Analytical Proof That There is no Effect of Confinement or Curvature on the Maxwell–Boltzmann Collision Frequency

[1]  J. Elliott,et al.  Particle trapping and banding in rapid colloidal solidification. , 2011, Physical review letters.

[2]  F. Gebhard,et al.  Relaxation of ideal classical particles in a one‐dimensional box , 2011, 1106.5344.

[3]  J. Beck.  Deterministic Approach to the Kinetic Theory of Gases , 2010 .

[4]  J. Elliott,et al.  Nonideal statistical rate theory formulation to predict evaporation rates from equations of state. , 2008, The journal of physical chemistry. B.

[5]  C. A. Ward,et al.  Kinetics of Evaporation: Statistical Rate Theory Approach , 2005 .

[6]  Ward Cheney,et al.  Measure and Integration , 2001 .

[7]  T. Panczyk,et al.  ANALYSIS OF THERMODESORPTION SPECTRA FROM HETEROGENEOUS SOLID SURFACES BASED ON THE STATISTICAL RATE THEORY OF INTERFACIAL TRANSPORT , 2000 .

[8]  C. A. Ward,et al.  Expression for predicting liquid evaporation flux: Statistical rate theory approach , 1999 .

[9]  C. A. Ward,et al.  Chapter 5. Statistical rate theory and the material properties controlling adsorption kinetics, on well defined surfaces , 1997 .

[10]  C. Jarzynski,et al.  A universal asymptotic velocity distribution for independent particles in a time-dependent irregular container☆ , 1993 .

[11]  R. Findlay,et al.  Statistical rate theory of interfacial transport. III. Predicted rate of nondissociative adsorption , 1982 .

[12]  E. W. Ng,et al.  A table of integrals of the error functions. , 1969 .

[13]  R. Schrage.  A theoretical study of interphase mass transfer , 1953 .

[14]  Irving Langmuir,et al.  The Vapor Pressure of Metallic Tungsten , 1913 .