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Interfacial Transport Phenomena 2nd ed - John C Slattery, Leonard Sagis, Eun-Suok Oh (Springer, 2007) pdf

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Description

 							
  
  ISBN 0-387-38438-3

  e-ISBN 0-387-38442-1
  ISBN 9780387384382
  
  Transport phenomena is used here to describe
momentuin, energy, mass, and entropy transfer [1, 2]. It includes thermodynamics, a special case of which is
thermosiaiics. Interfacial transport phenomena refers to momentum, energy, mass, and entropy transfer within the
immediate neighborhood of a phase interface, including the thermodynamics of the interface. In terms of qualitative
physical observations, this is a very old field. Pliny the Elder (Gains Plinius Secundus, 23-79 A. D.; Pliny [3])
described divers who released small quantities of oil from their mouths, in order to damp capillary ripples on the ocean
surface and in this way provide more uniform lighting for their work. Similar stories were retold by Benjamin Franklin,
who conducted experiments of his own in England [4]. In terms of analysis, this is a generally young field. Surface
thermostat ics developed relatively early, starting with Gibbs [5] and continuing with important contributions by many
others (see Chap. 4). Derjaguin and Lan dau [6] and Verwey and Overbeek [7] indicated how London-van der Waals and
electrostatic double-layer forces were to be incorporated in continuum mechanics, now often referred to as DLVO theory.
But prior to 1960, there were relatively few notable papers concerned with the analysis of dynamic systems. Two stand
out in my mind. Boussinesq [8] recognized the surface stress tensor and proposed the constitutive equation that we now
refer to as the Boussinesq surface fluid model (Sect. 4. 9. 5)." 						

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