Module 8: BoiIing Lecture 29: Boiling Heat Transfer. The Lecture Contains: Introduction. Boiling modes. Pool Boiling. Correlations in Pool Boiling
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1 The Lecture Contains: Introduction Boiling modes Pool Boiling Correlations in Pool Boiling file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_1.html[12/24/2014 6:10:30 PM]
2 Introduction For boiling, the convection coeffiecient depends on Difference between the surface and saturation temperatures - The body force arising from the liquid-vapour density difference The latent heat hfg -the surface tension The surface tension 10 variables in 5 dimensions Result in groups Here, is Prandtl number and is Bond number. file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_2.html[12/24/2014 6:10:31 PM]
3 Boiling modes Heat is transferred from solid surface to the liquid Heat transfer is strongly in inuenced by the growth of vapor bubbles Pool Boiling Nukiyama identified different regimes of pool boiling by using a similar apparatus shown in the figure file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_3.html[12/24/2014 6:10:31 PM]
4 The following are various regimes of Boilling : 1. Natural Convection: This phenomenon occurs at low temperatures. Heat transfer from the heated surface to the liquid in its vicinity causes the liquid to be superheated. The superheated liquid rises to the free liquid surface by natural convection where vapor is produced by evaporation. file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_4.html[12/24/2014 6:10:31 PM]
5 2. Nucleate Boiling: It commences with the increased difference between II (a): The bubbles formed are very few in number. These bubbles grow in size, separate from the heated surface and rise to the free surface. II(b): The rate of bubble formation and number of locations where they are formed increase. 3. Film Boiling: High bubble formation rate causes them to coalesce and blanket the surface.with a vapor film. III (a): The vapor lm is unstable and involves partial film boiling and partial nucleate boiling. III (b): A stable lm covers the entire surface. The temperature difference is of the order of significant. and the radiative transfer across the vapor film is In the region I, the heat flux is proportional to n where n is slightly greater than unity (1.3). When the transition from natural convection to nucleate boiling occurs, heat flux starts to increase more rapidly with the temperature difference, the value of n increasing to about 3. At the end of region II, the boiling curve reaches a peak (point A). In III (a), inspite of increasing temperature difference, the heat flux decreases because the thermal resistance to heat flow increases with the formation vapor film. At the end of III (a), heat flux passes through a minimum (point B). It starts increasing with only when stable film boiling begins and radiation becomes significantly important. file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_5.html[12/24/2014 6:10:31 PM]
6 It is of interest to know how the temperature of the heating surface changes as the heat flux is steadily increased from zero. Upto point A, nucleate boiling occurs and the temperature of the heating surface is obtained by reading o the value from the boiling curve and adding to the value of. If the heat flux is increased a little beyond the value at A, the temperature of the surface shoots up to the value corresponding to point C. For many surfaces, the temperature at C is high enough to cause the material to melt. Thus in many practical situations, it is undesirable to cross this value. This value is therefore of significance in engineering and is called the critical or peak heat flux. Correlations in Pool Boiling 1. Natural convection saturated pool boiling.all liquid properties are evaluated at 2. Nucleate saturated pool boiling: file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_6.html[12/24/2014 6:10:31 PM]
7 Boiling n = 1.0 for water and 1.7 for other liquids. = another constant Platinum-water and Copper-water, the value is Nickel-water and Brass-water, the value is Peak heat flux in saturated pool boiling (Developed by Kutateladze and Zuber) If 2:7 where L is the characteristic dimension of the heater. Due to Lienhard and Dhir For horizontal cylinder of radius R file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_7.html[12/24/2014 6:10:31 PM]
8 4. Film saturated pool boiling (i) Minimum heat flux where c=0.62 (ii) Stable film boiling file:///d /Web%20Course%20(Ganesh%20Rana)/Dr.%20gautam%20biswas/Final/convective_heat_and_mass_transfer/lecture29/29_8.html[12/24/2014 6:10:32 PM]
We know from thermodynamics that when the temperature of a liquid
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