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Dislocation - Dislocations slip and plasticity |  | Dislocation - Dislocations slip and plasticity: Encyclopedia II - Dislocation - Dislocations slip and plasticity |  | Until the 1930s, one of the enduring challenges of materials science was to explain plasticity in microscopic terms. A naive attempt to calculate the shear stress at which neighbouring atomic planes slip over each other in a perfect crystal suggests that, for a material with shear modulus G, shear strength τm is given approximately by:
As shear modulus in metals is typically within the range 20 000 to 150 000 MPa, this is difficult to reconcile with shear stresses in the range 0.5 t ...
See also:Dislocation, Dislocation - Dislocation geometry, Dislocation - Edge dislocations, Dislocation - Burgers vector, Dislocation - Screw and mixed dislocations, Dislocation - Observation of Dislocations, Dislocation - Dislocations slip and plasticity, Dislocation - Bibliography |  | | Dislocation, Dislocation - Bibliography, Dislocation - Burgers vector, Dislocation - Dislocation geometry, Dislocation - Dislocations slip and plasticity, Dislocation - Edge dislocations, Dislocation - Observation of Dislocations, Dislocation - Screw and mixed dislocations |  | |
|  |  | Dislocation: Encyclopedia II - Dislocation - Dislocations slip and plasticity
Dislocation - Dislocations slip and plasticity
Until the 1930s, one of the enduring challenges of materials science was to explain plasticity in microscopic terms. A naive attempt to calculate the shear stress at which neighbouring atomic planes slip over each other in a perfect crystal suggests that, for a material with shear modulus G, shear strength τm is given approximately by:
As shear modulus in metals is typically within the range 20 000 to 150 000 MPa, this is difficult to reconcile with shear stresses in the range 0.5 to 10 MPa observed to produce plastic deformation in experiments.
In 1934, Egon Orowan, Michael Polanyi and G. I. Taylor, roughly simultaneously, realised that plastic deformation could be explained in terms of the theory of dislocations. Dislocations can move if the atoms from one of the surrounding planes break their bonds and rebond with the atoms at the terminating edge. Even a simple model of the force required to move a dislocation shows that shear is possible at much lower stresses than in a perfect crystal. (Hence, the characteristic maleability of metals).
When metals are subjected to "cold working" (deformation at temperatures which are relatively low as compared to the material's absolute melting temperature, Tm, i.e., typically less than 0.3 Tm) the dislocation density increases due to the formation of new dislocations and dislocation multiplication. The consequent increasing overlap between the strain fields of adjacent dislocations gradually increases the resistance to further dislocation motion. This causes a hardening of the metal as deformation progresses. This effect is known as strain hardening (also “work hardening”).
The effects of strain hardening can be removed by appropriate heat treatment (annealing) which promotes the recovery and subsequent recrystallisation of the material.
Other related archives1905, 1930s, 1934, Dislocation (medicine), Dislocation (syntax), Egon Orowan, Field ion microscopy, G. I. Taylor, MPa, Materials science, Michael Polanyi, Transmission electron microscopy, Vito Volterra, annealing, atom probe, atoms, cold working, crystal, crystal structure, crystallographic defect, diffraction, electron, etching, grain boundaries, materials science, metals, microstructure, perfect crystal, planes, plasticity, recrystallisation, shear modulus, shear stress, strain hardening
 Adapted from the Wikipedia article "Dislocations slip and plasticity", under the G.N U Free Docmentation License. Please also see http://en.wikipedia.org/wiki |
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