Deformation and fracture of solids are discussed as comprehensive dynamics based on
a field theory. Applying the principle of local symmetry to the law of elasticity and
using the Lagrangian formalism, this theory derives field equations that govern
dynamics of all stages of deformation and fracture on the same theoretical
foundation. Formulaically, these field equations are analogous to the Maxwell
equations of electrodynamics, yielding wave solutions. Different stages of
deformation are characterized by differences in the restoring mechanisms
responsible for the oscillatory nature of the wave dynamics. Elastic deformation
is characterized by normal restoring force generating longitudinal waves;
plastic deformation is characterized by shear restoring force and normal
energy-dissipative force generating transverse, decaying waves. Fracture is
characterized by the final stage of plastic deformation where the solid has lost
both restoring and energy-dissipative force mechanisms. In the transitional
stage from the elastic regime to the plastic regime where both restoring and
energy-dissipative normal force mechanisms are active, the wave can take the
form of a solitary wave. Experimental observations of transverse, decaying
waves and solitary waves are presented and discussed based on the field
theory.
Keywords
deformation of solids, plastic deformation transverse-wave,
elasto-plastic solitary-wave