Acta Mechanica

, Volume 99, Issue 1–4, pp 21–33 | Cite as

Flow of a generalized second grade fluid between heated plates

  • G. Gupta
  • M. Massoudi
Contributed Papers

Summary

We examine the fully developed flow of a generalized fluid of second grade between heated parallel plates, due to a pressure gradient along the plate. The constant coefficient of shear viscosity of a fluid of second grade is replaced by a shear dependent viscosity with an exponentm. If the normal stress coefficients are set equal to zero, this model reduces to the standard power-law model. We obtain the solution for the case when the temperature changes only in the direction normal to the plates for the two most commonly used viscosity models, i.e. (i) when the viscosity does not depend on temperature, and (ii) when the viscosity is an exponentially decaying function of temperature.

Keywords

Viscosity Fluid Dynamics Pressure Gradient Normal Stress Shear Viscosity 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

List of symbols

Alphanumeric

A1,A2

Kinematical tensor

b

Body force

C

Dimensionless parameter related to the pressure gradient

h

Separation between the plates

L

Velocity gradient

m

Power-law index

M

Constant appearing in the Reynolds viscosity model

p

Pressure field

\(\hat p,\hat \bar p\)

Modified pressure field

q

Heat flux vector

r

Radiant heating

T

Cauchy's stress tensor

l

Unit tensor

v

Velocity vector

V

Characteristic velocity

x

Axis along the plate

y

Axis perpendicular to the plate

Greek

α1, α2

Normal stress coefficient

ε

Specific internal energy

Γ

Dimensionless parameter related to the viscous dissipation

ϕ

Conservative body force field

η

Specific entropy

κ

Thermal conductivity

μ

Coefficient of viscosity

μ0

Reference viscosity

Π

Second invariant of the stretching tensor

θ

Temperature

θ1

Temperature of the lower plate

θ2

Temperature of the upper plate

ϱ

Density

ψ

Specific Helmholtz free energy

Operators

div

Divergence

grad

Gradient

tr

Trace

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References

  1. [1]
    Tsai, C. Y., Novack, M., Roffe, G.: Rheological and heat transfer characteristics of flowing coal-water mixtures. Final Report, DOE/MC/23255-2763 (1988).Google Scholar
  2. [2]
    Ekmann, J. M., Wildman, D. J., Chen, J. L. S.: Laminar flow studies of highly loaded suspensions in horizontal pipes. Second International Symp. Slurry Flows, ASME FED38, pp. 85–92 (1986).Google Scholar
  3. [3]
    Schowalter, W. R.: Mechanics of non-Newtonian fluids. New York: Academic Press 1978.Google Scholar
  4. [4]
    Truesdell, C., Noll, W.: The non-linear field theories of mechanics. In: Handbuch der Physik (Flügge, S. ed.) III/3. Berlin Heidelberg New York: Springer 1965.Google Scholar
  5. [5]
    Rivlin, R. S., Ericksen, J. L.: Stress deformation, relations for isotropic materials. J. Rat. Mech. Anal.4, 323–425 (1955).Google Scholar
  6. [6]
    Man, C. S., Shields, D. H., Kjartanson, B., Sun, Q. K.: Creep of ice as a fluid of complexity 2: the pressuremeter problem. Proc. 10th CANCAM,1, pp. A347-A348 (1985).Google Scholar
  7. [7]
    Man, C. S., Sun, Q. K.: On the significance of normal stress effects in the flow of glaciers. J. Glaciology33, 268–273 (1987).Google Scholar
  8. [8]
    Szeri, A. Z., Rajagopal, K. R.: Flow of a non-Newtonian fluid between heated parallel plates. Int. J. Non-Linear Mech.20, 91–101 (1985).Google Scholar
  9. [9]
    Rajagopal, K. R.: Thermodynamics and stability of non-Newtonian fluids. Ph. D. Thesis, University of Minnesota, USA (1978).Google Scholar
  10. [10]
    Rajagopal, K. R.: Boundedness and uniqueness of fluids of the differential type. Acta Ciencia India18, (1982).Google Scholar
  11. [11]
    Dunn, J. E.: On the free energy and stability of nonlinear fluids. J. Rheology26, 43–68 (1982).Google Scholar
  12. [12]
    Dunn, J. E., Rajagopal, K. R.: A critical review and analysis of fluid of the differential type (to appear).Google Scholar
  13. [13]
    Dunn, J. E., Fosdick, R. L.: Thermodynamics, stability, and, boundedness of fluids of complexity 2 and fluids of second grade. Arch. Rat. Mech. Anal.56, 191–252 (1974).Google Scholar
  14. [14]
    Straughan, B.: Energy stability in the Benard problem for a fluid of second grade. J. Appl. Math. Phys. (ZAMP)34, 502–508 (1983).Google Scholar
  15. [15]
    Rajagopal, K. R., Na, T. Y.: Natural convection flow of a non-Newtonian fluid between two vertical flat plates. Acta Mech.54, 239–244 (1985).Google Scholar
  16. [16]
    Massoudi, M., Christie, I.: Natural convection flow of a non-Newtonian fluid between two concentric vertical cylinders. Acta Mech.82, 11–19 (1990).Google Scholar
  17. [17]
    Gupta, G., Massoudi, M.: Heat transfer and flow of a modified second grade fluid. In: Fundamentals of heat transfer in non-Newtonian fluids. ASME HTD174, 7–12 (1991).Google Scholar
  18. [18]
    Winter, H. H.: Viscous dissipation in shear flows of molten polymers. Adv. Heat Transfer13, 205–267 (1977).Google Scholar
  19. [19]
    Hutter, K.: Theoretical glaciology. Dordrecht: Reidel 1983.Google Scholar
  20. [20]
    Mansutti, D., Rajagopal, K. R.: Flow of a shear-thinning fluid between intersecting planes. Int. J. Non-Linear Mech.26, 769–775 (1991).Google Scholar

Copyright information

© Springer-Verlag 1993

Authors and Affiliations

  • G. Gupta
    • 1
  • M. Massoudi
    • 2
  1. 1.Department of Mechanical EngineeringUniversity of PittsburghPittsburghUSA
  2. 2.U.S. Department of EnergyPittsburgh Energy Technology CenterPittsburghUSA

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