Xm. Deng, THE ASYMPTOTIC STRUCTURE OF TRANSIENT ELASTODYNAMIC FIELDS AT THE TIPOF A STATIONARY CRACK, Proceedings - Royal Society. Mathematical and physical sciences, 446(1926), 1994, pp. 1-13
The asymptotic structure of the transient elastodynamic near-tip field
s around a stationary crack is investigated for all three fracture mod
es. The transient fields are obtained as the sum of their quasi-static
counterparts and corresponding transient correction terms, in terms o
f variable-separable expansions. By allowing the coefficients of terms
in the quasi-static expansion to deviate from their quasi-static rest
rictions, the correction terms are shown to be the particular solution
s of a set of first order (for mixed mode I and II) or second order (f
or mode III) ordinary differential equations with constant coefficient
s and non-homogeneous terms involving only sine and cosine functions o
f the independent variable. It is found that the transient effects of
dynamic loading on the near-tip fields are to alter the universal angu
lar variations of the quasi-static field quantities for the fifth and
higher order terms in their variable-separable expansions; thus the fi
rst four terms in the expansions have the same angular variations unde
r both quasi-static and dynamic loading conditions. This seems to sugg
est that transient effects on the crack-tip fields are in general less
severe for a stationary crack than for a propagating crack where only
the first two terms in the expansions hold the same angular variation
s under both steady-state and transient crack growth conditions. Furth
ermore, the transient higher order terms for a stationary crack do not
depend on the time-rate of the stress intensity factors; in fact, the
y only relate to the even order time-derivatives of the instantaneous
values of the coefficients of the terms in the quasi-static expansions
. This is also in contrast with the case of transient crack propagatio
n where the time rates of the dynamic stress intensity factors play im
portant roles in the higher order transient terms. Explicit expression
s for the transient near-tip stress and displacement fields are provid
ed.