## 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 40 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 205

Note that the velocity of light in vacuo is

result we will use later . Thus modern dispersion force theory starts with the

concept of a randomly fluctuating electromagnetic field pervading the material

system .

Note that the velocity of light in vacuo is

**given**by c = = ( EoMo ) -112 ( 4.7.23 ) aresult we will use later . Thus modern dispersion force theory starts with the

concept of a randomly fluctuating electromagnetic field pervading the material

system .

Page 404

10 ) from the midplane where X = 0 and Q = 0 to obtain corresponding values of

Q and X. When Q reaches the value ls , the corresponding X value corresponds ...

**Given**any arbitrary ym ( with lym < lyl ) one can integrate ( numerically ) eqn ( 7.3.10 ) from the midplane where X = 0 and Q = 0 to obtain corresponding values of

Q and X. When Q reaches the value ls , the corresponding X value corresponds ...

Page 515

and að = - = -ê дө ( see Exercise 9.7.1 ) , we find the local Cartesian components

of Av are

the rate of strain tensor , we see that the only non - zero components of eat 0 are

...

and að = - = -ê дө ( see Exercise 9.7.1 ) , we find the local Cartesian components

of Av are

**given**by Δυ , = Vo X2 and du Δυ , = X1 dr From the formula ( 9.5.9 ) forthe rate of strain tensor , we see that the only non - zero components of eat 0 are

...

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### Contents

CHARACTERIZATION OF COLLOIDAL | 2 |

BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |

PARTICLE SIZE AND SHAPE | 104 |

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 |

### Common terms and phrases

adsorbed adsorption angle applied approach approximation assumed becomes behaviour body bulk calculated called Chapter charge chemical coagulation colloidal compared component concentration Consider constant corresponding curve density depends described determined diffuse dipole discussion dispersion distance distribution double layer effect electric electrolyte electron equal equation equilibrium Establish estimate Exercise experimental expression field flocculation flow fluid follows force free energy frequency function given gives important increase integral interaction interface ions layer light limit liquid material mean measured method micelle molecules motion negative Note obtained occurs particles phase plates polymer positive possible potential presence pressure problem procedure quantity radius range referred region relation relative result scattering separation shape shear shown simple solid solution solvent stabilization stress surface surface tension suspension Table temperature tension term theory unit usually volume zero