Introduction to Dispersed Systems FDSC400 09/28/2001.

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Introduction to Dispersed Systems FDSC400 09/28/2001

Transcript of Introduction to Dispersed Systems FDSC400 09/28/2001.

Page 1: Introduction to Dispersed Systems FDSC400 09/28/2001.

Introduction to Dispersed Systems

FDSC400

09/28/2001

Page 2: Introduction to Dispersed Systems FDSC400 09/28/2001.

Goals

• Scales and Types of Structure in Food

• Surface Tension

• Curved Surfaces

• Surface Active Materials

• Charged Surfaces

Page 3: Introduction to Dispersed Systems FDSC400 09/28/2001.

COLLOIDAL SCALE

Page 4: Introduction to Dispersed Systems FDSC400 09/28/2001.

Dispersed Systems

A kinetically stable mixture of one phase in another largely

immiscible phase. Usually at least one length scale is in the

colloidal range.

Page 5: Introduction to Dispersed Systems FDSC400 09/28/2001.

Dispersed Systems

Dispersed phase

Continuous phase

Interface

Page 6: Introduction to Dispersed Systems FDSC400 09/28/2001.

Solid Liquid Gas

Solid Some glasses

Sol Smoke

Liquid Emulsion Aerosol

Gas Solid foam

Foam

Dis

pers

ed p

hase

Continuous phase

Page 7: Introduction to Dispersed Systems FDSC400 09/28/2001.

Properties of Dispersed Systems

• Too small to see

• Affected by both gravitational forces and thermal diffusion

• Large interfacial area– SURFACE EFFECTS ARE IMPORTANT

Page 8: Introduction to Dispersed Systems FDSC400 09/28/2001.

Increased Surface Area

The same oil is split into 0.1 cm radius droplets, each has a volume of 0.004 cm3 and a surface area 0.125 cm2.

As we need about 5000 droplets we would have a total area of 625 cm2

We have 20 cm3 of oil in 1 cm radius droplets. Each has a volume of (4/3..r3) 5.5 cm3

and a surface area of (4..r2) 12.5 cm2.As we need about 3.6 droplets we would have a total area of 45.5 cm2

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For a Fixed COMPOSITION

• Decrease size, increase number of particles

• Increase AREA of interfacial contact

decrease area

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Tendency to break

• LYOPHOBIC• Weak interfacial

tension• Little to be gained by

breaking• e.g., gums

• LYOPHILIC• Strong interfacial

tension• Strong energetic

pressure to reduce area• e.g., emulsions

Page 11: Introduction to Dispersed Systems FDSC400 09/28/2001.

Surface Tension-molecular scale-

Page 12: Introduction to Dispersed Systems FDSC400 09/28/2001.

Surface Tension-bulk scale-

Area, A

Force,

Inte

rfac

ial e

nerg

y

Interfacial area

Slope

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Curved Surface

Highly curved surface

Slightly curved surface

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Curved Surfaces

Molecules at highly deformed surfaces are less well anchored into their phase

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Laplace Pressure

Surface pressure pulls inwards increasing pressure on dispersed phase pressure

rPL

2

Increased pressure

Surface tension

radius

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Curved Surfaces -Consequences-

• Dispersed phase structures tend to be round

• Small fluid droplets behave as hard spheres

• Solubility increases with pressure so…

• Large droplets may grow at the expense of small (Ostwald ripening)– Depends on the solubility of the dispersed

phase in the continuous

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Surface Active Material

• Types of surfactant

• Surface accumulation

• Surface tension lowering

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Types of Surfactant-small molecule-

Hydrophilic head group (charged or polar)

Hydrophobic tail (non-polar)

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Types of Surfactant-polymeric-

Polymer backbone

Sequence of more water soluble subunits

Sequence of less water soluble subunits

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Surface Binding

Equilibrium

ENTHALPY COST ENTROPY COST

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Surface Binding Isotherm

ln Bulk concentration

Sur

face

con

cent

rati

on /m

g m

-2

Surface saturation

No binding below a certain concentration

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Surface Tension Lowering

Bare surface (tension 0)

Interface partly “hidden”(tension )

Surface pressure – the ability of a surfactant to lower surface tension