperature of the fluid far away from the plate

Time

Dimensionless time

Velocity of the fluid in the -direction

Velocity of the plate

Dimensionless velocity

Co-ordinate axis normal to the plate

Dimensionless co-ordinate axis normal to the plate

Greek Symbols

Thermal conductivity of the fluid

Thermal diffusivity

Volumetric coefficient of thermal expansion

Volumetric coefficient of expansion with concentration

μ       Coefficient of viscosity

ν        Kinematic viscosity

r         Density of the fluid

ρ        Electric conductivity

σ        Dimensionless temperature

erf      Error function

erfc     Complementary error function

Subscripts

Conditions on the wall

Free stream conditions

NOTES

*Corresponding author.