Long‐Range Intermolecular Forces

1956 ◽  
Vol 25 (5) ◽  
pp. 986-1005 ◽  
Author(s):  
John S. Dahler ◽  
Joseph O. Hirschfelder
2011 ◽  
Vol 115 (45) ◽  
pp. 12933-12940 ◽  
Author(s):  
G. V. Gibbs ◽  
T. D. Crawford ◽  
A. F. Wallace ◽  
D. F. Cox ◽  
R. M. Parrish ◽  
...  

1984 ◽  
Vol 110 (2) ◽  
pp. 123-129 ◽  
Author(s):  
A.J. Stone ◽  
R.J.A. Tough

2005 ◽  
Vol 73 (5) ◽  
pp. 792-798 ◽  
Author(s):  
Eun-Suok Oh ◽  
Jay R. Walton ◽  
John C. Slattery

A theory of fracture is presented that is based upon an extension of continuum mechanics to the nanoscale through the incorporation of long-range intermolecular forces which correct bulk material descriptions near interfaces. The surface energy on crack surfaces, which is given in terms of the long-range intermolecular forces, plays an important role in an expression for the stress distribution near the crack tip. It is observed through numerical simulation that the incorporation of these long-range intermolecular forces removes the square-root stress singularity predicted by classical linear elastic fracture mechanics.


1975 ◽  
Vol 28 (6) ◽  
pp. 1161 ◽  
Author(s):  
PE Schipper

The chemical manifestations of discrimination in long-range (non- contact) interactions of chiral molecules are analysed in three stages. A simple thermodynamic model is used to establish a method of presenting experimental data (such as differences in racemization rates, solubilities and redox potentials of pure enantiomers in non- associating chiral media) in terms of well defined thermodynamic discriminations. The thermodynamic quantities are then related directly to discriminations in intermolecular interactions through a statistical thermodynamic treatment. Estimates of the discrimination in intermolecular forces from experimental thermodynamic data suggest that only electrostatic interactions are sufficiently large to account for the experimentally observed values of the discrimination.


1985 ◽  
Vol 63 (1) ◽  
pp. 30-33 ◽  
Author(s):  
A. D. Buckingham

Intermolecular forces, and their effects on the properties of gases, liquids, and solids, are related, by long-range theory, to the properties of the isolated molecules. The usefulness of this approach is expounded, and its limitations investigated by means of ab initio computations. It is suggested that the structures of many Van der Waals molecules, and particularly those with a hydrogen bond, are attributable to electrostatic forces.


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