
Stress corrosion and acoustic emission during tensile crack propagation in Whin Sill dolerite and other basic rocks
Author(s) -
Meredith P. G.,
Atkinson B. K.
Publication year - 1983
Publication title -
geophysical journal of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.302
H-Index - 168
eISSN - 1365-246X
pISSN - 0016-8009
DOI - 10.1111/j.1365-246x.1983.tb01911.x
Subject(s) - sill , acoustic emission , amplitude , geology , logarithmic scale , ultimate tensile strength , mineralogy , materials science , composite material , physics , acoustics , petrology , optics
Summary. Double torsion tests in ambient air and liquid water have been used to establish critical stress intensity factors ( K Ic ) and stress intensity factor ( K I )‐crack velocity ( v ) diagrams for propagation of single tensile cracks in Whin Sill dolerite and Ralston Intrusive. K Ic for Whin Sill dolerite was 3.28 MN m ‐3/2 and for Ralston Intrusive was 2.58 MN m =3/2 . No stress corrosion limit was encountered. Acoustic response was monitored during experiments on Whin Sill dolerite which spanned a velocity range from 5 × 10 ‐4 to 5 × 10 ‐9 m s ‐1 . The rate of acoustic emission was an indirect measure of crack velocity. The slopes of K I ‐ v diagrams and K I ‐acoustic emission rate diagrams had similar slopes of c . 30 in double logarithmic coordinate frames. Slopes of the K I ‐ v curves for Ralston Intrusive fell from 43.4 in air to 23.3 in water, during tests which spanned a crack velocity range from 5 × 10 ‐4 to 10 ‐8 m s ‐1 . The activation enthalpy for dolerite between 20° and 75°C was determined by two complementary methods to be 30.4 × 1.9 and 33‐46 kJ mol ‐1 . Amplitude distributions of acoustic emission events depend strongly on K I and the ‘humidity’ at the crack tip. As K Ic is approached, b ‐values for dolerite in air decrease from 1.8 to 1.25, and for dolerite in water a decrease occurs in b ‐value from 3.5 to 1.25. At K I greater than 0.8 K Ic the b ‐values for tests in water and in air are virtually identical. A discussion is given of these results in terms of their implications for earthquake mechanics.