## 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 32

1.5.5 A kaolinite sample is found to have a surface area of 15m2g"\

that the particles are cylindrical discs of density 2.8 gcm13 and aspect ratio 10:1,

estimate the average radius. (This is called the area average size (section 3.3)).

1.5.5 A kaolinite sample is found to have a surface area of 15m2g"\

**Assuming**that the particles are cylindrical discs of density 2.8 gcm13 and aspect ratio 10:1,

estimate the average radius. (This is called the area average size (section 3.3)).

Page 330

This is a reasonable

>M(=<t>2) and for x > 0 it is determined by the Poisson equation (see appendix 3

for a discussion of the meaning of this equation): div D = div eE = p (6.3.1) ...

This is a reasonable

**assumption**for a metal. The potential at the plane x = 0 is <t>M(=<t>2) and for x > 0 it is determined by the Poisson equation (see appendix 3

for a discussion of the meaning of this equation): div D = div eE = p (6.3.1) ...

Page 361

... have ^e(w) + RT In a'(Ag+)w = jue(c) + RT In a'(Ag+)c + 9 A^dipoie (6.7.3)

where (') refers to quantities measured at the point of zero charge and it is

remains.

... have ^e(w) + RT In a'(Ag+)w = jue(c) + RT In a'(Ag+)c + 9 A^dipoie (6.7.3)

where (') refers to quantities measured at the point of zero charge and it is

**assumed**that at that point only the chi-(dipole)-potential difference (section 6.2)remains.

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### Contents

CHARACTERIZATION OF COLLOIDAL | 1 |

BEHAVIOUR OF COLLOIDAL DISPERSIONS | 49 |

Electrical charge and colloid stability | 89 |

Copyright | |

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