Surface and Interface
surface |
boundary between 2 phases, one of them is in the gaseous state |
interface |
boundary between 2 immiscible phases has context menu |
Types
gas-liquid |
surface tension |
gas-solid |
adsorption |
e.g., antiflatulents |
liquid-liquid |
interfacial tension |
e.g., emulsions |
solid-liquid |
wetting |
e.g., tablets |
Surface tension definition and units
Definition |
Force per unit length that must be applied to counterbalance the net inward pull. |
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the work done to increase the surface area of a mass of liquid by 1 cm2. (Units: erg/cm2) |
Units |
dyne/cm |
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Nm-1 |
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mNm-1 |
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erg/cm2 |
surface tension (γ)
Cohesive |
intermolecular forces between like molecules |
Adhesive |
intermolecular forces between unlike molecules |
inward force |
Molecules of the liquid at the surface exhibit an inward force toward the bulk, therefore contract the surface & pull it towards the inside. |
Net force
Surface molecule |
somewhat down because of the inward force |
Bulk molecule |
zero (cancel each others) |
Examples on ST
1. Water film on hand Water |
2. Water dipping from a tap |
3. Water beading on a leaf |
4. Soap bubbles |
5. Paper clip on water surface |
6. Coin on water surface |
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ST of water
Unit |
73 dyne/cm at 25C |
Why are water droplets spherical? |
High stability, low energy, low SA |
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A sphere has the smallest possible surface area to volume ratio |
Surface free energy |
Surface > Bulk |
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The surface layer of a liquid possesses additional energy as compared to the bulk liquid. This energy increases when the surface of the same mass of liquid increases. |
Cleansing effect between hot and cold water
There is an inverse relation between surface tension & temperature |
1. high temp. |
2. more kinetic energy |
3. weakens cohesion |
4. lower ST, which is defined as specific temp. |
Hot water is better cleaning agent than cold water, because it has lower ST, so can get better into pores and fissures, while cold wate can form only bridges between them |
IT (Interfacial Tension)
Definition |
the force per unit length existing at the interface between two immiscible liquid phases |
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the work required to separate the 2 sections of liquids. |
Unit |
dyne/cm |
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erg/cm2 |
The interfacial tension reflects the interaction between the 2 phases: |
1. high IT |
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2. low molecular interactions |
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3. low adhesive |
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4. high cohesive |
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5. immiscible liquids |
completely miscible |
high interactuins |
immiscible |
low interactions |
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Measurements of ST and IT
1. Capillary rise method |
2. Du Nouy ring method |
3. Wilhelmy plate method |
4. Pendent drop method |
5. Spinning drop method |
6. Bubble pressure method |
1. Capillary rise method
Capillary placed in a liquid contained in a beaker, the liquid generally rises up the tube a certain distance |
liquid rises due to the ST, at some point it will stop due to its weght. so the upwaed movement will be balanced by the downward force of gravity |
ST determined by measuring the rise in the capillary |
ST= 0.5 rhpg |
r = radius, h = hight, p = density, g = gravity |
2. DuNouy ring method
slowly lifting a platinum-irridium ring from the surface of a liquid. |
The force required to detach the ring from the liquid surface is recorded in dynes on a calibrated dial. |
This force is equivalent to the maximum pull exerted on the ring by the surface) |
3. Wilhelmy plate method
a thin plate usually made from glass or platinum-oriented perpendicular to the interface and attached to a scale or balance via a thin metal wire |
The force on the plate due to wetting is measured and used to calculate the surface tension. |
4. Pendant drop method (Drop weight)
A liquid drop hanging on the bottom of a capillary tube starts to fall when the weight of the drop is in an equilibrium state with the surface tension. |
The drop is falling when the weight (mg) is equal to the circumference (2πr) multiplied by the surface tension (σ). |
mg = 2 π r σ |
we can use a reference liquid of known surface tension (mostly using water as a reference) to compare with the liquid which we are interested in |
Methods used to measure IT between 2 liquids
Solid-liquid interface (Contact angle θ)
If a drop of liquid is placed on a flat, smooth, horizontal solid surface, it forms a drop. |
contact angle (θ): drop will exhibit a definite angle against the solid. It’s contact angle (θ): the angle the tangent to the liquid surface makes with the solid surface over which it spreads. |
θ is determined by the interactions across the three interfaces; solid/liquid/gas. |
θ depends on the nature of both the solid surface and the liquid drop. |
θ (range of 0 = 180) |
θ for pure water-pure silver is 90° |
Contact angle differs depending on surface type "even same types of drops” |
θ reflects wetting of the surface |
On contact of a liquid droplet with a surface, the behavior of the liquid drop will depend on the balance between the cohesive forces of the liquid and the adhesive forces with the solid surface. |
If the attractive forces between the liquid & solid exceed the cohesive forces in the liquid drop > low contact angle (α < 90°) > good wetting |
e.g., water drop on glass surface |
High θ = bad wetting |
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