2018
DOI: 10.1007/s40843-017-9198-4
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Impact of structure and flow-path on in situ synthesis of AlN: Dynamic microstructural evolution of Al-AlN-Si materials

Abstract: The Al-AlN-Si composites were prepared in the gas-in-liquid in situ synthesized flow-reaction-system, which was implemented by a powder metallurgy and reaction sintering route. The experimental results showed that Al-AlN50Si B material (prepared by ball-milling powders) and AlAlN-50Si M material (prepared by mixing powders) exhibited the semi-continuous Si structures and the isolated Si islands, respectively. Subsequently, the Al-AlN-50Si materials were selected as the model materials by phase identification a… Show more

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Cited by 17 publications
(7 citation statements)
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“…For an isothermal, isoviscous, laminar and inertialess ideal gas, the compressible Reynolds equation which governs the gas pressure profiles considering the gaseous rarefaction effects is given below. (5) where p = p/pa is the dimensionless gas film pressure, H = h/Cb is the dimensionless gas film thickness, pa and Cb are the ambient pressure and the radius clearance respectively. φ and λ denotes the dimensionless circumferential angle coordinate and axial coordinate of micobearing normalized by the journal radius R. Λ = 6μωR 2 /paCb 2 is the bearing number or compressibility parameter, μ is the dynamic viscosity of airflow, ω is the rotational speed of journal.…”
Section: Governing Equations For Ultra-thin Gas Film Lubricationmentioning
confidence: 99%
See 1 more Smart Citation
“…For an isothermal, isoviscous, laminar and inertialess ideal gas, the compressible Reynolds equation which governs the gas pressure profiles considering the gaseous rarefaction effects is given below. (5) where p = p/pa is the dimensionless gas film pressure, H = h/Cb is the dimensionless gas film thickness, pa and Cb are the ambient pressure and the radius clearance respectively. φ and λ denotes the dimensionless circumferential angle coordinate and axial coordinate of micobearing normalized by the journal radius R. Λ = 6μωR 2 /paCb 2 is the bearing number or compressibility parameter, μ is the dynamic viscosity of airflow, ω is the rotational speed of journal.…”
Section: Governing Equations For Ultra-thin Gas Film Lubricationmentioning
confidence: 99%
“…Due to the continuous development of rotating machinery for high precision, miniaturization, low energy consumption and long life span. Aerodynamic microbearings are widely used owing to their advantages of simple structure, low friction resistance, no contamination and minimal temperature limitation in comparison with the oil-lubricated bearings and electromagnetic bearings [4][5][6][7]. In these microfluidic applications, the lubricating films between the journals and bearing pads usually become very small and are found to be even smaller than the molecular mean free path [8,9], and the continuum flow of Reynolds equation is no longer valid for describing the rarefied gas flow characteristics.…”
Section: Introductionmentioning
confidence: 99%
“…In the process of questionnaire design, researchers spent much time and energy finding existing questionnaires in this field or in related fields to improve the validity and reliability of the questionnaire [45][46][47][48]. Afterward, researchers referred to those questionnaires and then designed the questionnaire that was used in this study.…”
Section: Questionnaire Designmentioning
confidence: 99%
“…In conventional gas bearing analysis and design procedures, the bearing characteristics are determined by assuming that the fluid flow in the gas films is in isothermal continuum and that the bearing pads are rigid bodies. As the gas film thickness becomes thinner, the flow behaviors of the compressible gas at the micro-scale differ from those at macro-scale, and the continuum theory may lose its usefulness [7][8][9][10]. The effect of gas rarefaction is the most important factor that considerably affects the bearing performance in microfluidic devices.…”
Section: Introductionmentioning
confidence: 99%