Foundations of Colloid Science, Volume 2Clarendon Press, 1987 - Colloids |
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Page 829
... becomes stronger . In a stable colloid , the thermal energy of the particles will stop them from coagulating , despite this ' stickness ' , by breaking up pairs before they have time to become clusters . If the potential is sufficiently ...
... becomes stronger . In a stable colloid , the thermal energy of the particles will stop them from coagulating , despite this ' stickness ' , by breaking up pairs before they have time to become clusters . If the potential is sufficiently ...
Page 856
... becomes increasingly attractive as the temperature is raised . Reference to eqn ( 14.4.3 ) shows that the scattering at high Q will become the same as that from a non - interacting system , since S ( Q ) then tends to unity ; this is ...
... becomes increasingly attractive as the temperature is raised . Reference to eqn ( 14.4.3 ) shows that the scattering at high Q will become the same as that from a non - interacting system , since S ( Q ) then tends to unity ; this is ...
Page 1017
... becomes too high . Just as the flow in a pipe becomes turbulent if the Reynolds number ( Re ) ( Section 9.8.1 ) exceeds about 2000 , so too does it become turbulent in a Couette viscometer when Re exceeds a certain figure ( Exercise ...
... becomes too high . Just as the flow in a pipe becomes turbulent if the Reynolds number ( Re ) ( Section 9.8.1 ) exceeds about 2000 , so too does it become turbulent in a Couette viscometer when Re exceeds a certain figure ( Exercise ...
Contents
Contents of Volume I ix | 675 |
ADSORPTION FROM SOLUTION | 709 |
CHARACTERIZATION OF COLLOIDAL DISPERSIONS 1 | 710 |
Copyright | |
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Foundations of Colloid Science. Vol. 1-2. Collab. Lee R. White, Leonard R ... No preview available - 1992 |
Common terms and phrases
adsorbed adsorption approximation assumed behaviour bulk C-potential calculated Chapter Chem co-surfactant coagulation coalescence Colloid interface Sci colloidal dispersions compare with eqn component constant corresponding counterions diffuse dilute double layer droplets effect electrical electrokinetic electrolyte electrolyte concentration electrostatic emulsion equilibrium Establish eqn estimate Exercise experimental Faraday ferrofluid field film flow fluid force free energy given hard sphere head group Hunter hydrophilic increases interaction K₁ latex liquid measured micelles microemulsion molecules neutron neutron scattering Newtonian fluid non-ionic surfactant Note obtained occur Ottewill Overbeek parameters particles phase Phys Poisson-Boltzmann equation polymer potential potential determining ions pressure procedure pseudoplastic radius region repulsion result scattering shear rate shear stress shown in Fig solution specific adsorption spherical stability structure surface charge surfactant suspension temperature thermodynamic thin thixotropic values velocity visco-elastic viscometer viscosity volume fraction Waals zero