Multiphase Flow and Heat Transfer

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Multiphase Flow and Heat Transfer Wettability Sudheer Siddapuredddy sudheer@iitp.ac.

1 Multiphase Flow and Heat Transfer Wettability Sudheer Siddapuredddy Department of Mechanical Engineering Indian Institution of Technology Patna Multiphase Flow and Heat Transfer Wettability 1 / 15

2 Wettability Usually, a liquid-vapor phase change is accomplished by transferring energy through the walls of a container or channel into or out of a two-phase system. The vaporization or condensation process ultimately takes place at the liquid-vapor interface. However, the contact through which the energy is transferred will strongly affect the resulting heat and mass transfer in the system. The performance of heat transfer equipment in which vaporization or condensation occurs may depend strongly on the way that the two phases contact the solid walls. Multiphase Flow and Heat Transfer Wettability 2 / 15

film to maximize the liquid-solid contact area.

3 Wettability Liquids with weak affinities for a solid wall will collect themselves into beads while those with high affinities for solid will form film to maximize the liquid-solid contact area. The affinity of liquids for solids - wettability of the fluid. Multiphase Flow and Heat Transfer Wettability 3 / 15

4 Wettability Liquids with weak affinities for a solid wall will collect themselves into beads while those with high affinities for solid will form film to maximize the liquid-solid contact area. The affinity of liquids for solids - wettability of the fluid. Multiphase Flow and Heat Transfer Wettability 3 / 15

5 Neumann s Formula or Young s Equation σ sv = σ sl + σ lv cos θ Vertical force σ lv sin θ must be balanced by a vertical reaction force in the solid. Multiphase Flow and Heat Transfer Wettability 4 / 15

6 Neumann s Formula or Young s Equation σ sv = σ sl + σ lv cos θ Vertical force σ lv sin θ must be balanced by a vertical reaction force in the solid. Small and also modulus of elasticity of solid is high No deformation occurs σ sl and σ sv are not available easily. Multiphase Flow and Heat Transfer Wettability 4 / 15

7 Neumann s Formula or Young s Equation As θ 180 (if g is negligible) Liquid droplet - sphere One point of contact on solid Completely non-wetting Multiphase Flow and Heat Transfer Wettability 5 / 15

8 Neumann s Formula or Young s Equation As θ 180 (if g is negligible) Liquid droplet - sphere One point of contact on solid Completely non-wetting As θ 0 A thin film configuration Completely wet the solid Multiphase Flow and Heat Transfer Wettability 5 / 15

9 Neumann s Formula or Young s Equation As θ 180 (if g is negligible) Liquid droplet - sphere One point of contact on solid Completely non-wetting As θ 0 A thin film configuration Completely wet the solid Wetting liquid: As 0 < θ < 90 Non-wetting liquid: As 90 < θ < 180 one point of contact on solid Multiphase Flow and Heat Transfer Wettability 5 / 15

10 Neumann s Formula or Young s Equation σ sv = σ sl + σ lv cos θ; cos θ 1 At equilibrium: σ sv σ sl σ lv < 1 Multiphase Flow and Heat Transfer Wettability 6 / 15

11 Neumann s Formula or Young s Equation σ sv = σ sl + σ lv cos θ; cos θ 1 At equilibrium: σ sv σ sl σ lv < 1 If σ sv σ sl < 1, σ sl pulls the contact line, θ 180 σ lv Never happens for a droplet surrounded by its vapor, but could happen for a liquid droplet in another immiscible liquid. Multiphase Flow and Heat Transfer Wettability 6 / 15

12 Neumann s Formula or Young s Equation σ sv = σ sl + σ lv cos θ; cos θ 1 At equilibrium: σ sv σ sl σ lv < 1 If σ sv σ sl < 1, σ sl pulls the contact line, θ 180 σ lv Never happens for a droplet surrounded by its vapor, but could happen for a liquid droplet in another immiscible liquid. If σ sv σ sl σ lv > 1, σ sv pulls the contact line, θ 0 Until the film becomes so thin that molecular interactions come into play. Multiphase Flow and Heat Transfer Wettability 6 / 15

13 Spreading Coefficient Sp ls = σ sv (σ lv + σ sl ) Sp ls measures the difference between the surface energy σ sv and its value in the case of complete wetting. Multiphase Flow and Heat Transfer Wettability 7 / 15

14 Spreading Coefficient Sp ls = σ sv (σ lv + σ sl ) Sp ls measures the difference between the surface energy σ sv and its value in the case of complete wetting. Sp ls = σ lv (cos θ 1) Multiphase Flow and Heat Transfer Wettability 7 / 15

15 Spreading Coefficient Sp ls = σ sv (σ lv + σ sl ) Sp ls measures the difference between the surface energy σ sv and its value in the case of complete wetting. Sp ls = σ lv (cos θ 1) Sp ls > 0, the liquid will wet the solid and spontaneously spread into a thin film. Sp ls < 0, the liquid will partially wet the solid and establish an equilibrium contact angle. Multiphase Flow and Heat Transfer Wettability 7 / 15

16 Spreading Coefficient Sp ls = σ sv (σ lv + σ sl ) Sp ls measures the difference between the surface energy σ sv and its value in the case of complete wetting. Sp ls = σ lv (cos θ 1) Sp ls > 0, the liquid will wet the solid and spontaneously spread into a thin film. Sp ls < 0, the liquid will partially wet the solid and establish an equilibrium contact angle. These results are theoretical and no lack of σ sv and σ sl. Multiphase Flow and Heat Transfer Wettability 7 / 15

Essentially, Forming 2 new interfaces Breaking one interface Adhesion: due to the minimum

17 Work of Adhesion Cylindrical column formed by l, s and low density gas, g. The net reversible work required per unit of interface area: w sl = σ lg + σ sg σ sl Essentially, Forming 2 new interfaces Breaking one interface Adhesion: due to the minimum reversible work required to tear the liquid off the solid surface. Multiphase Flow and Heat Transfer Wettability 8 / 15

18 Work of Cohesion Now consider, instead of solid-liquid column there is only one liquid column. To tear a single liquid column in half: w ll = 2σ lg Essentially, two interfaces are formed without breaking any interface. Cohesion: work required to break internal bonds of the material. Multiphase Flow and Heat Transfer Wettability 9 / 15

19 Work of Cohesion Now consider, instead of solid-liquid column there is only one liquid column. To tear a single liquid column in half: w ll = 2σ lg Essentially, two interfaces are formed without breaking any interface. Cohesion: work required to break internal bonds of the material. Adhesion - for dissimilar particles Cohesion - for similar particles Multiphase Flow and Heat Transfer Wettability 9 / 15

20 Work per Unit Area Required for Spreading Now lets march further. Lets say there is a liquid column of area A, and height δ. We are making it into a liquid column of area 2A and height of δ/2. Multiphase Flow and Heat Transfer Wettability 10 / 15

21 Work per Unit Area Required for Spreading Now lets march further. Lets say there is a liquid column of area A, and height δ. We are making it into a liquid column of area 2A and height of δ/2. w sp = σ lg + σ sl σ sg Multiphase Flow and Heat Transfer Wettability 10 / 15

We are making it into a liquid column of area 2A and height of δ/2.

22 Work per Unit Area Required for Spreading Now lets march further. Lets say there is a liquid column of area A, and height δ. We are making it into a liquid column of area 2A and height of δ/2. w sp = σ lg + σ sl σ sg = Sp ls Work interaction is negative (Sp ls is positive for spreading). Work could be extracted if we can (= Sp ls ). Multiphase Flow and Heat Transfer Wettability 10 / 15

23 Adhesion and Cohesion Sp ls = w sp =w sl w ll Spreading coefficient =difference between { the work of adhesion the work of cohesion Sp ls indicates the tendency of the liquid to adhere to the solid relative to its internal cohesive forces. Multiphase Flow and Heat Transfer Wettability 11 / 15

24 Surface Tension of a Mixture w sl = σ lg + σ sg σ sl Applying it to any two solid or liquid phases a and b, and a low density gas or vapor phase g, w ab = σ bg + σ ag σ ab Multiphase Flow and Heat Transfer Wettability 12 / 15

25 Surface Tension of a Mixture w sl = σ lg + σ sg σ sl Applying it to any two solid or liquid phases a and b, and a low density gas or vapor phase g, w ab = σ bg + σ ag σ ab σ ab = σ bg + σ ag w ab The work of adhesion is approximately given as: w ab = 2 (σag σ bg ) 1 2 σ ab = σ bg + σ ag 2 (σ ag σ bg ) 1 2 Multiphase Flow and Heat Transfer Wettability 12 / 15

26 Problem For water and hexane in contact with air at 20 C, σ wg is N/m and σ hg is N/m respectively. Use these data to estimate the interfacial tension between hexane and water. Compare this value to experimentally determined value of σ wh = N/m. σ ab = σ bg + σ ag 2 (σ ag σ bg ) 1 2 Multiphase Flow and Heat Transfer Wettability 13 / 15

27 Problem For water and hexane in contact with air at 20 C, σ wg is N/m and σ hg is N/m respectively. Use these data to estimate the interfacial tension between hexane and water. Compare this value to experimentally determined value of σ wh = N/m. σ ab = σ bg + σ ag 2 (σ ag σ bg ) 1 2 σ wh = N/m Multiphase Flow and Heat Transfer Wettability 13 / 15

28 Problem For water and hexane in contact with air at 20 C, σ wg is N/m and σ hg is N/m respectively. Use these data to estimate the interfacial tension between hexane and water. Compare this value to experimentally determined value of σ wh = N/m. σ ab = σ bg + σ ag 2 (σ ag σ bg ) 1 2 σ wh = N/m This is 65% accuracy or 35% of the actual value. Sp hw = σ wg σ hg σ wh Multiphase Flow and Heat Transfer Wettability 13 / 15

29 Problem Sp hw = σ wg σ hg σ wh = N/m Sp hw > 0, hexane would spontaneously spread over the surface of water However, close to zero and so tendency is weak. Hexane is unlikely to form lens-shaped droplets. Spread out into a film, not aggressively covers the entire liquid surface. Multiphase Flow and Heat Transfer Wettability 14 / 15

30 Spread Thin Films Spontaneous spreading of liquid helium over the walls of a Dewar flask Multiphase Flow and Heat Transfer Wettability 15 / 15

Polymer Interface and Adhesion

Polymer Interface and Adhesion SOUHENG WU E. I. du Pont de Nemours &.Company Wilmington, Delaware MARCEL DEKKER, INC. New York and Basel Preface Acknowledgments 1. INTERFACIAL THERMODYNAMICS 1 1.1 Formulation