When a polycrystalline fiber is heated for some time, grains change sh
ape and may evolve to one of two equilibrium configurations: isolated
spheres, or truncated spheres that remain connected. To which configur
ation do the grains evolve? How long does this evolution take? These a
re global questions, and call for a global way to look at the phenomen
on. The fiber is a nonequilibrium structure. The free energy consists
of the surface and grain-boundary energies; it is the reduction of thi
s energy that drives the diffusive flux of atoms on the surfaces and t
he grain boundaries. We describe the grain shape using two generalized
coordinates, the grain length and the dihedral angle. The fret: energ
y is expressed as a function of these coordinates. In the space of the
free energy and the coordinates, the energy function is represented b
y a surface, or a landscape. A point on the landscape represents a non
equilibrium state in general, and the bottom of a valley represents an
equilibrium state. We use a variational principle to assign a viscosi
ty matrix to every point on the landscape. The approach leads to a set
of ordinary differential equations that govern the evolution of the g
eneralized coordinates.