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ACS© 2005 Foam Technology – Lecture 7 Jean Siméon Chardin (1699-1779)

Lecture 7 Foam Technology - Colloidal Dispersions© 2005 Lecture 7 - Foam Technology 8 Uneven film drainage ... •Formation of liquid crystalline phases in the thin films ... Lecture

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ACS© 2005

Foam Technology – Lecture 7

Jean Siméon Chardin (1699-1779)

Lecture 7 - Foam Technology 1ACS© 2005

Foam Structures

Foam structure of a wet spherical foam made with Sodium Caproyl Lactylateat 400X magnification

Foam structure of dry hexagonal foam fromcocoamidopropyl betaineat 400X magnification

/www.ctmw.com/articles/Rita/2.htm

Lecture 7 - Foam Technology 2ACS© 2005

Plateau border

Exerowa and Kruglyakov, p. 15

Lecture 7 - Foam Technology 3ACS© 2005

The Kelvin tetrakaidecahedron

Lamella

Plateau border

Gibbs angle

Lecture 7 - Foam Technology 4ACS© 2005

Formation of bubbles

Exerowa and Kruglyakov, p. 2

Lecture 7 - Foam Technology 5ACS© 2005

Formation of foams

The pressure in the liquid at B is less than that at A or A’.

A A’B

Two bubbles floating at the liquid-air interface:

Lecture 7 - Foam Technology 6ACS© 2005

Draining Foam Films

http://ptcl.chem.ox.ac.uk/~rkt/tutorials/tutimages/foam.jpg

Lecture 7 - Foam Technology 7ACS© 2005

Formation of black films

Exerowa and Kruglyakov, p. 120

Lecture 7 - Foam Technology 8ACS© 2005

Uneven film drainage

Exerowa and Kruglyakov, p. 221

Wasan et al. discovered the stepwise thinning of thin films. The stable thicknesses are layers of close-packed micelles.

Lecture 7 - Foam Technology 9ACS© 2005

Dynamic Foam Stability

Ross & Suzin, Langmuir, 1985, 1, 145-9.

Liquid level

To gasflow meter

Nitrogen Fritted glass

Foam

Lecture 7 - Foam Technology 10ACS© 2005

Deep-channel surface viscosimeter

Rotating dish

Channel

Liquid

Fixed inner cylinder

Fixed outer cylinder

Lecture 7 - Foam Technology 11ACS© 2005

Equation of State of Foam

p Pr

− =4σ

VA

r=

6

pV nRT=

pV A nRT+ =23σ

dA V dP= −32σ

Consider a single bubble:

For a sphere:

For an ideal gas:

Combining gives:

Assume this is true for a foam.

The differential form is:

Text p. 297

Lecture 7 - Foam Technology 12ACS© 2005

“Static” Foam Stability

Nishioka & Ross, J. Colloid Interface Sci., 1981, 81(1), 1-7.

A schematic of the apparatus used. The jacketed sample vessel isgraduated for rough estimates of foam volume.

Liquid Gas

Pump

FlowControllers

Humidifier

FoamGenerator

Computer

PressureTransducer

SampleChamber

ReferenceChamber

ThermostatHeat Exchanger

A

B

C

D

E F

Lecture 7 - Foam Technology 13ACS© 2005

Theories of Foam Stability

Why doesn't a foam film fall?•Marangoni effects. Requires slow diffusion of surfactant to stretched surface. Marangoni effects are important in spontaneous healing of thin spots and in foam destruction by antifoaming agents.*

•Fluid viscosity. Especially when high MW materials are present, e.g. gelatin or proteins.

•Surface viscosity.

•Mutual repulsion of electrical double layers.

•Formation of layers of micelles "spacing" the surface apart.

•Formation of liquid crystalline phases in the thin films (originally associated with black films.)

*Explains why foam stability near saturation is often diminished. Above the CMC, the micelles serve as reservoirs for the surfactant.

Lecture 7 - Foam Technology 14ACS© 2005

Air Air-

-

--

--

-

-

+

+

+ +

+

+

+

+

+

-

Electrostatic stabilization of a foam film

Each interface is electrically charged. As the film thins, the repulsion increases.

Lecture 7 - Foam Technology 15ACS© 2005

Liquid crystals stabilize foams

AirAir

Micelle

Liquid crystal

Lecture 7 - Foam Technology 16ACS© 2005

Foaminess and Phase Diagram Isophroic Contours

Text p. 311

Not just solutions of "surfactants" foam.

Partially miscible liquids in multiple components foam near the critical point (two components) or plait point (three or more components.) Surface activity precedes phase separation.

If the separated phase has a lower surface tension, it will be adefoamer.

Lecture 7 - Foam Technology 17ACS© 2005

Ross’ Rule

Text p.126

Capillary effects are dramatic near phase boundaries. “Capillarity has been shown to inhere in multicomponent systems at conditions characterized by certain locations in phase diagrams that display partial miscibilities of two liquid phases.” - Ross’ words Examples: Adsorption precedes precipitation. Foaming can suddenly increase or disappear. Dispersion stability suddenly changes. Surface and interfacial tensions change abruptly near phase boundaries. The number and size of precipitates depend strongly on the position in the phase diagram. Sudden changes in product behavior may indicate some component is near its solubility limit.

Lecture 7 - Foam Technology 18ACS© 2005

Davidson, J.A. J. Colloid Interface Sci, 1981, 81(2), 541.

Foaming of Whiskey

U S P ro o f (6 0 o F )8 0 9 0 1 0 0 1 1 0

Bub

ble

stab

ility

(s)

0

5

1 0

1 5

2 0

2 5

3 0

E th an o l (% w e ig h t)0 .3 3 4 0 .3 7 9 0 .4 2 5 0 .4 7 2

Lecture 7 - Foam Technology 19ACS© 2005

Effect of PDMS Viscosity on Foaming

Centers, Tribology Trans., 1993, 36(3), 381.

At low molecular weight (<250) the polymer is too soluble in the ester to be surface active.

At intermediate molecular weights (ca. 6000) the polymer is less soluble and is surface active and is a profoamer.

At higher molecular weights (>60,000) the polymer is insoluble but spreads on the bubble surface and acts as a foam inhibitor.

l o g ( K i n e t m a t i c v i s c o s i t y ) , m 2 s - 1 @ 2 5 o C

- 7 - 6 - 5 - 4 - 3 - 2 - 1

Foam

fom

ratio

n ra

te (m

L s-1

)

0 . 0

0 . 5

1 . 0

1 . 5

2 . 0

Lecture 7 - Foam Technology 20ACS© 2005

Three Phase Foams

•Foams can also contain powders. A solid with a finite (receding) contact angle will sit at the air/liquid surface. It will move with the bubble - hence flotation. "Collectors" are added to dispersions to dewetparticles.

•Particle may stabilize thin films it they have low contact angles, holding the two interfaces apart.

•The finer the particles, the better the stability; lead, silica, ferric oxide are examples.

Lecture 7 - Foam Technology 21ACS© 2005

Foam Inhibition and Breaking

•Differentiate: Foam inhibition and foam breaking.

•Foam inhibitors - added before foam forms, displace foaming agents, or solubilizing the foaming agents (in micelles)

•Foam breaking - mechanical, shock waves, compression waves,ultrasonics, rotating discs, heating, an electrical spark.

•Antifoams - added to existing foams, in the form of small droplets, which spread on the lamellae, thinning and breaking it.

•Antifoams for lubricating oils - poly(hexadecyl methacrylate) plus glycerol monoricinoleate, potassium oleate, nitro-substituted aliphatic alcohols, metal salts of copolymers of styrene and maleic anhydride. (Bikerman)

Lecture 7 - Foam Technology 22ACS© 2005

Antifoams

(a)

(b)

(c)

(a) Antifoam drop(b) Entering the surface(c ) Leading to rupture of the film.

Lecture 7 - Foam Technology 23ACS© 2005

Antifoams

Air Air

-

-

--

-

-

+

+

+

+

+

+

+

-

With an antifoam on one surface, electrostatic stabilization is lost.

Lecture 7 - Foam Technology 24ACS© 2005

Foams in Industry

Marshmellow - foam formed from egg white, gelatin, and sugar.

Ice cream - refrigerated and aerated at the same time. Ice crystals and fat crystals form the matrix.

Dynamic foams: cakes, sponges, bead, meringes, soufflés. Bubbles change at various stages of preparation.

Foams on drying or stripping, especially in distillation columns. A foam blanket at the surface acts as an insulating layer - causing overheating.

Metallic slags foam probably because of the high viscosity. Cooling stabilizes the foam.

Paper making - Caused by lignin, resin, and fatty acids in wood, sulfate soaps from pitch. Also, sizing materials, dyes, fillers, oxidized starch, proteins, etc act as profoamers.

Beer - foam should not affect taste, but it remains important. Too little, beer looks "flat". Sources of foam: entrained air in the pouring, in the pressurizing, and from dissolved carbon dioxide. Mostly stabilized by proteins. Protein-polysaccharide complexes are especially stabilizing.

Lecture 7 - Foam Technology 25ACS© 2005

Froth floation

From the “Activated Sludge Pages”http://www.scitrav.com/wwater/asp/

Lecture 7 - Foam Technology 26ACS© 2005

Firefighting Foams•Primarily for fire protection in petroleum storage. Airplane fires.

•Foam is made in a self-aspirating branchpipe: high pressure pushes the water + foaming agent down a pipe, aspirating air, foaming because of the turbulence ( about 1mm bubbles) and is thrown from about 15 to 75 m.

•High expansion foams are formed by blowing through a net and laid down by coating.

•Reasons (1) Cools fuel below self-ignition temperature, (2) physically separates fuel and air, (3) dilutes oxygen supply

•Types: (1) Protein foam liquid - solution ofhydrolysed protein, (2) liquid with variousperfluorinated surfactants, (3) mixtures ofperfluorinated surfactants with proteins

Briggs in Prud'homme and Khan, Chapter 12.

http://www.pacificresources.com/ff-fc.html?10744094=Fireclout.html

Lecture 7 - Foam Technology 27ACS© 2005

Foams to Immobilize

• To retard evaporation. Improve insulation.

• For fumigants(toxic to fungi), insecticides, contraceptives, to keep them in place.

• Applying thin layers, such as adhesives or etching formulations, dyes or bleaches

• Capture of aerosols.

• Aqueous foam is an excellent suspending medium for paper fibers.Pseudoplasticity enables dispersion of long fibers. At low shear stress the fibers are "frozen" in position. Enables the use of long fibers which otherwise orient on coating.

•Shaving lather - no known use!

Lecture 7 - Foam Technology 28ACS© 2005

The alveolar surface in the lung

Exerowa and Kruglyakov, p. 753

Lecture 7 - Foam Technology 29ACS© 2005

Foam Technology

Lecture 7 - Foam Technology 30ACS© 2005

Bibliography

• Akers, R.J., Ed. Foams; Academic Press: New York; 1976.• Bikerman, J.J. Foams; Springer-Verlag: New York; 1973.• Boys, C.V. Soap bubbles; Dover Publications: New York; 1959.• Exerowa, D.; Kruglyakov, P.M. Foam and foam films; Elsevier: New

York; 1998.• Isenberg, C. The science of soap films and soap bubbles; Dover

Publications: New York; 1992.• Mysels, K.J.; Shinoda, K.; Frankel, S. Soap films; Pergamon Press:

New York; 1959.• Prud’homme, R.K.; Khan, S.A., Eds. Foams; Marcel Dekker: New York;

1996.• Weaire, D.; Hutzler, S. The physics of foams; Clarendon Press: Oxford;

1999.