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Effects of Sample Size on Various Metallic Glass Micropillars in MicrocompressionLai, Yen-Huei 16 November 2009 (has links)
Over the past decades, bulk metallic glasses (BMGs) have attracted extensive interests
because of their unique properties such as good corrosion resistance, large elastic limit, as
well as high strength and hardness. However, with the advent of micro-electro-mechanical
systems (MEMS) and other microscaled devices, the fundamental properties of
micrometer-sized BMGs have become increasingly more important. Thus, in this study, a
methodology for performing uniaxial compression tests on BMGs having micron-sized
dimensions is presented.
Micropillar with diameters of 3.8, 1 and 0.7 £gm are fabricated successfully from the
Mg65Cu25Gd10 and Zr63.8Ni16.2Cu15Al5 BMGs using focus ion beam, and then tested in
microcompression at room temperature and strain rates from 1 x 10-4 to 1 x 10-2 s-1.
Microcompression tests on the Mg- and Zr-based BMG pillar samples have shown an
obvious sample size effect, with the yield strength increasing with decreasing sample
diameter. The strength increase can be rationalized by the Weibull statistics for brittle
materials, and the Weibull moduli of the Mg- and Zr-based BMGs are estimated to be about
35 and 60, respectively. The higher Weibull modulus of the Zr-based BMG is consistent with
the more ductile nature of this system.
In additions, high temperature microcompression tests are performed to investigate the
deformation behavior of micron-sized Au49Ag5.5Pd2.3Cu26.9Si16.3 BMG pillar samples from
room to their glass transition temperature (~400 K). For the 1 £gm Au-based BMG pillars, a
transition from inhomogeneous flow to homogeneous flow is clearly observed at or near the
glass transition temperature. Specifically, the flow transition temperature is about 393 K atthe strain rate of 1 x 10-2 s-1.
For the 3.8 £gm Au-based BMG pillars, in order to investigate the homogeneous
deformation behavior, microcompression tests are performed at 395.9-401.2 K. The strength
is observed to decrease with increasing temperature and decreasing strain rate. Plastic flow
behavior can be described by a shear transition zone model. The activation energy and the
size of the basic flow unit are deduced and compared favorably with the theory.
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INFLUENCE OF IRRADIATION AND LASER WELDING ON DEFORMATION MECHANISMS IN AUSTENITIC STAINLESS STEELSKeyou Mao (6848774) 02 August 2019 (has links)
<p>
This dissertation describes the recent advancements in
micromechanical testing that inform how deformation mechanisms in austenitic stainless
steels (SS) are affected by the presence of irradiation-induced defects.
Austenitic SS is one of the most widely utilized structural alloys in nuclear
energy systems, but the role of irradiation on its underlying mechanisms of
mechanical deformation remains poorly understood. Now, recent advancement of
microscale mechanical testing in a scanning electron microscope (SEM), coupled
with site-specific transmission electron microscopy (TEM), enables us to
precisely determine deformation mechanisms as a function of plastic strain and
grain orientation.</p>
<p> </p>
<p>We focus on AISI 304L SSs irradiated in
EBR-II to ~1-28 displacements per atom (dpa) at ~415 °C and contains ~0.2-8
atomic parts per million (appm) He amounting to ~0.2-2.8% swelling. A portion
of the specimen is laser welded in a hot cell; the laser weld heat affected
zone (HAZ) is studied and considered to have undergone post-irradiation
annealing (PIA). An archival, virgin specimen is also studied as a control. We
conduct nanoindentation, then prepare TEM lamellae from the indent plastic
zone. In the 3 appm He condition, TEM investigation reveals nucleation of
deformation-induced <i>α</i>’ martensite in
the irradiated specimen, and metastable <i>ε</i>
martensite in the PIA specimen. Meanwhile, the unirradiated control specimen
exhibits evidence only of dislocation slip and twinning; this is unsurprising
given that alternative deformation mechanisms such as twinning and martensitic
transformation are typically observed only near cryogenic temperatures in
austenitic SS. Surface area of irradiation-produced cavities contribute enough
free energy to accommodate the martensitic transformation. The lower population
of cavities in the PIA material enables metastable <i>ε</i> martensite formation, while the higher cavity number density in
the irradiated material causes direct <i>α</i>’
martensite formation. In the 0.2 appm He condition, SEM-based micropillar
compression tests confirm nanoindentation results. A deformation transition map
with corresponding criteria has been proposed for tailoring the plasticity of irradiated
steels. Irradiation damage could enable fundamental, mechanistic studies of
deformation mechanisms that are typically only accessible at extremely low
temperatures. </p>
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