Abstract
The Obreimov—Gilman cleavage technique has been used to study, in a quantitative manner, the effects of a mercury environment on the cleavage fracture energy of high purity zinc monocrystals. The experimental observations support the view that the total energy involved in the propagation of a crack, Φ, can be conveniently represented by the relation Φ = η• ρ • γ0, where η is an environmental variable—-the coefficient of embrittlement—-which relates the energy required to separate atoms at the crack tip in the presence and absence of an embrittling phase, ρ is a dimensionless variable dependent upon the degree of plastic relaxation at the crack tip and independent of η, and γ0 is the true surface energy of the fracture plane. In this work, γ0Zn(77°K) was determined to be 90 ± 10 ergs/cm2, γ0Zn(29°K) to be 87 ± 5 ergs/cm2 and η Zn-Hg(298°) to be 0•61 ± 0•12.
On the basis of available experimental evidence concerning embrittlement by liquid metals, a new mechanism for this phenomenon is considered. This involves a localized reduction in cohesion introduced by the strain-activated chemisorption of liquid-metal atoms (i) at sites of high dislocation density, facilitating crack initiation, and (ii) at the tip of an initiated crack, facilitating its propagation.