1991
DOI: 10.1103/physrevlett.67.457
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Instability in dynamic fracture

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Cited by 387 publications
(167 citation statements)
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“…This is consistent with findings in experiments [34,35] and MD simulations [15,36], which indicated that brittle cracks have limiting velocities well below predictions by continuum fracture theory.…”
Section: Brittle-to-ductile Transitionsupporting
confidence: 80%
“…This is consistent with findings in experiments [34,35] and MD simulations [15,36], which indicated that brittle cracks have limiting velocities well below predictions by continuum fracture theory.…”
Section: Brittle-to-ductile Transitionsupporting
confidence: 80%
“…Instead of the propagation of a single simple crack, these experiments showed that rapid cracks are composed of an ensemble of simultaneously propagating cracks. Later experiments [46], suggested that the break-up of a simple crack to multiple cracks occurred at a critical velocity, at which a single crack became unstable. This instability, which became known at the "microbranching" instability, was later shown to be characteristic of many brittle amorphous materials [11,31,[46][47][48][49][50][51][52][53][54][55].…”
Section: A the Micro-branching Instabilitymentioning
confidence: 99%
“…Then, as v reaches the first critical velocity v a ≃165 m.s −1 =0.19 c R , Γ increases abruptly to a value about 3 times larger than K 2 c /E. Beyond v a , Γ increases slowly with v up to the second critical velocity, v b =0.36c R ≃ 317 m.s −1 [10], above which Γ diverges again with v. This second increase corresponds to the onset of the micro-branching instability, widely discussed in the literature [11] [10], whereas the first one, at v a , was reported in [38] for the first time. The high slope of Γ(v) around v a provides a direct interpretation for the repeated observation of cracks that span a large range of Γ but propagate at a nearly constant velocity of about 0.2c R (see e.g.…”
Section: -P2mentioning
confidence: 90%
“…The existence of a micro-branching instability [11,12] at a critical velocity v b = 0.4c R may explain part of this discrepancy: Beyond v b , the crack motion stops to be a single crack state to become a multiple crack state that cannot be described by Eq. 1 anymore.…”
Section: Introductionmentioning
confidence: 95%