Foundations of Colloid Science, Volume 2While Volume I stands as an essentially complete advanced textbook of colloidal science, Volume II extends the material to include important new areas, and develops some of the topics in much greater depth. An introductory chapter on the theory of liquids describes the concept of correlation functions and the use of Fourier transforms to analyse the scattering of light and neutrons by colloidal systems. Absorption is given detailed coverage and a chapter on electrokinetics introduces a new approach to time-dependent processes in the double layer. The principles of double layer theory are also used to review the behavior of thin films and emulsions. A final chapter on the rheology of colloidal suspensions calls on many of the concepts developed earlier to bring some cohesion to this important and rapidly developing field. |
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Page 677
The potential energy of a system of N molecules in a container of volume V
depends on the location of all the molecules and can be written as U ( 11 , 12 , . .
. , ) where ri ( i = 1 , 2 , . . . , N ) denotes the position of the ith molecule . Note that
for ...
The potential energy of a system of N molecules in a container of volume V
depends on the location of all the molecules and can be written as U ( 11 , 12 , . .
. , ) where ri ( i = 1 , 2 , . . . , N ) denotes the position of the ith molecule . Note that
for ...
Page 931
The general expression for the electrostatic interaction energy between two
dissimilar droplets of radius a , and az was given by Hogg et al . ( 1966 ) as (
compare with eqn ( 15 . 2 . 6 ) : V = AEQjQ2 [ yi + y2 ] ( a , + a2 ) 24 . 42 n | 1 + exp
( – KD ) ...
The general expression for the electrostatic interaction energy between two
dissimilar droplets of radius a , and az was given by Hogg et al . ( 1966 ) as (
compare with eqn ( 15 . 2 . 6 ) : V = AEQjQ2 [ yi + y2 ] ( a , + a2 ) 24 . 42 n | 1 + exp
( – KD ) ...
Page 940
For such eddies the viscosity is unimportant ( i . e . they are inviscid flows ) and so
they do not dissipate much energy . They are called ' energy bearing eddies ' and
we will suppose them to be of size le . These larger eddies pass on energy to ...
For such eddies the viscosity is unimportant ( i . e . they are inviscid flows ) and so
they do not dissipate much energy . They are called ' energy bearing eddies ' and
we will suppose them to be of size le . These larger eddies pass on energy to ...
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Contents
Contents of Volume I | 675 |
ADSORPTION FROM SOLUTION | 709 |
THE ELECTROKINETIC EFFECTS 786 13 THE ELECTROKINETIC EFFECTS | 786 |
Copyright | |
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Other editions - View all
Foundations of Colloid Science, Volume 1 Robert J. Hunter,Lee R. White,Derek Y. C. Chan Snippet view - 1987 |
Foundations of Colloid Science, Volume 1 Robert J. Hunter,Lee R. White,Derek Y. C. Chan Snippet view - 1987 |
Common terms and phrases
adsorbed adsorption applied approach approximation assumed average becomes behaviour bulk calculated Chapter charge Chem Colloid interface Sci colloidal component concentration constant correlation corresponding density depends described determined developed direction discussed dispersion distance double layer droplets effect electrical electrokinetic electrolyte emulsion energy equation equilibrium estimate et al example Exercise experimental expression factor field film flow fluid force fraction function given gives groups important increases interaction interface involved ions limit liquid material measured microemulsion molecules Note observed obtained occur pair parameters particles phase positive possible potential present pressure problem procedure radius range reduces referred region result scattering Section separation shear rate shown solution specific spheres stability stress structure surface surface charge surface tension suspension theory thin usually values viscosity volume zero