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 99
... force might be of the nature of a van der Waals or London force , similar to that occurring between atoms and molecules , and responsible for the condensation of gases into liquids . Such a force is certainly general enough — it occurs ...
... force might be of the nature of a van der Waals or London force , similar to that occurring between atoms and molecules , and responsible for the condensation of gases into liquids . Such a force is certainly general enough — it occurs ...
Page 510
... force on the top of the block is n ( 2012 ) Əx2x2 + Ax2 ê1Ax1Ax3 . Evaluating the force on the bottom of the block and then subtracting , we find that the net force per unit volume is 22v1 n ê1 , Əx2 a result which is consistent with ...
... force on the top of the block is n ( 2012 ) Əx2x2 + Ax2 ê1Ax1Ax3 . Evaluating the force on the bottom of the block and then subtracting , we find that the net force per unit volume is 22v1 n ê1 , Əx2 a result which is consistent with ...
Page 511
... force in the x1 direction is , per unit volume : nv2v1ê , with similar results for the x2 and x3 directions . In addition to the pressure gradient and the viscous force there will also be a contribution from the long - range forces . We ...
... force in the x1 direction is , per unit volume : nv2v1ê , with similar results for the x2 and x3 directions . In addition to the pressure gradient and the viscous force there will also be a contribution from the long - range forces . We ...
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