2: Colloidal Particles and Suspensions

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colloidal particle
an entity large in comparison with atomic dimensions so as to have a supramolecular structure and properties, but small enough to remain in suspension for a finite amount of time (at least of the order of hours) when dispersed in a liquid medium such as water
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size range of colloidal particles
approximately 1 nm to 10 μm
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soil classifications in which particles have potential to be colloidal
clay fraction and fine silt fraction
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clay fraction
fraction of soil with particle size less than 2 μm
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fine silt fraction
fraction of soil with particle size 2–10 μm
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components of soil colloids
clay minerals, oxides, organic matter (humic substances)
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the location at which many important chemical and physical processes take place
the surface of soil colloids
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colloidal suspension
a dispersion of colloidal particles in the bulk of another phase, usually in a different aggregation state, most commonly solid particles in a liquid medium
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solubility of colloidal particles
macromolecules may be soluble in the liquid medium (e.g., proteins in water); oxide particles will not be soluble
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phase boundaries of solutions and suspensions
solution has no phase boundary; a true suspension has phase boundary
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stability of solutions and suspensions
a solution can be thermodynamically stable; a suspension can be kinetically stable
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tendency of dispersed particles of the same material
aggregate, condense, aggregate, condense
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aggregating process (flocculation)
the process in which individual particles bind into clusters by intermolecular forces
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condensing process
the process in which aggregated clusters sediment into larger particles, losing their former identity
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kinetic stability
stability due to relatively slow motion of particles, in many cases due to energetic barriers (usually electrostatic); may last for many years
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kinetic and thermodynamic stability requirements
kinetic stability may be broken by addition of an indifferent electrolyte; thermodynamic stability may be broken by modifying thermodynamic variables, such as temperature
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solid-liquid interaction classifications
lyophobic, lyophilic
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lyophobic solid-liquid interaction classification
a solid-liquid system in which particles have low affinity for the dispersing medium
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lyophilic solid-liquid interaction classification
a solid-liquid system in which colloidal particles have great solvent affinity for the dispersing medium
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hydrophobic, hydrophilic
solid-liquid interaction classifications in which the dispersing medium is water
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sol
a hydrophobic suspension
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examples of substances that particles can form sols
AgI, Au, clays, crystalline oxides (e.g., hematite, gibbsite)
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influence of particle size on suspension appearance
nanoparticles can be invisible to the naked eye but revealed by Tyndall effect (dispersion of light); larger particles, e.g., those found in soil, usually give a milky appearance
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substances that particles can form hydrophilic suspensions
hydrous (oxo) hydroxides, e.g., Fe(OH)3 and Al(OH)3
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main difference between hydrophobic and hydrophilic colloids
hydrophobic colloids aggregate but in aggregation, the individual particles are preserved and can be redispersed (peptized) by replacing the electrolytic solution by water or a more diluted solution; hydrophilic colloids in many cases do not show coagulation and may be at borderline between suspensions and true solutions
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motion of colloidal particles in dispersed medium
individual particles can be observed subject to thermal (Brownian) motion, but upon coagulation they cluster to form larger aggregates that precipitate relatively quickly
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specific surface area (As)
area per unit mass (m^2/kg)
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material properties upon which specific surface area depends
particle size, surface roughness
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importance of surface roughness
actual particles, especially those found in natural environments, do not have perfectly flat surfaces but display defects and irregularities that increase the total area exposed to the surrounding phase
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surface Gibbs free energy
the reversible work per unit area (J/m^2) to increase the surface (e.g., change the shape of the phase)
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the concept of surface energy
when a molecule, immersed in the bulk of a condensed phase, is brought to the surface in the presence of a dilute gas or vacuum, attractive forces in the direction normal to the surface are missing, so that a net work should be done (the surface Gibbs free energy)
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surface tension
(N/m) the interpretation of surface energy as the force that should be applied to "stretch" the surface linearly a unit length in any direction
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interfacial free energy (interfacial tension)
the Gibbs free energy needed to expand the surface per unit area when the condensed phase is in contact with another solid or liquid phase
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definition of Gibbs free energy
$δW = γ_{AB} dA$
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amphipathic molecule
a molecule composed by a nonpolar part (usually a long aliphatic chain) and a polar part (either an ionizable group, such as sulfate or phosphate, or a highly hydrophilic group, such as a polyethylene oxide chain)
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important physicochemical properties across interfaces
concentrations, chemical potentials of the different species, electrostatic potential, entropy
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physicochemical properties across interfaces as a function of distance
they should not change abruptly at the interface because they, and in most cases their derivatives, should be defined everywhere
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interfacial region
the region about the interface across which physicochemical properties change
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Gibbs plane
a plane placed at an arbitrary location in the interfacial region at which accumulation or depletion of chemical species (as well as extensive properties such as entropy) can be measured relative to the bulk of each phase
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surface excess
$Γ_i=\frac{n_{i+}-n_{i-}}{A}$, (mol/area) "the amount of solute adsorbed at the surface"
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relative surface excess
surface excess defined in with respect to a datum: when one of the phases is a solution, especially an aqueous solution, usually the solvent is set to have zero surface excess by special placement of the Gibbs plane
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Gibbs equation
$dγ = -\sum_i Γ_i dμ_i$
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context of the Gibbs equation
since surface tension cannot be measured when dealing with solids, the Gibbs equation is more useful when dealing with interfaces not involving solid phases
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chemical potential of a solute
$\mu_i=\mu^0_i+RT \ln{a_i}$
where $\mu^0_i$ is the standard chemical potential, $a_i$ is the solute activity
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behavior of uncharged, poorly hydrated organic solutes in water
they show tendency to accumulate at the surface due to polarity reasons, giving a positive surface excess
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behavior of electrolytes and highly hydrated organic compounds in water
due to polarity effects, they dislike the surface and thus show negative surface excess (surface depletion or negative adsorption)
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behavior of amphipathic species in water
the surface is saturated with this solute even at very low concentrations; after a particular temperature-dependent concentration value, there is almost no surface excess of this solute
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micelle
• a structure, or cluster, in which amphipathic molecules group together with the nonpolar tails directed toward the interior and the polar heads in the exterior part in contact with water
• usually of colloidal size and display most colloidal properties
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critical micellar concentration
the concentration threshold at which the surface excess vanishes, indicating micelle formation
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properties upon which critical micellar concentration depends
the particular substance, temperature, ion strength
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micelle capabilities
micelles can dissolve nonpolar compounds in the inner part and also can interact with ions and polar molecules at the surface
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presence of amphipathic compounds and micelles in the natural environment
amphipathic compounds and, eventually, micelles are usually not found in natural soils, but can be present as a consequence of human activity, such as detergent spillage
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