Abstract
Two-dimensional laminar boundary-layer equations of momentum, heat and mass transfer have been numerically solved tinder forced convection. A finite difference approximation of the governing equations in a Göertler-type variable domain has been implemented on computer. To provide rigorous initial conditions at x 0 in the boundary-layer code, differential equations governing heat and mass transfer in the stagnation region have been set up and solved numerically.
The effect of outer flow condition on skin friction as well as heat and mass transfer has been demonstrated. Results obtained made an improvement over past theoretical predictions based on analytical approximation, and agreed favorably with experimental data available.
Similar content being viewed by others
Abbreviations
- a:
-
Constant in stagnation region velocity
- Ai :
-
Coefficients in outer flow equation
- C:
-
Concentration
- CP :
-
Specific heat at constant pressure
- D:
-
Binary diffusity
- f:
-
Stagnation function defined by eq. (38)
- F:
-
Normalized velocity defined by eq. (27)
- G:
-
Stagnation function defined by eq. (38)
- L:
-
Characteristic length
- T:
-
Temperature
- u:
-
Streamwise velocity, dimensional
- U:
-
Outer flow velocity, dimensional
- v:
-
Normal velocity, dimensional
- V:
-
Normal velocity defined by eq. (28)
- x:
-
Streamwise coordinate, dimensional
- y:
-
Normal coordinate, dimensional
- y:
-
Stagnation region normal coordinate defined by eq. (38)
- w:
-
Condition at wall
- e:
-
Condition at boundary-layer edge
- *:
-
Dimensionless quantity defined by eqs. (11) and (12)
- Re:
-
Reynolds number = LUoρ/Μ(Uo =-free-stream velocity)
- Sc:
-
Schmidt number = Ν/D
- Sh:
-
Sherwood number = bL/D (b=mass transfer coefficient)
- Pr:
-
Prandtl number = CPΜ/k(k = thermal conductivity)
- α :
-
Thermal diffusity
- η :
-
Normal coordinate defined by eq. (22)
- Μ :
-
Viscosity
- Ν :
-
Kinematic viscosity
- ξ :
-
Streamwise coordinate defined by eq. (21)
- ρ :
-
Density
- ΤΩ :
-
Wall shear stress
- θ :
-
Angle measured from the front stagnation point
Reference
Winding, C.C. and Cheney, A.J.:Ind. Eng. Chem.,40, 1087 (1948).
Spalding, D.B. and Pun, W.M.:Int’l. J. Heat & Mass Trans.,5, 239 (1962).
Zukauskas, A.: “Advances in Heat Transfer”, 8, Academic Press, New York, NY (1972).
Frossling, N.: NACA TM 1433, 1940.
Chao, B.T.:Int’l. J. Heat & Mass Trans.,15, 907 (1972).
Sano, T.: J. Heat Trans., Trans. ASME,3, 100 (1978).
Krall, K.M. and Eckert, E.R.: Heat Transfer 1970, 3, FC7. 5(1970).
Bird, R.B., Stewart, W.E. and Lightfoot, E.N.: “Transport Phenomena”, Wiley, New York, NY (1960).
Telionis, D.P.: “Unsteady Viscous Flow”, Springer, New York, NY (1981).
Telionis, D.P., Tsahalis, D.T. and Werle, M.J.:Physics of Fluid,16, 968 (1973).
Schlichting. H.: “Boundary-Layer Theory”, 7th ed., McGraw-Hill, New York, NY (1079).
Sogin, H.H. and Sabaramanian. V.S.:J. Heat Trans., Trans. ASME, 483 (1961).
Borell, G., Kim, B.K., Ekhaml, W., Diller, T.E. and Telionis, D.P. : “Pressure and Heat Transfer Measurement”, Presented at 1984 ASME Fluid Engineering Conference, New Orleans, (1984).
Kim, B.K.: Ph D Dissertation, Virginia Polytechnic Institute and State Univ. (Dec. 1984), Blacksburg, Virginia, U.S.A.
Saxena, U.C. and Laird, A.D.:J. Heat Trans., Trans. ASME,3, 100 (1978).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Kim, B.K. Boundary-layer analysis of heat and mass transfer over a circular cylinder in crossflow. Korean J. Chem. Eng. 4, 29–35 (1987). https://doi.org/10.1007/BF02698096
Received:
Accepted:
Issue Date:
DOI: https://doi.org/10.1007/BF02698096