Todd C. Hufnagel
Department of Materials Science and Engineering,
Johns Hopkins
University
Abstract:
Reactive multilayer foils are energetic materials comprised of
alternating nanoscale layers of materials that can sustain a
self-propagating exothermic reaction. The reaction
characteristics, including the maximum temperature, heat released, and
speed of propagation, can be precisely controlled by appropriate design
of the multilayer architecture. However, the characteristic length
and time scales make studying the reaction itself a significant
challenge. For instance, the reaction zone is typically about 100
µm wide and propagates at about 1 ms-1,
reaching temperatures in excess of 1500°C in
less than 100 µs, followed by rapid cooling. One aspect that makes
these reactions interesting from a scientific point of view is that the
rapid heating and cooling may provide kinetic constraints which would
alter the phase transformations relative to those observed in a slower
reaction (e.g. by annealing) in the same multilayer system.
We have studied phase evolution during self-propagating reaction in A1/Ni reactive multilayers, in situ and in real time, by means of x-ray diffraction using a pixel array detector at the Cornell High Energy Synchrotron Source. The time resolution (~50 µs) and spatial resolution (~50 µm) of the measurements was sufficient to allow us to observe the phase transformation sequence in detail. In particular, we can track both the integrated peak area (which is proportional to the volume fraction) and the interplanar spacings for peaks from the various phases.
We observe that the initial reaction occurs within the first 100 µs, forming one of the final phases along with an amorphous (possibly liquid) phase. For example, A1/Ni multilayers with an overall composition of A13Ni2 form the cubic intermetallic A1Ni and an amorphous phase first, followed by hexagonal A13Ni2 some 37 ms later (during cooling after the reaction front has passed). Formation of A13Ni2 appears to occur by a peritectic transformation similar to that present in the equilibrium phase diagram. We also observe changes in lattice parameter that we attribute to the combined effects of interdiffusion and thermal expansion.
abstract (pdf)
2008 Run
Nov 19th - Dec 22nd