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Recent Advances in Condensation on Tube Banks P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Reduce the Degree of Over Design!!!

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Presentation on theme: "Recent Advances in Condensation on Tube Banks P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Reduce the Degree of Over Design!!!"— Presentation transcript:

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2 Recent Advances in Condensation on Tube Banks P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Reduce the Degree of Over Design!!!

3 N Condensation on Horizontal Bundles: Prediction of Heat Transfer Coefficient in Nth Tube Row

4 Falling Film Condensation on Horizontal Tubes Falling-film heat exchangers are attractive because they provide good heat transfer performance and low working-fluid inventories. The design of falling-film heat exchangers has been largely based on empirical data. A thorough understanding of the falling-film flow and heat transfer interactions is important. An ability to predict the falling film mode would allow better data correlation and improve the modeling and analysis of heat transfer and fluid flow. The ultimate aim of this advanced learning is to enhance economy of heat exchanging.

5 Modes of Condensation on Tube Bundle The droplet mode The jet modeThe sheet mode

6 Daily Load Variation on A Power Plant % of Maximum Capacity

7 Daily Variation of Flow Rate through Condenser

8 Flow Rate Vs Mode of Falling Film

9 Identification of flow Regimes

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11 Condensation on Horizontal Tube Bundles : Flow Map Hu and Jacobi (1996) proposed flow mode transition equations with Re Γ versus Ga+ (film Reynolds number vs the Galileo number) Following principal flow modes were defined : sheet flow, column flow and droplet flow. The mixed mode transition zones of column-sheet and droplet- column were also considered as regimes, bringing the total to five.

12 Flow Transition Map

13 Identification Condensation Mode

14 The true characteristic Dimension The film thickness is the true characteristic dimension: Nusselt Number,

15 Ripples & Waves Experimental results showed a positive difference when compared to Nusselt theory. This positive difference was attributed to interfacial instability and occurrence of ripples in film. The ripples enhances the surface area and lowers the film thickness. The effect of ripples are accounted in the Nusselt number through a new number called Archimedes number. Archimedes Number,

16 Final Correlations for Condensation Heat Transfer For the Sheet Mode For the Jet Mode For the Drop Mode

17 Onset of Turbulence & Turbulent Film Condensation The transition film Reynolds number for the tube bundle is adapted from a vertical plate turbulent transition criterion of 1600 (but also values of 1200, 1800 and 2000 have been proposed). Thus, the film will become turbulent on the tube bundle at Re Γ equal to 1600 and thus when Re Γ > 1600 the following expression should be used.

18 Condensation on Horizontal Tube Bundles : Turbulent Flow Turbulent flow of the condensate film may be reached in a condenser, which significantly increases heat transfer. Comparatively little has been published on turbulent film condensation on tube bundles compared to the information available for laminar films. Butterworth (1983) recommends adapting the Labuntsov expression for turbulent film condensation on a horizontal tubes for predicting local turbulent film condensation on the N th tube row in horizontal tube bundles h

19 Computation of Wall Temperatures It is often necessary to calculate the wall temperature by an iterative approach. The summarized procedure is: 1.Assume a film temperature, T f 2.Evaluate the fluid properties (viscosity, density, etc.) at this temperature 3.Use the properties to calculate a condensing heat transfer coefficient. 4.Calculate the wall temperature. The relationship will typically be something like

20 5. Use the wall temperature to calculate a film temperature 6.Compare the calculated film temperature to that from the initial step. 7.If not equal, reevaluate the properties and repeat.

21 Extreme Limits Shell And Tube Heat Exchanger

22 Extreme Combinations Large cold fluid to hot fluid specific heat ratios. Large ratios of Volumetric flow rates. Large ratios of Convection heat transfer coefficients. Numerical value of these ratios tending to infinite. Impossible to contain the large volume flow rates. How to obtain a velocity of wetting without containing?

23 Power Plant Steam Generator : An extreme HX

24 Cylinder in Cross Flow

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28 Generally the overall average Nusselt number for heat transfer with the entire object is important. Correlations are developed from experimental data to compute Nu as a f(Re m,Pr n ) Overall Average Nusselt number All properties are evaluated at the freestream temperature, except Pr s which is evaluated at the surface temperature.

29 Values for C and m Expect an accuracy within  20% with these correlations Re D Cm 1 -400.750.4 40 - 10000.510.5 1000 – 2X 10 5 0.260.6 2X 10 5 - 10 6 0.0760.7


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