Abstract
A numerical analysis has been performed to examine the characteristics of laminar natural convection in vertical channel with unheated entry and unheated exit. The heated section is subjected to uniform wall temperature (UWT) or uniform heat flux (UHF). Theoretical results for average Nusselt number\(\overline {Nu} \) and induced volume flow rateQ were derived under fully developed condition. Particular attention is paid to investigating the effects of the partially heated section on the induced volume flow rate and Nusselt number for various conditions. Results show that for UWT the induced volume flow rateQ increases with decreasing unheated entry length or increasing total length of heated section and unheated exit. For a fixed unheated entry length, the channel with a longer heated section length causes a greaterQ. Additionally, for both UWT and UHF, the average Nusselt number\(\overline {Nu} \) under fully-developed condition increases with increasing value ofE 1/E 2.
Zusammenfassung
Die numerische Untersuchung soll das Verhalten einer laminaren Strömung bei natürlicher Konvektion in einem senkrechten Kanal mit unbeheiztem Ein- und Austritt klären. Der beheizte Abschnitt wird entweder mit gleichförmiger Wandtemperatur (UWT) oder gleichförmigem Wärmefluß (UHF) beaufschlagt. Bezüglich voll ausgebildeter Strömung ließen sich theoretische Ergebnisse für die mittlere Nußelt-Zahl\(\overline {Nu} \) und den induzierten VolumenstromQ gewinnen. Besonderes Interesse galt der Untersuchung des Einflusses des teilbeaufschlagten Abschnittes auf Volumenstrom und Nußelt-Zahl unter verschiedenen Nebenbedingungen. Die Ergebnisse zeigen, daß im UWT-Fall der induzierte VolumenstromQ mit abnehmender unbeheizter Einlauflänge oder zunehmender Gesamtlänge des Heizabschnittes anwächst. Bei fester unbeheizter Einlauflänge erzeugt der Kanal mit längerem Heizabschnitt einen höheren StromQ.
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Abbreviations
- b :
-
half channel width
- E 1 :
-
ratio of unheated exit length to channel length,l 1/l
- E 2 :
-
ratio of heated section length to channel length,l 2/l
- E 3 :
-
ratio of unheated entry length to channel length,l 3/l
- Gr L :
-
Grashof number, Eq. (4)
- g :
-
gravitational acceleration
- k :
-
thermal conductivity
- l :
-
channel length
- l 1 :
-
unheated exit length
- l 2 :
-
heated section length
- l 3 :
-
unheated entry length
- L :
-
dimensionless channel length, Eq. (4)
- L 1 :
-
dimensionless unheated exit length
- L 2 :
-
dimensionless heated section length
- L 3 :
-
dimensionless unheated entry length
- \(\overline {Nu} \) :
-
average Nusselt number
- Nu x :
-
local Nusselt number
- p′ :
-
pressure defect
- P :
-
dimensionless pressure defect, Eq. (4)
- Pr :
-
Prandtl number,ν/α
- q w :
-
wall heat flux of heated section
- Q :
-
dimensionless induced volume flow rate, Eq. (8)
- Ra E :
-
Rayleigh number based on the heated section length,Ra L/E2
- Ra L :
-
Rayleigh number based on the full channel length,Gr LPr
- T :
-
temperature
- T 0 :
-
inlet temperature
- T w :
-
wall temperature
- u, v :
-
velocity components in thex andy directions, respectively
- U, V :
-
dimensionless velocity components in thex andy directions, respectively, Eq. (4)
- u 0,U 0 :
-
dimensional and dimensionless inlet velocity, respectively
- x, y :
-
coordinates in thex andy directions, respectively
- X, Y :
-
dimensionless coordinates in thex andy directions, respectively, Eq. (4)
- X′ :
-
ratio of longitudinal distance from the entrance of heated section to the heated section length,X′=[X−(L−L 1−L 2)]/L 2
- α :
-
thermal diffusivity
- β :
-
thermal expansion coefficient
- ν :
-
kinematic viscosity
- θ :
-
dimensionless temperature, Eq. (4)
- ϱ 0 :
-
fluid density at ambient temperature
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Lee, K.T., Yan, W.M. Laminar natural convection between partially heated vertical parallel plates. Wärme- und Stoffübertragung 29, 145–151 (1994). https://doi.org/10.1007/BF01548598
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DOI: https://doi.org/10.1007/BF01548598