Abstract
The effective surface energy of four brittle materials, alumina, poly(methylmethacrylate), glass, and graphite, is calculated from load/deflection curves of notched bars deformed in three-point bending. Two of the methods, which are commonly used in fracture mechanics studies,viz the modified Griffith treatment and the compliance analysis method, are concerned with the effective surface energy at the initiation of fracture,γ I . The third method, the work of fracture test, is concerned with the mean effective surface energy over the whole fracture process,γ F . The two estimates ofγ I give consistent values, and there is no systematic variation ofγ I with notch depth. Values ofγ F decrease with increasing notch depth as the fracture process becomes more controlled. For aluminaγ I ∼γ F . For PMMA and glassγ I > γγ F because of a multiplicity of crack sources during fracture initiation. For graphiteγ I <γ F because of subsidiary cracking as fracture proceeds.
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References
H. G. Tattersall andG. Tappin,J. Matls. Sci. 1 (1966) 296.
J. Nakayama,J. Amer. Ceram. Soc. 48 (1965) 583.
G. R. Irwin,Trans. ASM 40A (1948) 147.
E. Orowan,Welding J. 34 (1955) 157.
D. H. Winne andB. M. Wundt,Trans. ASME 80 (1958) 1643.
B. Gross andJ. E. Srawley, NASA Report TN-2603, 1965.
J. E. Srawley andW. F. Brown, “Fracture Toughness Testing and its Application” (ASTM, 1964) and NASA TM X-52030 (1964).
J. M. Corum, USAEC Report ORNL-4030(1966).
F. J. P. Clarke,Acta Met. 12 (1964) 139.
R. W. Davidge andG. Tappin,J. Matls. Sci. 3 (1968) to be published.
J. J. Benbow andF. C. Roesler,Proc. Phys. Soc. B70 (1957) 201.
J. P. Berry,J. Appl. Phys. 34 (1963) 62.
A. Van Den Boogaart, “Physical Basis of Yield and Fracture” (Phys. Soc., London, 1966) p. 167.
E. B. Shand,J. Amer. Ceram. Soc. 44 (1961) 21.
F. F. Lange andK. A. D. Lambe,Phil. Mag. in press.
S. M. Wiederhorn,J. Amer. Ceram. Soc. 50 (1967) 407.
R. H. Knibbs,J. Nucl. Matls. 24 (1967) 174.