## 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 794

situation is a formidable problem, thanks to the presence of the non-

njV and tijVxp. To overcome this problem we consider systems which are only

slightly disturbed from the equilibrium state; these terms can then be

approximated ...

situation is a formidable problem, thanks to the presence of the non-

**linear*** termsnjV and tijVxp. To overcome this problem we consider systems which are only

slightly disturbed from the equilibrium state; these terms can then be

approximated ...

Page 818

Since the governing equations are

fields, one due to En and the other due to E±. From the geometry of the problem it

follows that the component of <5t//(r) due to E± is zero/ and thus: 6>(r) = A(r)En ...

Since the governing equations are

**linear**, we may regard £ V as the sum of twofields, one due to En and the other due to E±. From the geometry of the problem it

follows that the component of <5t//(r) due to E± is zero/ and thus: 6>(r) = A(r)En ...

Page 1018

(The data in the

against Sfb (=T0/2nRlL) and determining the slope (which is t/pl).) 18.5.5 For the

power law fluid: in a coaxial cylinder viscometer we have T„ = Snnr2L ,*,(- r^jlnfL.

(The data in the

**linear**regime (where 7i«Q is treated by plotting this function yagainst Sfb (=T0/2nRlL) and determining the slope (which is t/pl).) 18.5.5 For the

power law fluid: in a coaxial cylinder viscometer we have T„ = Snnr2L ,*,(- r^jlnfL.

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### Contents

INTRODUCTION TO STATISTICAL MECHANICS | 675 |

ADSORPTION FROM SOLUTION | 709 |

THE ELECTROKINETIC EFFECTS | 786 |

Copyright | |

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adsorbed adsorption approximation assumed average behaviour bulk calculated Chapter Chem co-surfactant coagulation coalescence Colloid interface Sci colloidal dispersion colloidal particles compare with eqn component constant correlation function corresponding counterions diameter diffuse dilute double layer droplets effect electrical electrokinetic electrolyte electrostatic emulsion equilibrium Establish eqn estimate Exercise experimental Faraday ferrofluid field film flow fluid force free energy given hard sphere head group Hunter hydrophilic increases interaction ion density latex linear liquid magnetic measured micelles microemulsion molecules neutron Newtonian fluid non-ionic surfactant Note obtained occur Ottewill Overbeek pair parameters phase Phys plane polymer potential potential determining ions pressure procedure pseudoplastic radius region repulsion result scattering shear rate shear stress shown in Fig solution specific adsorption spherical stability surface charge surfactant suspension temperature thermodynamic thin thixotropic values velocity visco-elastic viscometer viscosity volume fraction Waals zero