Abstract
To find the distribution function θ 0 c (α) satisfying the conditions (8.2.24)–(8.2.27) one needs more detailed information on quantities r u , q u . This problem cannot be solved in a general form. Therefore let us consider first of all the case of structureless particles, when θ 0 c (α) should be replaced with θ0(α) and the condition (8.2.27) is absent. One can readily prove that the quasiequilibrium solution meeting (8.2.24) can be presented in the following way
where μ R (β,t) is an arbitrary function having a sense of the chemical potential of the β-th layer, and T = Ts here and below unless otherwise specified.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
Preview
Unable to display preview. Download preview PDF.
Rights and permissions
Copyright information
© 1995 Springer-Verlag Berlin Heidelberg
About this chapter
Cite this chapter
(1995). Equilibrium and Quasiequilibrium Solutions to the LG Model. In: Interaction of Gases with Surfaces. Lecture Notes in Physics Monographs, vol 25. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-49107-1_9
Download citation
DOI: https://doi.org/10.1007/978-3-540-49107-1_9
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-540-58802-3
Online ISBN: 978-3-540-49107-1
eBook Packages: Springer Book Archive