Developing and characterizing bulk metallic glasses for extreme applications

Metallic glasses have typically been treated as a “one size fits all” type of material. Every alloy is considered to have high strength, high hardness, large elastic limits, corrosion resistance, etc. However, similar to traditional crystalline materials, properties are strongly dependent upon the constituent elements, how it was processed, and the conditions under which it will be used. An important distinction which can be made is between metallic glasses and their composites. Charpy impact toughness measurements are performed to determine the effect processing and microstructure have on bulk metallic glass matrix composites (BMGMCs). Samples are suction cast, machined from commercial plates, and semi-solidly forged (SSF). The SSF specimens have been found to have the highest impact toughness due to the coarsening of the dendrites, which occurs during the semi-solid processing stages. Ductile to brittle transition (DTBT) temperatures are measured for a BMGMC. While at room temperature the BMGMC is highly toughened compared to a fully glassy alloy, it undergoes a DTBT by 250 K. At this point, its impact toughness mirrors that of the constituent glassy matrix. In the following chapter, BMGMCs are shown to have the capability of being capacitively welded to form single, monolithic structures. Shear measurements are performed across welded samples, and, at sufficient weld energies, are found to retain the strength of the parent alloy. Cross-sections are inspected via SEM and no visible crystallization of the matrix occurs.

Next, metallic glasses and BMGMCs are formed into sheets and eggbox structures are tested in hypervelocity impacts. Metallic glasses are ideal candidates for protection against micrometeorite orbital debris due to their high hardness and relatively low density. A flat single layer, flat BMG is compared to a BMGMC eggbox and the latter creates a more diffuse projectile cloud after penetration. A three tiered eggbox structure is also tested by firing a 3.17 mm aluminum sphere at 2.7 km/s at it. The projectile penetrates the first two layers, but is successfully contained by the third.

A large series of metallic glass alloys are created and their wear loss is measured in a pin on disk test. Wear is found to vary dramatically among different metallic glasses, with some considerably outperforming the current state-of-the-art crystalline material (most notably Cu₄₃Zr₄₃Al₇Be₇). Others, on the other hand, suffered extensive wear loss. Commercially available Vitreloy 1 lost nearly three times as much mass in wear as alloy prepared in a laboratory setting. No conclusive correlations can be found between any set of mechanical properties (hardness, density, elastic, bulk, or shear modulus, Poisson’s ratio, frictional force, and run in time) and wear loss. Heat treatments are performed on Vitreloy 1 and Cu₄₃Zr₄₃Al₇Be₇. Anneals near the glass transition temperature are found to increase hardness slightly, but decrease wear loss significantly. Crystallization of both alloys leads to dramatic increases in wear resistance. Finally, wear tests under vacuum are performed on the two alloys above. Vitreloy 1 experiences a dramatic decrease in wear loss, while Cu₄₃Zr₄₃Al₇Be₇ has a moderate increase. Meanwhile, gears are fabricated through three techniques: electrical discharge machining of 1 cm by 3 mm cylinders, semisolid forging, and copper mold suction casting. Initial testing finds the pin on disk test to be an accurate predictor of wear performance in gears.

The final chapter explores an exciting technique in the field of additive manufacturing. Laser engineered net shaping (LENS) is a method whereby small amounts of metallic powders are melted by a laser such that shapes and designs can be built layer by layer into a final part. The technique is extended to mixing different powders during melting, so that compositional gradients can be created across a manufactured part. Two compositional gradients are fabricated and characterized. Ti 6Al¬ 4V to pure vanadium was chosen for its combination of high strength and light weight on one end, and high melting point on the other. It was inspected by cross-sectional x-ray diffraction, and only the anticipated phases were present. 304L stainless steel to Invar 36 was created in both pillar and as a radial gradient. It combines strength and weldability along with a zero coefficient of thermal expansion material. Only the austenite phase is found to be present via x-ray diffraction. Coefficient of thermal expansion is measured for four compositions, and it is found to be tunable depending on composition.

Prevalência de sobrepeso e obesidade em adolescentes das regiões Nordeste e Sudeste do Brasil, 1996-1997

A questão nutricional tem sido objeto de interesse da saúde pública, não só em nosso país, como também em outros, independentemente dos diferentes níveis de desenvolvimento. O sobrepeso e a obesidade são considerados agravos nutricionais importantes, cuja frequência vem aumentando entre adolescentes, acarretando consequências negativas, imediatas ou futuras, para a saúde. Este estudo pretende descrever a prevalência de sobrepeso e obesidade em adolescentes, segundo o sexo, nas regiões Nordeste e Sudeste do Brasil, e investigar a sua reação com fatores socioeconômicos e com a prática de atividade física. A investigação tem como base os dados da Pesquisa sobre Padrões de Vida (PPV) do IBGE, realizada entre março de 1995 e março de 1997, nas duas regiões. Dadas as peculiaridades de crescimento e desenvolvimento durante essa fase da vida, somados a ausência de dados sobre maturação sexual, optou-se por incluir os dados de adolescentes de 15 a 19 anos de idade. A amostra contou com os dados de 1027 adolescentes da Região Nordeste e 854 da Região Sudeste com amplo predomínio numérico nas áreas urbanas em ambas regiões.O termo sobrepeso/obesidade foi utilizada para caracterizar os adolescentes que se encontravam com valores de índice de Massa Corporal (IMC) iguais ou acima do percentil 85, de acordo com o sexo e a idade, da distribuição de IMC da população norte americana (WHO, 1995). A análise estatística considerou os fatores de expansão e o desenho da amostra. A prevalência de sobrepeso/obesidade foi de 8,45% IC 95% 6,51-10,90) na Região Nordeste, contra 11,53% (IC 95% 8,90- 14,81) na Região Sudeste. No Nordeste, observou-se maior risco de sobrepeso/obesidade para adolescentes do sexo feminino (razão de prevalência: RP meninas/meninos=3,00; IC 95% 1,73-5,22), situação que se manteve entre os residentes da área urbana (RPr3,21; IC 95% 1,72-5,99) e os da área rural (RP=2,27; IC 95% 0,68-7,60). Na Região Sudeste, o risco de sobrepeso/obesidade foi maior entre os meninos (RP meninas/meninos=0,58; IC 95% 0,37-0,92). Ao se estratificarem os dados por situação de moradia, os residentes da área urbana desta região mantiveram essa diminuição entre meninas (RPO,51; IC 95% 0,31-0,85), porém na área rural houve aumento de risco entre as meninas (RP=1 86; IC 95% 0,83-4,16). A renda per capita domiciliar mensal só associou ao risco de sobrepeso/obesidade, em ambas as regiões, apenas entre as meninos de maior renda per capita domiciliar mensal, quando comparados aos de renda inferior (Região Nordeste: OR bruto=9,64; IC 95% 3,17-29,35 e CR ajustado=10,13; IC 95% 2,83-36,27 e, na Região Sudeste: OR bruto13; IC 95% 1,50-17,48 e OR ajustado=8,70; IC 95% 1,17-32,34). Embora tenha sido observada grande frequência de sedentarismo entre as meninas, a realização de atividade física não se associou a prevalência do sobrepeso/obesidade em nenhuma das regiões estudadas. Os resultados apontam para a necessidade de medidas do controle dessas condições, visando a prevenção de doenças crônicas, bem como da condução de estudos que aprofundem as questões associadas ao risco de sobrepeso/obesidade entre os adolescentes de diferentes regiões do país.

Nuclear reactions leading to energy levels of Ar37 and K37

In view of recent interest in the Cl³⁷ (ʋ solar’^e-)Ar³⁷ reaction cross section, information on some aspects of mass 37 nuclei has been obtained using the K³⁹ (d, ∝) Ar³⁷ and Cl³⁵ (He³, p) Ar³⁷ reactions. Ar³⁷ levels have been found at 0, 1.41, 1.62, 2.22, 2.50, 2.80, 3.17, 3.27, 3.53, 3.61, 3.71, (3.75), (3.90), 3.94, 4.02, (4.21), 4.28, 4.32, 4.40, 4.45, 4.58, 4.63, 4.74, 4.89, 4.98, 5.05, 5.10, 5.13, 5.21, 5.35, 5.41, 5.44, 5.54, 5.58, 5.67, 5.77, and 5.85 MeV (the underlined values correspond to previously tabulated levels). The nuclear temperature calculated from the Ar³⁷ level density is 1.4 MeV. Angular distributions of the lowest six levels with the K³⁹ (d, ∝) Ar³⁷ reaction at E_d = 10 MeV indicate a dominant direct interaction mechanism and the inapplicability of the 2I + 1 rule of the statistical model. Comparison of the spectra obtained with the K³⁹ (d, ∝) Ar³⁷ and Cl³⁵ (He³, p) Ar³⁷ reactions leads to the suggestion that the 5.13-MeV level is the T = 3/2 Cl³⁷ ground state analog. The ground state Q-value of the Ca⁴⁰ (p, ∝) K³⁷ reaction has been measured: -5179 ± 9 keV. This value implies a K³⁷ mass excess of -24804 ± 10 keV. Description of a NMR magnetometer and a sixteen-detector array used in conjunction with a 61-cm double-focusing magnetic spectrometer are included in appendices.