Foundations of Colloid Science, Volume 2 |
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Page 700
13 ) On the other hand , in the limit of large Q , it can be shown from egn ( 11 . 7 .
12 ) that S ( Q ) →1 as Q→ 00 ( 11 . 7 . 14 ) because h ( r ) →0 ( i . e . 8 ( r ) →1 )
as r . Physically we can see how the large Q limit comes about . From eqns ( 11 .
13 ) On the other hand , in the limit of large Q , it can be shown from egn ( 11 . 7 .
12 ) that S ( Q ) →1 as Q→ 00 ( 11 . 7 . 14 ) because h ( r ) →0 ( i . e . 8 ( r ) →1 )
as r . Physically we can see how the large Q limit comes about . From eqns ( 11 .
Page 839
... the colloidal particles themselves . The OCM is thus equivalent to the primitive
model ( PM ) in the limit 820 , and since it is numerically no more difficult to solve
the PM for finite counterions than in this limit ( see , for example , Naegele et al .
... the colloidal particles themselves . The OCM is thus equivalent to the primitive
model ( PM ) in the limit 820 , and since it is numerically no more difficult to solve
the PM for finite counterions than in this limit ( see , for example , Naegele et al .
Page 863
An interesting corollary of this type of experiment is that the absence of
anisotropy in the scattering under shear allows an upper limit to be placed on the
particle anisotropy in the dispersion . This is because , if there is no anisotropy at
a shear ...
An interesting corollary of this type of experiment is that the absence of
anisotropy in the scattering under shear allows an upper limit to be placed on the
particle anisotropy in the dispersion . This is because , if there is no anisotropy at
a shear ...
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Contents
Contents of Volume I | 675 |
ADSORPTION FROM SOLUTION | 709 |
THE STRUCTURE OF CONCENTRATED | 827 |
Copyright | |
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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 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 temperature theory thin usually values viscosity volume zero