Foundations of Colloid Science, Volume 1Liquid suspension systems are the basic ingredients of paints, detergents, biological cells, and countless other systems of scientific and technological importance. This book presents the fundamental physical and chemical concepts necessary to the understanding of these systems and of colloid science in general. New ideas are introduced carefully and formulae are developed in full, with exercises to help the reader throughout. The frequent references to the many applications of colloid science will be especially helpful to beginning research scientists and people in industry, medicine and agriculture who often find their training in this area inadequate. Integrating developments from the time of colloid science's infancy forty years ago to its present state as a rigorous discipline, this intelligently assembled work elucidates a remarkable range of concepts, techniques, and behaviors. |
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Page 3
... example , Evans and Langdon 1976 ) . Likewise , dispersions of solids and liquids in gases will not be treated in Table 1.1 The various types of colloidal dispersion with some common examples . The nomenclature is adapted from Ostwald ...
... example , Evans and Langdon 1976 ) . Likewise , dispersions of solids and liquids in gases will not be treated in Table 1.1 The various types of colloidal dispersion with some common examples . The nomenclature is adapted from Ostwald ...
Page 421
... example , give the ratio ( for z = 1 , 2 , and 3 ) : 50 : 0.7 0.091 : 0.014 : 0.0018 compared to the ' theoretical ' 1 : 0.016 : 0.0014 . Although this agreement is impressive there is some doubt as to its significance . For one thing ...
... example , give the ratio ( for z = 1 , 2 , and 3 ) : 50 : 0.7 0.091 : 0.014 : 0.0018 compared to the ' theoretical ' 1 : 0.016 : 0.0014 . Although this agreement is impressive there is some doubt as to its significance . For one thing ...
Page 640
... example , to use the CGS system , we see from eqn ( A4.2 ) that the units to be assigned to ( 4л ) must be ( statcoulomb ) 2 cm2 dyne1 or ( statcoulomb ) 2 cm ̄1 erg1 , since an erg is a dyne cm . But 1 erg = 1 statcoulomb × 1 statvolt ...
... example , to use the CGS system , we see from eqn ( A4.2 ) that the units to be assigned to ( 4л ) must be ( statcoulomb ) 2 cm2 dyne1 or ( statcoulomb ) 2 cm ̄1 erg1 , since an erg is a dyne cm . But 1 erg = 1 statcoulomb × 1 statvolt ...
Contents
CHARACTERIZATION OF COLLOIDAL | 2 |
BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |
PARTICLE SIZE AND SHAPE | 104 |
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adsorbed adsorption aggregation approximation aqueous assumed behaviour Brownian motion bulk calculated capillary chemical chemical potential coagulation coefficient Colloid interface Sci colloid science colloidal dispersions colloidal particles component constant contact angle crystal curvature curve density determined dielectric diffuse dipole distance distribution DLVO theory double layer droplet effect electrolyte electron electrostatic enthalpic entropy equation equilibrium Establish eqn Exercise experimental flocculation flow fluid force formula free energy frequency function given head group hydrocarbon interaction energy ions liquid material measured method micelle microscope molar mass molecular molecules monomer negative Note obtained occurs Overbeek phase plates polymer potential energy procedure quantity R₁ radius region repulsion result scattering sedimentation separation shear silver iodide solid solution solvent spheres spherical stabilizing moieties steric stabilization stress surface tension surfactant suspension temperature term theory thermodynamic vector velocity viscosity volume Waals x₁ Young-Laplace equation zero