Surface and Interface Chemistry Thermodynamics of Surfaces (LG and LL Interfaces) Valentim M. B....
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![Page 1: Surface and Interface Chemistry Thermodynamics of Surfaces (LG and LL Interfaces) Valentim M. B. Nunes Engineering Unit of IPT 2014.](https://reader035.fdocuments.us/reader035/viewer/2022070412/56649d705503460f94a529ea/html5/thumbnails/1.jpg)
Surface and Interface Chemistry
Thermodynamics of Surfaces(LG and LL Interfaces)
Valentim M. B. Nunes
Engineering Unit of IPT
2014
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Adsorption in liquid surfaces
Certain materials, such as fatty acids or alcohols, are soluble in water or in (e.g.) hydrocarbons. The nonpolar part is responsible for the solubility in "oil" and the polar part (-OH or -COOH) by solubility in water (Intermolecular forces).
C2H5COOHC3H7COOHC4H9COOH
Hydrophobic partHydrophilic part
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Adsorption of molecules occurs (surfactants) in water-oil or water-air interfaces.
ar
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The solutes that decrease the surface tension of a solvent are positively adsorbed in the interface, and the surface layers are enriched of solute.
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The solutes that increase surface tension tend to stay within the solution (e.g. Ionic salts) and are adsorbed negatively in the interface.
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The adsorption on solutions does not conduct in general to more than monolayers. The molecules that have a pronounced effect on surface tension are designated surfactants or surfactants.
If the surface tension between two liquids is sufficiently reduced by the addition of surfactants it may form micro emulsions.
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The thermodynamic treatment of Gibbs allows the estimation of the adsorption on a liquid surface from the surface tension.
Since the interface is a material system, with a given volume, they thermodynamic properties can be calculated.
GIBBS ADSORPTION ISOTHERM.
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Let us consider a binary mixture containing ni moles of each component, and two homogeneous phases α and β, separated by an arbitrarily located interface.
A
nii
Surface excess concentration.
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From the laws of Thermodynamics:
iiii
ii
ii
i
dndnAddAdpVpdVdTSTdSdU
nApVTSU
The combination of the 1st and 2nd laws gives:
ii
idndApdVTdSdU
0 ii
i dnAddpVdTS
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At constant p and T, we have:
iiii ddA
nd
For a binary mixture (solvent + solute):
BBAA ddd
Considering A = 0,
BBdd
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BB
BBB
aRTdd
aRT
ln
ln
Introducing the chemical potential,
We finally obtain:
BB aRT ln
1
And for dilute solutions:
B
BB cRT
c
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B
BB cRT
c
Gibbs Isotherm
AmáxBB NA
,
1
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Monolayers
Pockels and Rayleigh (1899): some poorly soluble substances spread on the surface to form films with thickness of a molecule monolayers
This superficial film causes a lowering of the surface tension. It is determined by measuring the force, f, exerted in a calculated barrier to separate the region with film of the pure liquid.
gas
liquid
liquid + film
0f
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Considering now, kc 0
RTRT
kc
0
Designating the difference of surface tensions 0 - by superficial pressure, , so that = 0 - , we obtain:
RTA
ni
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Rearranging: RTnA iDividing both members of equation by the Avogadro constant:
TkA Bm The isothermal for the monolayer has the meaning of an equation of state (note the similarity to the equation of State of a perfect gas: pV = nRT)
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The type of isotherms (,Am) depends on the compounds structure.
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Materials with large surface activity tend to form micelles. The concentration from which the micelles are formed is called critical micelle concentration (c.m.c.)
concentrationc.m.c.
0~c
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Surfactants forming micelles exhibit a solubility increase above a certain temperature – kraft point. This is due to the high solubility of the micelles. At temperatures below kraft point, the solubility of the surfactant is insufficient to form micelles.
Nº de átomos de carbono 10 12 14 16 18
Temperatura kraft / ºC 8 16 30 45 56
Kraft points for sodium alkyl sulfates
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Spreading
The work or energy of adhesion between two immiscible liquids is equal to the work necessary to separate a unit area of the liquid/liquid interface. By the Dupré equation:
aW
For the cohesion work:
2cW
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Let us consider a drop of oil over water:
oilAW
OA
OW
air
water
We define the initial spreading coefficient in the following way:
OWOAWAS
The spreading occurs if S 0. Replacing in the Dupré equation we obtain:
óleoOW WWS