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 258
... components , R the number of chemical reactions between components , P the number of phases , the number of surface phases and S the number of surfaces . Assuming = ( the usual case ) and R = 0 we have , for two phases in contact : f ...
... components , R the number of chemical reactions between components , P the number of phases , the number of surface phases and S the number of surfaces . Assuming = ( the usual case ) and R = 0 we have , for two phases in contact : f ...
Page 500
... components of a stress tensort , denoted by σ . The expression ( 9.3.5 ) is formally written in terms of σ as S ( x , î ) = σ ( x ) · î . ( 9.3.8 ) It is customary to write the components of the stress tensor in the † In mathematical ...
... components of a stress tensort , denoted by σ . The expression ( 9.3.5 ) is formally written in terms of σ as S ( x , î ) = σ ( x ) · î . ( 9.3.8 ) It is customary to write the components of the stress tensor in the † In mathematical ...
Page 507
... components of e we can write the expression ( 9.5.3 ) for the relative velocity in the component form 3 3 v , ( x + Ax ) = v , ( x ) + 1 Σ ( 3U ; _ 3v ) Ov1 ) Ax , + Σ e ,, Ax ,, j = 1 e¡¡Ax ;, ( 9.5.13 ) where e , is evaluated at the ...
... components of e we can write the expression ( 9.5.3 ) for the relative velocity in the component form 3 3 v , ( x + Ax ) = v , ( x ) + 1 Σ ( 3U ; _ 3v ) Ov1 ) Ax , + Σ e ,, Ax ,, j = 1 e¡¡Ax ;, ( 9.5.13 ) where e , is evaluated at the ...
Contents
CHARACTERIZATION OF COLLOIDAL | 1 |
BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |
PARTICLE SIZE AND SHAPE | 104 |
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