TY - JOUR
T1 - Energy considerations in crack deflection phenomenon in single crystal silicon
AU - Sherman, Dov
N1 - Funding Information:
Acknowledgements This research was supported by the Israel Science Foundation (Grant No. 1110/04).
PY - 2006/7
Y1 - 2006/7
N2 - Crack deflection in single-crystal brittle occurs when a crack, propagating on one cleavage plane, 'chooses', from energy considerations, to continue propagating on another cleavage plane. This phenomenon was identified during dynamic crack propagation experiments of thin, rectangular [0 0 1] single-crystal (SC) silicon specimens subjected to three-point bending (3PB). Specimens with long pre-cracks (hence propagating at a 'low' energy and velocity) cleave along the vertical (110) plane, while the same specimens but with short pre-cracks (and therefore with higher propagation energy and velocity) cleave along the inclined (111) plane. The same specimens with intermediate pre-crack length show that the crack first propagates on the (110) plane and then deflects to the (111) plane. We show that the deflection is due to variations of the material property that resists cracking, Γ, the dynamic cleavage energy, with velocity and crystallographic orientation. We propose selection criteria to explain the deflection: The crack will deflect to the plane with the lowest dynamic cleavage energy. We further suggest that crack deflection is the basic mechanism controlling the way the crack consumes energy while propagating and is the main cause of surface perturbations. The spatial temporal fracture energy along the (110) cleavage plane is evaluated.
AB - Crack deflection in single-crystal brittle occurs when a crack, propagating on one cleavage plane, 'chooses', from energy considerations, to continue propagating on another cleavage plane. This phenomenon was identified during dynamic crack propagation experiments of thin, rectangular [0 0 1] single-crystal (SC) silicon specimens subjected to three-point bending (3PB). Specimens with long pre-cracks (hence propagating at a 'low' energy and velocity) cleave along the vertical (110) plane, while the same specimens but with short pre-cracks (and therefore with higher propagation energy and velocity) cleave along the inclined (111) plane. The same specimens with intermediate pre-crack length show that the crack first propagates on the (110) plane and then deflects to the (111) plane. We show that the deflection is due to variations of the material property that resists cracking, Γ, the dynamic cleavage energy, with velocity and crystallographic orientation. We propose selection criteria to explain the deflection: The crack will deflect to the plane with the lowest dynamic cleavage energy. We further suggest that crack deflection is the basic mechanism controlling the way the crack consumes energy while propagating and is the main cause of surface perturbations. The spatial temporal fracture energy along the (110) cleavage plane is evaluated.
KW - Cleavage
KW - Crack deflection
KW - Dynamic fracture
KW - Energy dissipation
KW - Single-crystal
UR - http://www.scopus.com/inward/record.url?scp=33750307544&partnerID=8YFLogxK
U2 - 10.1007/s10704-006-0048-9
DO - 10.1007/s10704-006-0048-9
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AN - SCOPUS:33750307544
SN - 0376-9429
VL - 140
SP - 125
EP - 140
JO - International Journal of Fracture
JF - International Journal of Fracture
IS - 1-4
ER -