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 542
... problem is linear , we can write S as the sum of a dipole strength due to the rigid body velocity field , plus a dipole strength due to the portion of the ambient field ( 9.10.11 ) Since there is no force or torque on the particle , it ...
... problem is linear , we can write S as the sum of a dipole strength due to the rigid body velocity field , plus a dipole strength due to the portion of the ambient field ( 9.10.11 ) Since there is no force or torque on the particle , it ...
Page 543
... problem will exhibit less interaction than in the sedimentation problem , and our dilute approximation should , therefore , be valid for a greater concentration range than in the sedimentation problem . For a rigid particle , the ...
... problem will exhibit less interaction than in the sedimentation problem , and our dilute approximation should , therefore , be valid for a greater concentration range than in the sedimentation problem . For a rigid particle , the ...
Page 557
... problem was given by Smoluchowski ( 1921 ) for the κa >> 1 ( thin double - layer ) case . Smoluchowski reasoned that the problem of determining the local flow in the double layer in this case is the same as the electro - osmosis problem ...
... problem was given by Smoluchowski ( 1921 ) for the κa >> 1 ( thin double - layer ) case . Smoluchowski reasoned that the problem of determining the local flow in the double layer in this case is the same as the electro - osmosis problem ...
Contents
CHARACTERIZATION OF COLLOIDAL | 2 |
BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |
PARTICLE SIZE AND SHAPE | 104 |
Copyright | |
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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