Impression creep of zinc and the rate-controlling dislocation mechanism of plastic flow at high temperatures

1982 ◽  
Vol 70 (1) ◽  
pp. 63-71 ◽  
Author(s):  
G. S. Murthy ◽  
D. H. Sastry
1964 ◽  
Vol 101 (6) ◽  
pp. 488-495 ◽  
Author(s):  
R. Bradshaw ◽  
M. K. Wells

AbstractA layer of massive and lineated hornblende-biotite-gneiss has fractured along ac-joints (perpendicular to the layering and b–lineation), at regular intervals along its lower surface in contact with a thin marble bed. The joints have been opened from below and the marble has penetrated upwards to form intrusive tongues caused by extremely plastic flow folding, as shown by the unbroken banding in the marble. The structure constitutes a variety of one-sided boudinage involving segmentation in the lowest metre or so of the hornblendic rock, while the extreme marble deformation is all accommodated in a few centimetres thickness. The structures must have developed at relatively high temperatures to allow contemporaneous segregation of quartz-feldspar pegmatite veins from the hornblendic rock, and of diopside reaction skarns at the marble junctions.


1947 ◽  
Vol 20 (1) ◽  
pp. 171-172
Author(s):  
J. R. Scott

Abstract It has already been shown that liquids consisting essentially of aliphatic hydrocarbons, e.g., petroleum ether, paraffin, and transformer oil, had practically no swelling action at 34° C on two samples of hard rubber composed of rubber and sulfur only. Hard rubber shows a pronounced change in properties at temperatures above a critical value (“yield temperature”) in the neighborhood of 50° –80° C, the most noticeable effect being that it becomes much softer and more susceptible to plastic flow. It seemed likely, therefore, that the swelling action of liquids such as those mentioned above might be much greater at temperatures above this critical value. This view was strengthened by the statement of Dunton and Muir that hard rubber is “badly attacked” by immersion for 7 days in “hot” transormer oil. As no data appear to have been published on the effect of temperature on the swelling of hard rubber, experiments were made to examine this effect. Details of the hard rubber samples used are as follows.


1999 ◽  
Vol 47 (12) ◽  
pp. 3507-3514 ◽  
Author(s):  
V.V. Bulatov ◽  
O. Richmond ◽  
M.V. Glazov

Recovery processes tend to counteract the effects of work hardening during plastic deformation at high temperatures and at strain rates ranging from those of slow creep to those of rapid hot working operations. However, in metals in which recovery is relatively slow, sufficient stored energy can be accumulated to cause the occurrence of dynamic recrystallization during deformation once a critical strain is exceeded. This process then occurs repeatedly with continued straining. If any metal that has been deformed at high temperatures by a dislocation mechanism is held at temperature after deformation, static recrystallization tends to occur with time. The effects of dynamic and static recrystallization on microstructure and on the flow stress or creep rate of the metal are considered in this paper and particular attention is given to the range of deformation conditions under which these recrystallization processes are expected to occur. When metals deform plastically by crystal slip at elevated temperatures, the work hardening produced by deformation tends to be counteracted by recovery processes. These recovery processes cause rearrangement and annihilation of dislocations so that, as strain increases, the dislocations tend to form into two dimensional subgrain walls. In some metals and alloys the recovery entirely balances work hardening, and steady state is achieved and can be maintained to large strains before fracture occurs. In other metals in which recovery is less rapid, certain conditions of stress and temperature of deformation can result in the accumulation of sufficiently high local differences in dislocation density to nucleate recrystallization during deformation. This recrystallization is referred to as dynamic recrystallization to distinguish it from the recrystallization that can occur in all metals when deformation is discontinued but the elevated temperature is maintained, or when deformation is carried out at low temperature and the metal is subsequently annealed. In this paper, both types of recrystallization and their effects on deformation behaviour and microstructure will be outlined and the range of deformation conditions under which they are likely to occur will be considered.


1992 ◽  
Vol 156 (2) ◽  
pp. 125-130 ◽  
Author(s):  
T. Sakuma ◽  
H. Hondo

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