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  • 1975-1979  (3)
  • 1960-1964
  • 1979  (3)
Material
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  • 1975-1979  (3)
  • 1960-1964
Year
  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 14 (1979), S. 891-896 
    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 Crystals of (SN) X were mechanically deformed and examined using transmission electron microscopy. Numerous kink bands with axes perpendicular to the chain axis were formed as part of the deformation process. The kink bands were observed to have the following characteristics: (1) high distortion beyond their edges, (2) ultimately full return of the material on either side of the kink band to the mean crystal orientation, (3) apparently random angles of kinking and (4) continuous change in orientation across the kink edge. It was noted, in describing how kink bands would form, that chain continuity poses problems that would not be present in simpler solids. A kink-band formation model is presented. In this model, particular attention is paid to chain continuity. By allowing elastic regions within the kink-band edge, it is possible to attain arbitrary kink angle.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of materials science 14 (1979), S. 221-227 
    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 Unnotched specimens of polycarbonate were deformed to failure in equal tension-compression, under load control. Fracture surfaces exhibited two distinctly different crack propagation regimes. In the first zone, the crack moves forward through an already existing craze. Craze ageing at the crack tip is necessary for propagation and several stress cycles are required before the crack tip can move from arrest site to arrest site. In the second zone, the crack tip must form and age its own craze(s) before moving forward. In the initial stage of Zone 2, the crack mobility is still restricted by the age of the craze. Later in this zone, the crack tip is able to create craze and move through it in the same cycle. Static tensile deformation from 90% to 95% of the yield point produced an increase in the low-load fatigue life. This increase is explained on the basis of the mechanics of coarse crazes.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 0098-1273
    Keywords: Physics ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: Linear polyethylene was crystallized isothermally from the melt. Specimens were removed at different crystallization times and quenched to room temperature. The density, static mechanical properties, and small-angle x-ray scattering (SAXS) behavior of these specimens were measured at room temperature. The density and Young's modulus increased with crystallization time, whereas the upper yield point decreased with crystallization time. SAXS data showed that a zero-angle peak gradually disappeared as crystallization time increased. Concurrently, the breadth of the SAXS peaks, the Bragg angle, and the integrated intensity decreased. Changes in the ratio of second- and first-order peak intensities were also noted. On the basis of the SAXS and density data, it was concluded that a competition exists between the thickening of existing crystals and the creation of new crystallites between the older ones. At relatively low crystallization times, numerous new crystals can form during quenching to room temperature, whereas quenching after prolonged crystallization primarily results in the additional thickening of existing crystals. No change in the density of the amorphous material is found. A model is given whereby the upper yield stress is coupled to these morphological changes through a stress concentration effect caused by a decreased population of chains connecting adjacent crystallites. The tie-chain population change occurs by their elimination as crystallites disappear.
    Additional Material: 11 Ill.
    Type of Medium: Electronic Resource
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