Analysis and Mechanics. Fourth International Conference on by D.M. R. Taplin

By D.M. R. Taplin

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Cambridge Phil. S o c , ,56, 1960, 269. BYRD, P. F. and FRIEDMAN, M. , Handbook of Elliptic Integrals for Engineers and Scientists, Second Edition, Springer Berlin, 1971. FREUND, L. B. and CLIFTON, R. , J. Elasticity, £, 1974, 293. , J. Mech. Phys. Solids, _2^, 1973, 229. 5 0. Figure 1 Figure 2 Crack Geometry Limiting Crack Speeds v/c, Figure 3 Normalized Energy Release Rates Versus Crack Speed 38 Fracture 1977, Volume Z, ICF4, Waterloo, Canada, June 19 - 24, 1977 A CRACK GROWTH GAGE FOR ASSESSING FLAW GROWTH POTENTIAL IN STRUCTURAL COMPONENTS A.

J. Eng. , L4, 1976, 181. SIH, G. C , PARIS, P. C. , J. Appl. , ,2£, 1962, 306. CRAGGS, J. , Proc. Cambridge Phil. S o c , ,56, 1960, 269. BYRD, P. F. and FRIEDMAN, M. , Handbook of Elliptic Integrals for Engineers and Scientists, Second Edition, Springer Berlin, 1971. FREUND, L. B. and CLIFTON, R. , J. Elasticity, £, 1974, 293. , J. Mech. Phys. Solids, _2^, 1973, 229. 5 0. Figure 1 Figure 2 Crack Geometry Limiting Crack Speeds v/c, Figure 3 Normalized Energy Release Rates Versus Crack Speed 38 Fracture 1977, Volume Z, ICF4, Waterloo, Canada, June 19 - 24, 1977 A CRACK GROWTH GAGE FOR ASSESSING FLAW GROWTH POTENTIAL IN STRUCTURAL COMPONENTS A.

For a more realistic pressure profile we would expect it to drop even more and to approximately correspond to the other extreme value which is no gas penetration and modelled by q ■> °°. Based on these curves we also expect that the theoretical limiting velocity may be lower than the Rayleigh wave velocity in a situation where the gas doesn't entirely fill a propaga­ ting crack. The results presented above can only form a qualitative basis for the equa­ tion of motion of a pressurized crack in a blasting situation.

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