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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 17 (1982), S. 652-670 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract High speed cinematography (up to 6000 frames sec−1), as well as optical and electron microscopy, was used to study the formation and propagation of thin and thick shear bands in atactic polystyrene, with and without obstacles in their paths of propagation. Three different kinds of obstacles were studied, an existing thick band, a fully recovered thick band and a region dispersed with 2 to 6 μm rubber particles (a strip of high impact polystyrene). Except for the fully recovered thick band which behaved like undeformed polystyrene, the other two obstacles effectively reduced the speed of propagation of the shear band packets and changed their mode of operation by dispersing them into thin bands and spreading them out into larger spaces. However, the original localized mode of operation resumed after the shear band packet passed through the obstacles.
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 18 (1983), S. 3047-3053 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract A specimen with coarse shear bands produced at stress concentrations by compression was immersed in methanol to observe craze formation. Thin crazes were initiated at shear bands and joined together while propagating to form thick crazes. Crazes were formed only on the tension side of shear bands with the craze planes perpendicular to the shear bands. When a craze propagated through a shear band, each displaced the other at intersections. Some secondary shear bands were transformed partly into crazes resulting in about a factor of ten increase in thickness. This transformation was achieved by a tensile deformation of fibrous sheets in the shear band with simultaneous production of fine fibres.
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 17 (1982), S. 3445-3459 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Shear bands produced in polystyrene by compression can be reverse sheared by a second compression in a perpendicular direction. The net shear strain can be zero or negative. Like the forward shear, the reverse shear also produces a ridge on the surface. The height of the ridge seems to be proportional to the reverse shear strain. On the side surface the reverse shear produces a step whose height increases at an average rate of 1.17 mm sec−1 (at a crosshead speed of 1 mm sec−1), estimated by high-speed cinematography at 1000 frames sec−1. During the reverse shear the second compression experiences a yield drop whose size increases with the forward strain due to the first compression. The implications of these results are discussed.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 16 (1981), S. 1858-1873 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Thick shear bands in polystyrene formed by compression could cause fracture or the formation of cracks by intersecting with themselves, by relaxing after the removal of the load, by propagating all the way to the side surfaces and by subsequent tensile deformation. The microstructural mechanisms involved in all these fracture processes are discussed.
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 20 (1985), S. 2359-2368 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Craze network with interconnecting crazes was produced in thin (~60nm) polystyrene films by using a spherical stretching method. For 30% and 45% radial strain, the average mesh size, defined as the square root of average non-crazed areas enclosed by crazes, decreased from about 28μm to 4.6 and 2.7μm, respectively, as the molecular weight increased from 46 900 to 1 350 000. At a molecular weight of about 106, the interactions between crazes became evident by the split and change of directions at the end of their propagation. Two types of intersection appeared to exist in parallel. The first type showed void formation at the intersections with no apparent fibril displacement effect. The second type showed that the fibrils at the intersection of two perpendicular crazes reoriented to a new direction which seemed to be determined by the relative displacements of the two crazes at the intersections. This observation suggests that the craze fibrils can be displaced and further stretched by a second crazing process.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 27 (1992), S. 5645-5652 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Polybenzobisoxazole fibres were compressed uniaxially in a tension-compression stage for direct observation of deformation in a scanning electron microscope. Kink bands were observed to develop on the fibre surface at early stages of deformation. They seemed to initiate heterogeneously and propagate across a large part of the fibre. Both the length and thickness of the band increased dramatically with slight compression. Upon continued deformation, cracks or openings were seen to develop from surface irregularities near the kink bands. The cracks or openings extended along the fibre length while new bands continued to develop adjacent to them. Cracks and kink bands seemed to be mutually inducible to result in a localized bulge at later stages of deformation. In Kevlar 49 fibres, cracks or openings seemed to develop at higher compressive strains notably at intersections of kink bands.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 14 (1979), S. 2172-2182 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Three types of intersection between coarse shear bands are described. The first is the most numerous and happens in a single compression. The two bands shear each other. The reason why a new band can be sheared by an existing old band seems to be that it is easier for the new band to propagate along the striation direction of the old band rather than along its own direction. The merging of striations, the stretching of molecules, and the displacement of bands are described in some detail. The second type of intersection can be created by two mutually perpendicular compressions. As in the first type, the material inside the intersection is sheared twice, first by the old band and then by the new band. However, unlike the first, the two shears are in opposite directions in the second type of intersection. Both intersections cause sufficient disturbances so that microcracks and new shear bands (both coarse and fine bands) are generated to relieve some stresses. A third type of intersection which takes place also during two mutually perpendicular compressions has a small angle of intersection. The two shears of the material in the intersection are also in nearly opposite directions. However, the disturbance is so small that no microcracks or new shear bands are generated. As a result the bands offer little resistance to each other at the intersection of the third type. For all three types of intersection, the displacement of one band corresponds approximately to the shear strain of the other intersecting band. These observations suggest that molecular ordering or directional defects exist in the coarse shear bands in polystyrene.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 14 (1979), S. 1593-1608 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract On the surface parallel to the shear direction, coarse bands appear as ridges, usually of isosceles cross-section with a height-to-base ratio of about 1/10. They split and join with thickness conservation but a corresponding change of cross-section. The shear strain along the same band is almost a constant with a most probable value of 1.8 but a spread between 1 and 3 among different bands. The bands terminate by reducing the shear strain to zero or by converting themselves to a bundle of fine bands at obstacles. Upon annealing the height of the band ridge is reduced until it disappears. When a banded surface is polished, the band pattern reappears upon either annealing or recompression. However, in the former case, the bands are valleys with reverse shear strain but in the latter they are ridges with almost no strain. Similar behaviour occurs on the polished cut surfaces in the middle of the specimen after annealing. On the side surface, the bands are wavy and they are steps rather than ridges. They also split and join with thickness conservation and they terminate freely. Based on these characteristics, the propagation of coarse bands can be viewed as the motion of macroscopic Volterra dislocations.
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 15 (1980), S. 1898-1906 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Shear bands of 0.1 to 0.6 mm thick were produced in polystyrene by compression. These bands were studied by optical microscopy and surface profilometry. Both the as-deformed bands and the bands developed after annealing were investigated. Parameters such as the shear strain, step height and the height-to-base ratio of the band cross-section (ridges or valleys) were recorded.
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 25 (1990), S. 2129-2132 
    ISSN: 1573-4803
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Notes: Abstract Biaxially oriented styrene-acrylonitrile (SAN) copolymer films with a draw ratio of 6.9 in the machine direction (MD) and 2.9 in the transverse direction (TD) were annealed under constraint in both directions. The films fractured during annealing developed cracks along the TD. The temperature dependence of the time to fracture showed an Arrhenius plot with an activation energy of 114 kcal mol−1. When annealing was terminated before fracture, the work to fracture on tensile deformation of the annealed film increased with annealing time, with a maximum increase of about 53% in the MD and 40% in the TD. The annealed films showed fewer bands or more fine shear bands as compared with unannealed films. These observations suggest a toughening effect in oriented films when annealed under dimensional constraint.
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