Magnetic Behavior of Titanates and Its Implications
Investigation of layer conditions and heat transfer in viscoelastic fluid flow
by Dr. J. Altaf Ahamad*,
- Published in Journal of Advances and Scholarly Researches in Allied Education, E-ISSN: 2230-7540
Volume 6, Issue No. 11, Jul 2013, Pages 0 - 0 (0)
Published by: Ignited Minds Journals
ABSTRACT
As far as possible layer conditions for energy and warmth trade which are non-straight fractional differential condition are changed over into non-direct regular differential condition using similarity change. The resulting non-direct condition is understood using numerical shooting system for three darken starting conditions with fourth demand Runge-Kutta technique. This work deals with the point of confinement layer stream and warmth move in a visco-adaptable liquid stream a broadening sheet inside seeing radiation. Two unmistakable temperature are considered here, (I) PST, that is the sheet with embraced surface temperature (ii)PHF, that is the sheet with prescribed warm change. To know the material study of the issue, numerical results are discussed with the help of diagrams for various of parameters, for instance, liquid consistency parameter, visco-flexible parameter, Prandtl number, Eckert number, warm sourcesink parameter and radiation parameter.
KEYWORD
Magnetic behavior, Titanates, Implications, Layer conditions, Energy exchange, Non-linear fractional differential equation, Similarity transformation, Numerical shooting method, Viscoelastic fluid flow, Heat transfer, Material study, Diagrams
1. INTRODUCTION
The examination of the limit layer stream over a nonstop solid surface moving with relentless speed. The examination of the stream and warmth trade of an incompressible homogeneous second grade liquid over a non-isothermal extending sheet. Using similarity change they change over the fragmentary Differential conditions to standard differential conditions. Twofold amigo and Hiranmoymondal researched the examination of combined effects of Soret and Dufour on uncertain MHD non-Darcy mixed convection over an extending sheet. Limit layer lead over a moving predictable solid surface is a basic kind of stream occurring overall designing structures. The warmth trade due to an interminably moving surface through an incorporating liquid is one of the push zones of back and forth movement examine. Such examinations find their application over a broad range of science and designing controls particularly in the field of manufactured building process like metallurgical process, polymer ejection process includes cooling of a fluid, liquid being stretched out into a cooling (Andersson, 1992). The effect of radiation on the warmth and liquid stream over an unreliable extending surface. MHD stream of a visco adaptable liquid past an extending surface. Warmth and mass move in an extending sheet suction or blowing (Abo-Eldahab, et. al., 2004). These coupled non-direct conditions, speaking to the issue, are diminished to an arrangement of coupled non-straight higher-arrange customary differential conditions by applting sensible similarity changes. This resultant limit regard issue has been changed over into the arrangement of six-simultaneous conditions of first request for six inquiries. By then this framework is lit up by using a numerical shooting strategy (for two cloud starting conditions) with fourth-arrange Runge-Kuttamix contrives. Count is finished for temperature and even speed profiles, Nusselt number and skin disintegration parameter when the dividers are stayed aware of prescribed surface temperature and embraced divider warm changes. Examinations have been had to investigate the effect of liquid thickness, visco-adaptability, vulnerability of the porous medium and Prandtl number on the stream direct and warm trade process. Highlight has been laid to think about the effect of liquid thickness on the other physical characteristics. One of the crucial disclosures in the present examination is that the effect of liquid viscocity parameter is to lessen the temperature profile basically when the stream is through a porous medium.
2. MATHEMATICAL FORMULATION
Consider a steady laminar stream of an incompressible visco-adaptable liquid (walter's liquid B) in a porous medium past a semi-limitless two identical and opposite forces along the x-hub which achieves extending of the sheet and in this way the stream is created in light of the extending of the sheet. We have x-pivot along the surface, y-hub being ordinary to it and u and v are the liquid distracting speed and typical speed separately (Bataller, 2007). Where k0 is the visco flexible parameter, ν is the kinematic consistency, are vulnerability of the porous medium, k is the warm conductivity of the liquid, μ is the coefficient of thickness of the liquid, is the consistent estimation of temperature and coefficient of thickness a long way from the sheet and qr is the radiative heat progress. The term Q addresses the volumetric rate of warmth age. Eq. (2) has been induced with the doubt that the dedication from the ordinary weight is of an indistinct request of greatness from the shear stress, despite the run of the mill limit layer estimation. Here, μ is the coefficient of thickness, which is considered to change as a part of temperature (Chen and Char, 1988).
3. NUMERICAL SOLUTION
The above conditions (1) and (2) are nonlinear standard differential condition. Which establish the nonlinear limit regard issue as no prescribed method is available to handle nonlinear limit regard issue; it must be diminished to an underlying regard issue. This methodology is done by Runge-Kutta shooting procedure. To begin the shooting strategy. We have to make an underlying figure admirably for the estimations offꞌꞌꞌ (0), fꞌꞌ (0) θꞌ (PHF case). The accomplishment of the strategy depends particularly on how extraordinary the figure is .Numerical results are found for a couple of estimations of the physical parameters E, Pr, k1, k2,, R.
4. RESULTS AND DISCUSSION
In the present work, the effect of liquid consistency, visco-flexibility, penetrability of the porous medium and prandtl number on the stream lead and warmth exchange process. The limit layer fragmented differential condition which are extremely non-direct, have been changed over into set of typical differential condition by applying likeness change and they are lit up by numerically using Runge-Kuttastrategy (Carragher, P and Crane L.J. (1982). Fig1depicts the effect of radiation for various viscoelastic parameter on the warmth exchange by virtue of PST. Two plots reveal that the dimensionless temperature θ (n ) versus from the divider, increases with growing the estimations of visco-adaptable warmth exchange by virtue of PST. Two plots reveal that the dimensionless speed fꞌ(n ) versus from the divider, increases with extending estimations of visco-adaptable parameter (k1) and reducing estimations of radiation parameter (R).
Fig.1 Effect of radiation parameter for various values of K1 in PST case with Pr=7.0, E=0.02, K2=0.0, B=- 0.05 for temperature profile
Fig.2 Effect of radiation parameter for various values of K1 in PST case with Pr=7.0, E=0.02, K2=1.0, B=-0.05 for velocity profile.
Fig 3 Depicts the effect of radiation for various of liquid thickness parameter on the warmth exchange because of PST. Two plots reveal that the dimensionless temperature θ (n) versus from the divider, increases with extending estimations of liquid consistency parameter (An) and decreasing estimations of radiation parameter (R).fig4 Shows the effect of radiation for various estimations of prandtl number on the warmth exchange by virtue of PST. Two plots reveal that the dimensionless speed fꞌ(n) versus from the divider increases with growing estimations of prandtl number (Pr) and lessening estimations of radiation parameter (R) (Dual and Hiranmoy, 2011). It is seen from that the effect of growing qualities pf prandtl number and radiation parameter diminished the speed profile in PST case.
Dr. J. Altaf Ahamad*
Fig.3 Effect of radiation parameter for various values of A in PST case withPr=7.0, E=0.02, K1=0.1, K2=0.2, B=-0.05 for temperature profile
Fig.4 Effect of radiation parameter for various values of Prandtl number in PST case with E=0.02, B=-0.05, K1=0.1, K2=0.2 for velocity profile
Fig 5 speaks to the effect of radiation for various estimations of Eckert number on the warmth exchange by virtue of PST. Two plots reveal that the dimensionless temperature θ (n) versus from the divider increases with growing estimations of Eckert number (E) and diminishing estimations of radiation (R). It is seen from expect that the effect of extending estimations of Eckect number and radiation reduced the temperature profile in PST case (Gupta and Gupta, 1977).
Fig.5 Effect of radiation parameter for various values of Eckert number in PST case with Pr=7.0, B=-0.05, K1=0.1, K2=0.2 for velocity profile
Fig 6. Demonstrates the effect of radiation for various estimations of warmth source/sink parameter on the warmth exchanges because of PST. Two plots reveal that the dimensionless speed fꞌ(n) versus n from the divider, increases with growing estimations of warmth source/sink parameter (β) and diminishing estimations of radiation parameter (R). It is seen from the expect that the effect of revive estimations of warmth source/sink parameter and radiation parameter decelerate the speed profile in PST case.
Fig 6 Effect of radiation parameter for various values of heat source/sink in PST case with Pr=7.0, E=0.02, K1=0.1, K2=0.2 for velocity profile
Table I gives the values of skin friction coefficient for different values of Pr, k1, k2, and R. The expands singular values of Pr, k1, k2, and R are to diminishes, the rate of heat transfer in skin friction coefficients (Hayat, 2010)
5. CONCLUSION
The effect of warmth radiation on the stream of walter's liquid B over an impermeable extending sheet with warmth source/sink and adaptable parameter have been discussed. The examination were finished for two sorts of different warming procedure particularly (I) Prescribed surface temperature (PST) and (ii) Prescribed divider warm change (PHF). The effects of rising parameters have been what's more, inspected through table in (PHF) (Lai and Kulacki, 1990). The end got from this examination as said underneath • It is found that the temperature profile and speed profile decreases with the extending estimation of the visco-adaptable parameter, Eckert number and warmth source/sink parameter. • The temperature lessens with the extending estimation of Prandtl number, liquid thickness parameter and radiation parameter. • The combined effect of extending of radiation parameter with growing visco flexible parameter, Eckert number, Prandtl number and liquid thickness reduces the temperature profile and speed profile (Mahantesh and Vajravelu, 2011)
6. REFERENCES
1. Andersson, H.I. (1992). MHD flow of a visco-elastic fluid past a stretching surface, Acta. Mech., 95, pp. 227-232 2. Abo-Eldahab Emad, M. and E.I. AZIZ Mohammed, A. (2004). Blowing suction effect on hydromagentic heat transfer by mixed convection from an inclined continuously stretching surface with internal heat 3. Bataller, P. (2007). Effects of heat source/sink, radiation and work done by deformation on flow and heat transfer of a viscoelastic fluid over a stretching sheet, computer and maths with Appl., 35, pp. 305-316. 4. Chen, C.K and Char, M.I. (1988). Heat transfer on a continuous stretching surfaces with suction or blowing, J. Math .Anal. Appl., 33, pp. 568-580 5. Carragher, P and Crane L.J. (1982). Heat transfer on a continuous stretching sheet, ZAM P, 12, pp. 564-565 6. Dual Pal, E. and Hiranmoy Mondal, M. (2011). Effects of soretDuffour, chemical reaction and thermal radiation on MHD non-Darcy stretching sheet, Int. J. Nonlinear Mech., 45, pp. 1942-1958 7. Gupta, P.S and Gupta, A.S. (1977). Heat and mass transfer in a stretching sheet with suction or blowing, Can .J. Chem. Eng, 21, pp. 744-746. 8. Hayat, P. (2010). Effects of radiation and magnetic field on the mixed convection stagnation point flow over a vertical stretching sheet in a porous medium, Int. J. Heat Mass Transfer., 30, pp. 466-474 9. Lai, F.C and Kulacki, F.A. (1990). The effect of variable viscosity on convective heat transfer along a vertical surface in a saturated porous medium, Int.J. Heat Mass Transfer, 56, pp. 10-28 10. Mahantesh, M. and Vajravelu, K. (2011). Heat transfer in MHD viscoelastic boundary layer flow over a stretching sheet with thermal radiation and non-uniform heat source/sink, Int. J. Nonlinear mech., 24, pp. 578-3590.
Corresponding Author Dr. J. Altaf Ahamad*
Associate Professor of Physics, S.B.S.Y.M. Degree College, Kurnool, Andhra Pradesh