MICROSCOPIC MECHANISMS AND MECHANICS OF CRAZE GROWTH AND FRACTURE

被引:302
作者
LAUTERWASSER, BD [1 ]
KRAMER, EJ [1 ]
机构
[1] CORNELL UNIV,CTR MAT SCI & ENGN,ITHACA,NY 14853
来源
PHILOSOPHICAL MAGAZINE A-PHYSICS OF CONDENSED MATTER STRUCTURE DEFECTS AND MECHANICAL PROPERTIES | 1979年 / 39卷 / 04期
基金
美国国家科学基金会;
关键词
D O I
10.1080/01418617908239285
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Isolated air crazes have been produced in thin films of polystyrene (PS) bonded to copper grids by straining these in tension. The craze thickness profile, r(x), was directly determined from a series of transmission electron micrographs taken along the craze. Local values of the craze fibril volume fraction v1 and fibril extension ratio λ were established at frequent intervals along the craze by optical densitometry of the micrographs. The craze surface displacement profile w(x), craze surface stress profile S(x) and the true stress at in the craze fibrils are computed from these parameters. The λ(x) profile provides conclusive evidence that the craze increases in thickness as it grows in length by drawing new polymer from the craze surface into the fibrils rather than by creep of the existing fibrils. The S profile exhibits a modest maximum at the craze tip but falls slowly over a distance of about 15 μm behind the craze tip to a value about 10% below the applied tensile stress. The λ of the drawn craze fibrils is a function of the surface stress S at the time they are drawn. The fibrils drawing at high S just behind the growing craze tip result in formation of the midrib, a layer of high λ in the craze midway between the craze surfaces. The highest values of λ observed, in the midrib and the craze tip, are nearly those required to completely extend PS molecules between molecular entanglements in the glass; further extension must result in chain disentanglement and fibril rupture. While chain disentanglement in the fibrils of the midrib is the probable first step in fracture, propagation of a crack in an existing craze results in a large increase in S ahead of the crack, and two layers of very-high-λ craze fibrils draw from the craze surfaces in response. The crack now prefers to propagate in these layers, rather than in the midrib, and jumps from one to the other causing the familiar mackerel or patch pattern on PS fracture surfaces. © 1979 Taylor & Francis Group, LLC.
引用
收藏
页码:469 / 495
页数:27
相关论文
共 48 条
[1]   MECHANISM OF FRACTURE IN GLASSY MATERIALS CAPABLE OF SOME INELASTIC DEFORMATION [J].
ARGON, AS ;
SALAMA, M .
MATERIALS SCIENCE AND ENGINEERING, 1976, 23 (2-3) :219-230
[2]   GROWTH OF CRAZES IN GLASSY POLYMERS [J].
ARGON, AS ;
SALAMA, MM .
PHILOSOPHICAL MAGAZINE, 1977, 36 (05) :1217-1234
[3]   PHYSICAL BASIS OF DISTORTIONAL AND DILATIONAL PLASTIC-FLOW IN GLASSY POLYMERS [J].
ARGON, AS .
JOURNAL OF MACROMOLECULAR SCIENCE-PHYSICS, 1973, B 8 (3-4) :573-596
[4]   FRACTURE PROCESSES IN POLYSTYRENE [J].
BEAHAN, P ;
BEVIS, M ;
HULL, D .
PROCEEDINGS OF THE ROYAL SOCIETY OF LONDON SERIES A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 1975, 343 (1635) :525-&
[5]   MORPHOLOGY OF CRAZES IN POLYSTYRENE [J].
BEAHAN, P ;
BEVIS, M ;
HULL, D .
PHILOSOPHICAL MAGAZINE, 1971, 24 (192) :1267-&
[6]  
BEAHAN P, 1972, J MATER SCI, V8, P162
[8]   THICK SPECIMENS IN CEM AND STEM .1. CONTRAST [J].
CREWE, AV ;
GROVES, T .
JOURNAL OF APPLIED PHYSICS, 1974, 45 (08) :3662-3672
[9]  
DOYLE MJ, 1976, ADV CHEM SER, P63
[10]   DENSITY OF CRAZE LAYER ON FRACTURE SURFACE OF POLYSTYRENE [J].
DOYLE, MJ .
JOURNAL OF MATERIALS SCIENCE, 1973, 8 (08) :1185-1188