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5th International Conference and Exhibition on Polymer Chemistry

Toronto, Canada

Alan F. Jankowski

Alan F. Jankowski

Sandia National Laboratory, USA

Title: Interdiffusion kinetics in Cu-Ni(Fe) nanolaminate structures


Biography: Alan F. Jankowski


The decomposition of a one-dimensional composition wave in Cu-Ni(Fe) nanolaminate structures is quantified using x-ray diffraction to quantify the kinetics of interdiffusion processes. A schematic of an A/B nanolaminate structure with A (dark-shaded) and B (light-shaded) atoms is shown (below left) as viewed in cross-section. Features are shown such as a threading dislocation (d), grain boundary (gb) between columnar grains, and the A/B layer pair thickness, i.e. the composition wavelength (lA/B). Cu-Ni(Fe) is a spinodal alloy system where the growth or decay growth of the composition modulation occurs within or above the critical temperature for the chemical spinodal, respectively. A transmission electron microscope, bright-field image and selected area diffraction pattern (insert) are shown (below right) for a Cu-Ni(Fe) nanolaminate with a 4.34 nm composition wavelength, revealing its ultra-fine grain nanocrystalline structure. Evidence of a negative interdiffusivity is found for each of sixteen different nanolaminate samples that are aged at room temperature over a composition wavelength range of 2.1–10.6 nm. A diffusivity value Ď of 1.77 × 10−24 cm2·s−1 is determined for the alloy system at room temperature – perhaps, the first such measurement at a ratio of melt temperature to test temperature that is greater than 5. Although this diffusivity value is extremely small, it is several orders of magnitude greater than that value extrapolated from high temperature to room temperature for a bulk diffusion mechanism. Diffusion mechanisms that are operative from room to high temperatures for the Cu-Ni(Fe) nanolaminate structures (shown in the image below) are reviewed, including the possible effects of short-circuit diffusion through interlayer grain boundaries.