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These little quasicrystalline particles impede the motion of dislocation in the material.
In situ transmission electron microscopy during annealing revealed that 1-D motion of dislocation loops occurred in pure Fe at 623 K, while 1-D motion of dislocation loops occurred minimally in Fe 1.4Mn annealed at temperatures below 773 K.
These results indicate that 1-D motion of dislocation loops play a key role in producing the differences in the microstructures between pure Fe and Fe 1.4Mn.
The solute atoms as barriers to hinder the motion of dislocation and the severe lattice distortion to suppress the free slipping of dislocation are significantly stronger obstacles to strengthen HEA.
Elucidation of the one-dimensional (1-D) motion of dislocation loops is important for describing the microstructural development of materials under irradiation.
Cyclic deformation mechanisms at low and high strain amplitudes have been discussed in terms of the motion of dislocation multipoles and the dislocation reactions between the primary and secondary slip systems.
Similar(52)
Plastic flow both on cold rolling and hydrogenation occurs via formation and motion of dislocation-like defects which are the reason of the observed anelastic anomalies.
In order to get around this, materials are being studied in which the motion of dislocations is inhibited.
Strength is derived by inhibiting the motion of dislocations in a continuous metal phase by obstacles.
In principle, the strengthening of metals is accomplished by increasing the resistance of lattice structures to the motion of dislocations.
The motion of dislocations is assumed to be unaffected by hydrogen diffusion.
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