The dynamics of the hydrogen bond breaking and reforming are investigated u
sing a model for water in which each water molecule is a hard sphere with f
our sticky spots located at the corners of a tetrahedron. H-bonding arises
when a pair of particles attach at their sticky spots by means of the narro
w, anisotropic square well potential. To escape the square well, and break
the H-bond, a solvent molecule must collide with the bonded pair and commun
icate sufficient energy along the line of centers so as to exceed the thres
hold energy. The calculated time correlation function describes the fluctua
tion in the number of H-bonded pairs. Its correlation time, associated with
the three-body direct rupture, is roughly 0.83 ps in water at 300 K and ob
eys an Arrhenius law. After bond rupture, the restituting solvent molecule
can return (or backscatter) and in so doing, cause the initial dimer to ref
orm its H-bond. As a result, the overall correlation time for bond breaking
is roughly 14 ps. Employed here are aspects of the kinetic theory of squar
e well fluids together with Wertheim's theory for associating systems. (C)
2001 American Institute of Physics.