Summary
An analysis has been performed using a method similar to Graetz’s formulation for the laminar thermal entry region. The fluid is assumed to have a fully developed turbulent velocity profile throughout the length of the pipe. Local and fully developed Nusselt numbers are presented for fluids with Prandtl numbers ranging from 0.7 to 100 for Reynolds numbers between 50000 and 500000. A thermal entrance length is defined as the heated length required to bring the local Nusselt number to within 5 percent of the fully developed value. This length is found to decrease with increasing Prandtl number, dropping from about 10 diameters for a Prandtl number of 0.7 to less than one diameter for a Prandtl number of 100. Comparison is made with the results of Deissler, who used an integral method-boundary layer approach, and also with available experimental data. The effect of the thermal boundary conditions was studied by comparing the present uniform heat flux results with those of previous investigators who considered uniform wall temperature.
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Abbreviations
- a 2 :
-
thermal diffusivity,k/ρc p
- A n :
-
quantity used in calculating the Nusselt number from equation (18), C n φ n (r +0 )/G(r +0 ), dimensionless
- C n :
-
coefficient in the series expansion ofϑ 2, dimensionless
- c p :
-
specific heat at constant pressure
- D :
-
pipe diameter
- G(r+):
-
radial variation of the fully developed temperature profile, dimension-less
- h :
-
local heat transfer coefficient,q/(T w −T b )
- k :
-
thermal conductivity
- Nu :
-
local Nusselt number,hD/k, dimensionless;Nu ∞, fully developed Nusselt number
- Pr :
-
Prandtl number,v/a 2 =c p μ/k, dimensionless
- q :
-
local heat transfer rate at wall to fluid
- r :
-
radial coordinate;r 0, pipe radius
- r + :
-
dimensionless radial coordinate, (r√τ 0/ρ)/v;r +0 dimensionless pipe radius, (r 0√ρ 0/ρ)/v
- Re :
-
Reynolds number,Dū/v, dimensionless
- T :
-
temperature;T i , entering fluid temperature;T w , wall temperature;T b , bulk temperature
- u :
-
velocity component inx direction;ū, mean velocity
- u + :
-
dimensionless velocity inx direction,u/(√τ 0/ρ)
- x :
-
coordinate measuring axial distance from tube entrance
- x + :
-
dimensionless axial coordinate,x/r 0
- y :
-
coordinate measuring normal distance from tube wall,r 0 −r
- y + :
-
dimensionless coordinate normal to wall,y√τ 0/ρ)/v
- β 2 n :
-
eigenvalues of eq. (12b), dimensionless
- γ :
-
dimensionless total thermal diffusivity, (a 2 +te h )/ν
- ε h ,ε m :
-
eddy diffusivities for heat and momentum
- ϑ :
-
dimensionless temperature, (T −T i )/(qr 0/k)
- ν :
-
kinematic viscosity
- ρ :
-
fluid density
- τ 0 :
-
shear stress at wall
- ϕ :
-
eigenfunctions of eq. (12b), dimensionless
- χ :
-
exponentially decaying portion of entrance region temperature profile, dimensionless
References
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Beckers, H. L., Appl. Sci. Res.A6 (1956) 147.
Deissler, R. G., Trans. Amer. Soc. Mech. Engrs77 (1955) 1221. See also NACA TN 3016, 1953.
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Sparrow, E.M., Hallman, T.M. & Siegel, R. Turbulent heat transfer in the thermal entrance region of a pipe with uniform heat flux. Appl. sci. Res. 7, 37–52 (1957). https://doi.org/10.1007/BF03184700
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DOI: https://doi.org/10.1007/BF03184700