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FRACTURE MECHANICS. Energy approach. 0. r. . x. a. H.M.Westergaard, 1939, N.I.Muskhelischvili, 1943 – 2D analysis of the stress field around the notch tip. A. y. Dla. Singularity !. Stress intensity factor.
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FRACTURE MECHANICS Energy approach
0 r x a H.M.Westergaard, 1939, N.I.Muskhelischvili, 1943 – 2D analysis of the stress field around the notch tip A y Dla Singularity ! Stress intensity factor
Stress intensity factors for different orientation of crack plane and loading has been calculated around 1960 (G.Sih) To stystemise above, three cases are distinguished: KII KI KIII Mode I - Tearing; crack surfaces open perpendicular to the planes of its movement Mode II – Out-of-plane shear; crack surfacesslide perpendicular to the planes of its movement Mode III - Out-of-plane shear; crack surfacesslide paralel to the planes of its movement
Stress-based approach Safe design requires following conditions to be fulfilled: KI < KIc KII < KIIc KIII < KIIIc KIc , KIIc , KIIIc where are critical values of responsible stress intensity factors, experimentally determined
b a Griffith theory G.V. Kolosow 1910 & C.E.Inglis, 1913 – Thin plate of unlimited width containing an elliptical hole q[Pa] y x σ 3q a b INDEPENDENT OF THE MAGNITUDE OF a !!! σ b 0 q[Pa]
if but y x l l where With then c ! for |x|<l w PSS for |x|<l w PSD for |x|>l The work of external load on displacementu(c=1m) u
q Energy required W0 y W0-W u l x l l W Energy supplied q The work of external load on displacementu • Energy required to form a free surface of the length 2x2l (over unit thickness of the plate) - surface energy of unit thickness [N/m] d(W0-W)/dl=0 lkr Instability point
d(W0-W)/dl=0 For l=lkr LFM:
You will see an experiment showing how elastic energy released with the crack length growth is transferred to the region of final failure
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q Even 5-fold reduction of cross section area does not reduce strength of the specimen! q
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