Abstract
A crystal structure of the T 1 phase (Al2CuLi), commonly observed in aged Al–Cu–Li alloys containing ∼3%Cu and 2%Li, is proposed. It is an ‘ideal’ crystal structure in the sense that it predicts X-ray peaks with intensities in fair agreement with those reported semiquantitatively by Hardy and Silcock, but for which additional structure refinement is not warranted. With the ideal crystal structure as a basis, the expected electron diffraction patterns for the zone axes [00l], [110], [111], [112], [013], and [114] have been predicted. These are demonstrated to be in excellent agreement with those observed experimentally. However, in addition to the structure factor for the unit cell, multiple diffraction, the T 1 plate thickness and shape, the number of T 1 variants contributing to a given reflection, and possibly faulting within the T 1 particles all contribute to the intensities of the diffracted electron beams. The roles of plate thickness and multiple diffraction are particularly important since many of the T 1 reflections observed are not centred on T 1 reciprocal lattice points lying exactly in the zero order Laue zone of the matrix. The observed T 1 reflections are therefore frequently a consequence of the intersections of streaks of diffracted intensity with the reflecting sphere. Since all the observed diffraction effects are attributable to T 1 precipitates there is no need to invoke the existence of a precursor T 1′ phase, as has been recently proposed. It is concluded that there is no evidence for the existence of a metastable plate-shaped precipitate preceding T 1 particles in the aging sequence of the alloy.
MST/599
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