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 40 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 191
Under these circumstances, a very useful approximate expression for the
interaction energy of the bodies can be derived from the corresponding
interaction energy per unit area of plane parallel half-spaces. The approximation
is due, ...
Under these circumstances, a very useful approximate expression for the
interaction energy of the bodies can be derived from the corresponding
interaction energy per unit area of plane parallel half-spaces. The approximation
is due, ...
Page 235
5.2.3) there are fewer and fewer pairs of molecules attracting across the test
plane as the centre of the sphere approaches the surface and hence the
magnitude of the static pressure contribution decreases for both the pressure
across a plane ...
5.2.3) there are fewer and fewer pairs of molecules attracting across the test
plane as the centre of the sphere approaches the surface and hence the
magnitude of the static pressure contribution decreases for both the pressure
across a plane ...
Page 339
The plane where the diffuse layer begins (at x = d) is called the outer Helmholtz
plane (OHP) and additional adsorbed charge is assumed to be confined to
another plar- called the inner Helmholtz plane (IHP). At the mercury-aqueous
solution ...
The plane where the diffuse layer begins (at x = d) is called the outer Helmholtz
plane (OHP) and additional adsorbed charge is assumed to be confined to
another plar- called the inner Helmholtz plane (IHP). At the mercury-aqueous
solution ...
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Contents
CHARACTERIZATION OF COLLOIDAL | 2 |
Classification of colloids | 6 |
BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |
Copyright | |
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adsorbed adsorption aggregation approximation aqueous assumed behaviour Brownian Brownian motion bulk calculated capillary Chapter charge chemical chemical potential coagulation coefficient Colloid interface Sci colloid science colloidal dispersions colloidal particles component constant contact angle crystal curvature curve density determined diameter dielectric diffuse dipole distance distribution double layer droplet effect electrolyte electrolyte concentration electron electrostatic entropy equilibrium Establish eqn Exercise experimental flocculation flow fluid force free energy frequency function given hydrocarbon integral interaction energy ions Kelvin equation liquid material measured membrane mercury method micelle microscope molar mass molecular molecules negative Note obtained occurs Overbeek phase plane plates polymer procedure quantity radius region repulsion result sedimentation separation shear shown in Fig silver iodide solid solution solvent spheres spherical steric stabilization stress surface tension surfactant suspension temperature term theory thermodynamic vapour pressure vector velocity viscosity volume Waals Young-Laplace equation zero