ICMCTF 2012! - CD-Lab Application Oriented Coating Development
ICMCTF 2012! - CD-Lab Application Oriented Coating Development
ICMCTF 2012! - CD-Lab Application Oriented Coating Development
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distributions for several peaks to yield temperature values of 2.24 to 3.27<br />
eV, and found them to be within reasonable estimates based on the<br />
measured electrical energy delivered to each device.<br />
More recently, we acquired streak spectrographs from Ni/Al laminates<br />
encapsulated with vacuum-deposited parylene. This process insured that<br />
any emission came only from the electrically Ni/Al laminates, and should<br />
allow better quantification of temperature without the same level of<br />
interference from residual gases. The encapsulation layer caused a much<br />
slower 60 ns rise to peak emission intensity, compared to 8 ns for previous,<br />
un-encapsulated tests. This rise time likely corresponded to a physical<br />
acceleration of a portion of the encapsulation layer away from the substrate,<br />
which we will measure and report in the final paper. We will also correlate<br />
spectroscopic emission at early times with measured electrical input, and<br />
gain insight into phase changes, mixing, and expected exothermic release<br />
over these extremely short timescales. These studies are important for future<br />
nanomanufacturing techniques, where it may be necessary to control spatial<br />
thermal distributions much more precisely by careful control of the<br />
timescales over which reactions take place.<br />
10:20am TS3-1-8 Numerical simulations of self-propagating reactions<br />
and analysis of reacted microstructures in Ru/Al multilayers, K. Woll<br />
(k.woll@mx.uni-saarland.de), Functional Materials, Dept of Materials<br />
Science and Engineering, Saarland University, Germany, I. Gunduz, C.<br />
Rebholz, Dept. of Mechanical and Manufacturing Engineering, University<br />
of Cyprus, Cyprus, F. Mücklich, Functional Materials, Dept of Materials<br />
Science and Engineering, Saarland University, Germany<br />
Energetic materials based on equiatomic Ru/Al multilayers have been<br />
recently introduced by our group. The unusual combination of high<br />
temperature as well as room temperature properties makes the equiatomic<br />
Ru/Al system interesting as a new energetic material. So far, selfpropagating<br />
reactions in Ru/Al multilayers have been studied with a focus<br />
on the early stages of reaction. Parameters such as front velocity and<br />
reaction temperature as well as the reaction mechanism have been<br />
experimentally determined and compared to other systems. These results<br />
clearly demonstrate that the Ru/Al system expands the reaction parameter<br />
range of previously used systems in terms of velocity and temperature.<br />
However, for a more detailed understanding of the reactions, numerical<br />
simulation which focuses on the early reaction stages as well as<br />
microstructural analysis to reveal the processes during later stages of<br />
cooling was performed. Experimental studies were carried out to investigate<br />
the effects of the interaction with surrounding air as a function of multilayer<br />
period. For this, pyrometric measurements to follow the temperature<br />
evolution during the reaction and cross sectional transmission electron<br />
microscopy analysis of reacted foils were performed.<br />
10:40am TS3-1-9 Fabrication, Characterization and <strong>Application</strong>s of<br />
Novel Nanoheater Structures, Z. Gu (Zhiyong_Gu@uml.edu), Q. Cui, J.<br />
Chen, J. Buckley, University of Massachusetts Lowell, US, T. Ando, D.<br />
Erdeniz, Northeastern University, US, P. Wong, Tufts University, US, C.<br />
Rebholz, A. Hadjiafxenti, I. Gunduz, C. Doumanidis, University of Cyprus,<br />
Cyprus<br />
Nanoheaters are reactive nanostructures that can generate localized heat<br />
through controlled ignition. Besides the widely used nanofoil structure with<br />
multiple alternative aluminum-nickel (Al-Ni) layers, various new<br />
nanostructures have been fabricated in the last several years, including<br />
consolidated compacts, bimetallic nanoparticles, and ball milled micro/nano<br />
powders. In this presentation, we show that (1) Al-Ni compacts can be<br />
fabricated by a novel ultrasonic powder consolidation (UPC) method, using<br />
Al and Ni nanopowders as source materials; (2) Al-Ni bimetallic<br />
nanoparticles have been synthesized by a galvanic replacement reaction<br />
method using Al nanoparticle templates; (3) Al-Ni micro/nanopowders can<br />
be prepared by a ball milling method using Al and Ni powders. The<br />
structure and compositions of the nanoheater structures have been<br />
characterized by electron microscopies (SEM and TEM), energy dispersive<br />
x-ray spectroscopy (EDS), and x-ray diffraction (XRD). The ignition of<br />
these nanoheater structures has been initiated by the electrical (ohmic)<br />
method, microplasma (plasma arc discharge) method, etc. The reaction<br />
characteristics of the nanoheater structures were investigated using high<br />
speed optical and infrared imaging, and the thermal characteristics of the<br />
samples were studied using differential scanning calorimetry (DSC). These<br />
novel nanoheater structures have great potential to be used in micro-joining,<br />
microelectronics assembly, and flexible electronics bonding.<br />
Thursday Morning, April 26, <strong>2012</strong> 82<br />
11:00am TS3-1-10 Effect of Mechanical Activation on SHS and<br />
Structure Formation in Nanostructured Geterogenious Reaction<br />
Systems, N. Shkodich (n.f.shkodich@mail.ru), Vadchenko, Rogachev,<br />
Sachkova, Institute of Structural Macrokinetics and Materials Science RAS,<br />
Russia, Neder, Magerl, Institute of Crystallography and Structural Physics,<br />
University of Erlangen-Nürnberg, Germany<br />
One of the possibilities to produce nanostructured materials is the<br />
combination of two non-equilibrium processing techniques, namely<br />
mechanical activation (MA) and self-propagating high-temperature<br />
synthesis (SHS). Mechanical activation provides the possibility of both<br />
modificating the conditions of the chemical reaction run and changing the<br />
thermal parameters of the synthesis (temperature, combustion velocity,<br />
heating rate, and others) thus leading to the different structures and<br />
properties of the final product.<br />
Our investigation aimed at establishing the influence of MA on SHS. The<br />
Ni─Al, Ti─BN and Ti─SiC─C systems were studied. Green mixtures were<br />
prepared by dry mixing of the initial components in china crucibles at the<br />
stoichiometric ratios corresponding to the following reactions : Ni+Al =<br />
NiAl, 3Ti+2BN = 2TiN+TiB2 and 3Ti+SiC+C = Ti3SiC2.<br />
Preliminary MA was preformed in a water cooled planetary ball mill (AGO-<br />
2) type at room temperature under argon. The milling procedure was carried<br />
out at the ball/mill ratio of 20: 1. The milling time varied from 0.20 s to 30<br />
min.<br />
The resultant mechanically activated particles were composed of layers of<br />
the initial components alternating with each other at the nano level [1, 2]..<br />
During mechanical activation of Ni+Al mixtures up to 7 min, specific<br />
contact area between reagents Ni and Al increased approximately 15-20<br />
times for each fraction.<br />
Using high-resolution SEM and TEM methods for microstructural<br />
investigation of Ni─Al activated samples, nanoscale structural components<br />
were observed. Their average atomic weight was intermediate between the<br />
Ni and Al. The main influence on the reactivity of heterogeneous systems<br />
Ni ─ Al during milling is formation of nanoscale X-ray amorphous phases<br />
and solid solutions.<br />
Ignition temperature was measured for small amounts of activated mixtures<br />
in the form of activated particles, pressed pellets, and rolled foil. The<br />
dependences of the ignition temperature on the MA duration and the way of<br />
the sample preparation were studied. It was found that after MA for 0 − 30<br />
min the ignition temperature lowered by approximately 600°C for Ti─BN<br />
and Ti─SiC─C systems; after MA for 0– 7 min it could be diminished by<br />
300–400 °C for N─Al system.<br />
For the determination of the internal microstructure, the particle size and<br />
microstrains of mechanically activated powders 3Ti+2BN and 3Ti+SiC+C<br />
and of the combustion products were analyzed by X-ray powder diffraction<br />
on a Huber Guinier diffractometer at the Institute of Crystallography and<br />
Structural Physics, in Erlangen, Germany.<br />
Analysis showed that an increase in the MA duration of the 3Ti+2BN and<br />
3Ti+SiC+C mixtures led to a decrease in the peak intensities and<br />
broadening of the Ti peaks. With increasing activation time, the BN reflexes<br />
in the 3Ti+2BN reaction mixtures were instantly broadened and in three<br />
minutes their intensity became comparable to that of the background.<br />
Similar behavior was also observed in case of graphite in the activated<br />
3Ti+SiC+C mixtures. This evidences the destruction of the crystal structure<br />
(amorphization) of boron nitride and graphite in the MA process [3].<br />
The effect of milling time on the crystalline size and strain in the powder<br />
mixtures and SHS products we determined from line broadening analysis of<br />
the XRD peaks. The Rietveld full profile refinements were carried out with<br />
the Fullprof Suite. As a result of up to 30 min MA, the average size of the<br />
Ti crystallites was found to reduced down to 25 and 50 nm in the Ti + BN<br />
and Ti─SiC─C systems, respectively. Mechanical activation was found to<br />
affect the size of product crystallites. The value of the micro stains<br />
increased with the MA duration.<br />
Formation of nanocomposites at the stage of mechanical activation provides<br />
proper conditions for synthesizing nanostructured SHS materials with a<br />
complete inherence of the precursors’ structural morphology.<br />
References<br />
[1] N.F. Shkodich, N.A. Kochetov, A.S. Rogachev, D.Yu. Kovalev, N.V.<br />
Sachkova, Izv. Vyssh. Uchebn. Zaved. Tsvetn. Metall., 5, (2006) 44-50.<br />
[2] M.A. Korchagin, M.R. Sharafutdinov, N.F. Shkodich, B.P. Tolochko,<br />
P.A. Tsygankov, I.Yu. Yagubova. Nuclear Instruments and Methods in<br />
Physics Research A, 575, (2007) 149-151.<br />
[3] Shkodich N. F, Rogachev A. S, Neder R. B., Magerl A., S.G.<br />
Vadchenko, and O. Boyarchenko, High-Temperature Ceram. Mater.<br />
Composites, 911 (2010) 881-887.<br />
Acknowledgement