Performance of a small high-speed liquid jet apparatus

The performance of a small high-speed liquid jet apparatus is described. Water jets of 200m/s to 700m/s have been obtained by firing a deformable lead slug from an air rifle into a stainless steel nozzle containing water sealed with a rubber diaphragm. Nozzle devices of using the impact extrusion (IE) method and cumulation (CU) method are designed to generate jets. The injection sequences are visualized using schlieren photography. The difference between the IE and CU methods in the jet generation is found.

Advancing EDL technologies for future space missions : from ground testing facilities to ablative heatshields

Motivated by recent MSL results where the ablation rate of the PICA heatshield was over-predicted, and staying true to the objectives outlined in the NASA Space Technology Roadmaps and Priorities report, this work focuses on advancing EDL technologies for future space missions.

Due to the difficulties in performing flight tests in the hypervelocity regime, a new ground testing facility called the vertical expansion tunnel is proposed. The adverse effects from secondary diaphragm rupture in an expansion tunnel may be reduced or eliminated by orienting the tunnel vertically, matching the test gas pressure and the accelerator gas pressure, and initially separating the test gas from the accelerator gas by density stratification. If some sacrifice of the reservoir conditions can be made, the VET can be utilized in hypervelocity ground testing, without the problems associated with secondary diaphragm rupture.

The performance of different constraints for the Rate-Controlled Constrained-Equilibrium (RCCE) method is investigated in the context of modeling reacting flows characteristic to ground testing facilities, and re-entry conditions. The effectiveness of different constraints are isolated, and new constraints previously unmentioned in the literature are introduced. Three main benefits from the RCCE method were determined: 1) the reduction in number of equations that need to be solved to model a reacting flow; 2) the reduction in stiffness of the system of equations needed to be solved; and 3) the ability to tabulate chemical properties as a function of a constraint once, prior to running a simulation, along with the ability to use the same table for multiple simulations.

Finally, published physical properties of PICA are compiled, and the composition of the pyrolysis gases that form at high temperatures internal to a heatshield is investigated. A necessary link between the composition of the solid resin, and the composition of the pyrolysis gases created is provided. This link, combined with a detailed investigation into a reacting pyrolysis gas mixture, allows a much needed consistent, and thorough description of many of the physical phenomena occurring in a PICA heatshield, and their implications, to be presented.

Through the use of computational fluid mechanics and computational chemistry methods, significant contributions have been made to advancing ground testing facilities, computational methods for reacting flows, and ablation modeling.

Collimation testing using axial intensity

We proposed a new method of measuring the degree of collimation of laser beam using axial intensity information near paraxial focus. Preceding methods for collimation testing are mainly either based on self-imaging or interferometric techniques. The new method is to employ the diffraction behavior of noncollimated wave in circular aperture diaphragm. The principle of the proposed method and experiment results are presented. Due to simplicity of the method and its low cost, it is a promising method for checking the collimation of laser beam. (c) 2005 Published by Elsevier GmbH.

基于同步移相技术的1/4波片快轴方位角的实时测量

提出了一种基于同步移相技术的1/4波片快轴方位角的实时测量方法。由正交光栅、光阑、检偏器组和四象限探测器实现同步移相功能。检偏器组由4个不同方位角的检偏器组成。通过检偏器组的四束光束的光强由四象限探测器同时测量。1/4波片的快轴方位角由这四光束的光强得到。由于该方法不需旋转偏振器件，从而实现的1/4波片的快轴方位角的实时测量。

基于同步移相技术的1/4波片相位延迟量的快速测量

提出了一种基于同步移相技术的1/4波片相位延迟量的快速测量方法。由正交光栅、光阑、检偏器组和四象限探测器实现同步移相功能。检偏器组由4个不同方位角的检偏器组成。通过检偏器组的四束光束的光强由四象限探测器同时测量。1/4波片的相位延迟量由这四光束的光强得到。该方法中波片的快轴不需被事先确定。另外光源光强的波动对测量结果没有影响。通过实验验证了该方法的有效性。

Efeitos benéficos da rosuvastatina na estrutura renal de ratos espontaneamente hipertensos (SHR)

A incidência de doenças renais crônicas está aumentando no mundo, e há uma grande necessidade de identificar as terapias capazes de deter ou reduzir a progressão da doença. Há crescente evidência clínica e experimental de que as estatinas poderiam desempenhar um papel terapêutico. Recentes estudos clínicos e experimentais têm mostrado que as estatinas têm "efeitos pleiotrópicos", além da modulação lipídica. Estudos têm avaliado os efeitos das estatinas sobre a progressão da doença renal crônica, mas os resultados são controversos. Estudos ultra-estruturais em humanos e em ratos demonstraram a presença de junções GAP dentro de todas as células do glomérulo e os podocitos demonstraram conter principalmente conexina-43 (Cx-43). O presente estudo tem como objetivo observar os efeitos da rosuvastatina na estrutura e ultra-estrutura renal e a expressão glomerular de Cx-43 em ratos normotensos (WKY) e em ratos espontaneamente hipertensos (SHR). O foco do estudo foi avaliar os efeitos pleiotrópicos da rosuvastatina em rins de animais hipertensos normocolesterolêmicos. Os ratos foram divididos aleatoriamente em quatro grupos: WKY-C: animais normotensos que não receberam rosuvastatina; WKY-ROS: animais normotensos que receberam rosuvastatina 20mg/kg/dia por gavagem orogástrica; SHR-C: animais hipertensos que não receberam rosuvastatina; SHR-ROS: animais hipertensos que receberam rosuvastatina, como descrito no grupo WKY-ROS. Os animais dos grupos SHR-C e SHR-ROS apresentaram níveis de pressão arterial maiores que os animais dos grupos WKY-C e WKY-Ros. A massa corporal dos grupos de animais não diferiram significativamente durante o experimento. Não houve diferença nos níveis sanguíneos de uréia, creatinina, ácido úrico e creatinafosfoquinase entre os animas dos grupos estudados. No entanto, houve um aumento da excreção de proteína de 24 horas nos animais do grupo SHR-C. Houve um aumento na área capsular nos animais do grupo SHR-C. Por microscopia eletrônica de transmissão observou-se que nos animais SHR-C a barreira de filtração glomerular, o diafragma de fenda e os podócitos estão alterados exibindo os vacúolos nos podócitos e pedicelos mais curtos e mais espessos. Por microscopia eletrônica de varredura, os animais SHR-C exibiram pedicelos mais afilados, curtos e tortuosos. Um aumento da imunofluorescência para Cx-43 foi observada em células epiteliais viscerais dos glomérulos dos animais do grupo WKY-ROS e nas células parietais e viscerais dos glomérulos dos animais do grupo SHR-ROS, se comparado com os grupos WKY-C e SHR-C. Em conclusão, podemos supor que o efeito pleiotrópico renal da rosuvastatina pode ser uma ferramenta terapêutica para melhorar a estrutura e conseqüentemente a função renal em indivíduos hipertensos.

Efeitos da rosuvastatina e da atividade física de baixa intensidade na morfologia renal de ratos normotensos e espontaneamente hipertensos (SHR)

Desordens do sistema renal podem ser as causas da hipertensão arterial, a qual pode, por sua vez, causar doenças renais. A pressão sanguínea elevada é muito comum também nas doenças crônicas dos rins, e é, além disso, um conhecido fator de risco para uma mais rápida progressão da falha renal. A incidência de doenças renais crônicas está aumentando no mundo, e há uma grande necessidade de identificar as terapias capazes de deter ou reduzir a progressão da doença. Há crescente evidência de que as estatinas poderiam desempenhar um papel terapêutico. Além disso, tem sido demonstrado que a atividade física melhora a função renal em pacientes. Estudos ultra-estruturais em humanos e em ratos demonstraram a presença de junções gap dentro de todas as células do glomérulo e os podócitos demonstraram conter principalmente conexina-43 (Cx-43). O presente estudo tem como objetivo observar os efeitos da rosuvastatina e da atividade física de baixa intensidade na estrutura e ultra-estrutura renal e na expressão glomerular de Cx-43 em ratos normotensos (WKY) e em ratos espontaneamente hipertensos (SHR). Os ratos foram divididos aleatoriamente em oito grupos: WKY-C: animais normotensos que não receberam rosuvastatina; WKY-ROS: animais normotensos que receberam rosuvastatina 20mg/kg/dia por gavagem orogástrica; SHR-C: animais hipertensos que não receberam rosuvastatina; SHR-ROS: animais hipertensos que receberam rosuvastatina, como descrito no grupo WKY-ROS; SED-WKY: animais normotensos sedentários; EX-WKY: animais normotensos exercitados; SED-SHR: animais hipertensos sedentários; e, EX-SHR: animais hipertensos exercitados. Os animais dos grupos SHR-C, SHR-ROS e SED-SHR apresentaram níveis de pressão arterial maiores que os animais dos grupos WKY-C, WKY-ROS, SED-WKY, EX-WKY e EX-SHR. A massa corporal dos grupos de animais não diferiram significativamente durante o experimento. Não houve diferença nos níveis sanguíneos de uréia, creatinina, ácido úrico e creatinafosfoquinase entre os animas dos grupos estudados. No entanto, houve um aumento da excreção de proteína de 24 horas nos animais do grupo SHR-C. Houve um aumento na área capsular nos animais do grupo SHR-C. Por microscopia eletrônica de transmissão observou-se que nos animais SHR-C e SED-SHR a barreira de filtração glomerular, o diafragma de fenda e os podócitos estão alterados exibindo os vacúolos nos podócitos e pedicelos mais curtos e mais espessos. Por microscopia eletrônica de varredura, os animais SHR-C e SED-SHR exibiram pedicelos mais afilados, curtos e tortuosos. Um aumento da imunofluorescência para Cx-43 foi observada em células epiteliais viscerais dos glomérulos dos animais do grupo WKY-ROS e nas células parietais e viscerais dos glomérulos dos animais do grupo SHR-ROS, se comparado com os grupos WKY-C e SHR-C. Por outro lado, os animais dos grupos SED-SHR e EX-SHR exibiram diminuição da expressão de Cx-43, comparados aos animais SED-WKY e EX-WKY. Em conclusão, podemos supor que os efeitos renais da rosuvastatina e da atividade física de baixa intensidade podem ser ferramentas terapêuticas para melhorar a estrutura e conseqüentemente a função renal em indivíduos hipertensos

Building damage and repair due to leakage in a deep excavation

The north-south line in Amsterdam is being built underneath the historic centre of the city. Three deep stations are being constructed in deep excavations supported by diaphragm walls. During the excavation for Vijzelgracht station, leakage through the wall resulted in large settlements and damage to historic buildings, which threatened continuation of the project. The authors analysed the cause of the leakage and the damage to the buildings. With the application of robust preventative measures at two of the deep excavations it was possible to continue the project. This paper reports on the cause of the events, the damage to the buildings and the counter-measures taken. It includes lessons learned for the project and for the foundations industry.

Marine Vertebrates and Low Frequency Sound: Technical Report for LFA EIS

Over the past 50 years, economic and technological developments have dramatically increased the human contribution to ambient noise in the ocean. The dominant frequencies of most human-made noise in the ocean is in the low-frequency range (defined as sound energy below 1000Hz), and low-frequency sound (LFS) may travel great distances in the ocean due to the unique propagation characteristics of the deep ocean (Munk et al. 1989). For example, in the Northern Hemisphere oceans low-frequency ambient noise levels have increased by as much as 10 dB during the period from 1950 to 1975 (Urick 1986; review by NRC 1994). Shipping is the overwhelmingly dominant source of low-frequency manmade noise in the ocean, but other sources of manmade LFS including sounds from oil and gas industrial development and production activities (seismic exploration, construction work, drilling, production platforms), and scientific research (e.g., acoustic tomography and thermography, underwater communication). The SURTASS LFA system is an additional source of human-produced LFS in the ocean, contributing sound energy in the 100-500 Hz band. When considering a document that addresses the potential effects of a low-frequency sound source on the marine environment, it is important to focus upon those species that are the most likely to be affected. Important criteria are: 1) the physics of sound as it relates to biological organisms; 2) the nature of the exposure (i.e. duration, frequency, and intensity); and 3) the geographic region in which the sound source will be operated (which, when considered with the distribution of the organisms will determine which species will be exposed). The goal in this section of the LFA/EIS is to examine the status, distribution, abundance, reproduction, foraging behavior, vocal behavior, and known impacts of human activity of those species may be impacted by LFA operations. To focus our efforts, we have examined species that may be physically affected and are found in the region where the LFA source will be operated. The large-scale geographic location of species in relation to the sound source can be determined from the distribution of each species. However, the physical ability for the organism to be impacted depends upon the nature of the sound source (i.e. explosive, impulsive, or non-impulsive); and the acoustic properties of the medium (i.e. seawater) and the organism. Non-impulsive sound is comprised of the movement of particles in a medium. Motion is imparted by a vibrating object (diaphragm of a speaker, vocal chords, etc.). Due to the proximity of the particles in the medium, this motion is transmitted from particle to particle in waves away from the sound source. Because the particle motion is along the same axis as the propagating wave, the waves are longitudinal. Particles move away from then back towards the vibrating source, creating areas of compression (high pressure) and areas of rarefaction (low pressure). As the motion is transferred from one particle to the next, the sound propagates away from the sound source. Wavelength is the distance from one pressure peak to the next. Frequency is the number of waves passing per unit time (Hz). Sound velocity (not to be confused with particle velocity) is the impedance is loosely equivalent to the resistance of a medium to the passage of sound waves (technically it is the ratio of acoustic pressure to particle velocity). A high impedance means that acoustic particle velocity is small for a given pressure (low impedance the opposite). When a sound strikes a boundary between media of different impedances, both reflection and refraction, and a transfer of energy can occur. The intensity of the reflection is a function of the intensity of the sound wave and the impedances of the two media. Two key factors in determining the potential for damage due to a sound source are the intensity of the sound wave and the impedance difference between the two media (impedance mis-match). The bodies of the vast majority of organisms in the ocean (particularly phytoplankton and zooplankton) have similar sound impedence values to that of seawater. As a result, the potential for sound damage is low; organisms are effectively transparent to the sound – it passes through them without transferring damage-causing energy. Due to the considerations above, we have undertaken a detailed analysis of species which met the following criteria: 1) Is the species capable of being physically affected by LFS? Are acoustic impedence mis-matches large enough to enable LFS to have a physical affect or allow the species to sense LFS? 2) Does the proposed SURTASS LFA geographical sphere of acoustic influence overlap the distribution of the species? Species that did not meet the above criteria were excluded from consideration. For example, phytoplankton and zooplankton species lack acoustic impedance mis-matches at low frequencies to expect them to be physically affected SURTASS LFA. Vertebrates are the organisms that fit these criteria and we have accordingly focused our analysis of the affected environment on these vertebrate groups in the world’s oceans: fishes, reptiles, seabirds, pinnipeds, cetaceans, pinnipeds, mustelids, sirenians (Table 1).

Fibre optic monitoring of a deep circular excavation

This paper describes part of the monitoring undertaken at Abbey Mills shaft F, one of the main shafts of Thames Water's Lee tunnel project in London, UK. This shaft, with an external diameter of 30 m and 73 m deep, is one of the largest ever constructed in the UK and consequently penetrates layered and challenging ground conditions (Terrace Gravel, London Clay, Lambeth Group, Thanet Sand Formation, Chalk Formation). Three out of the twenty 1-2 m thick and 84 m deep diaphragm wall panels were equipped with fibre optic instrumentation. Bending and circumferential hoop strains were measured using Brillouin optical time-domain reflectometry and analysis technologies. These measurements showed that the overall radial movement of the wall was very small. Prior to excavation during a dewatering trial, the shaft may have experienced three-dimensional deformation due to differential water pressures. During excavation, the measured hoop and bending strains of the wall in the chalk exceeded the predictions. This appears to be related to the verticality tolerances of the diaphragm wall and lower circumferential hoop stiffness of the diaphragm walls at deep depths. The findings from this case study provide valuable information for future deep shafts in London. © ICE Publishing: All rights reserved.

Fracture Properties of LPCVD Silicon Nitride and Thermally Grown Silicon Oxide Thin Films From the Load-Deflection of Long Si3N4 and SiO2/Si3N4 Diaphragms

The bulge test is successfully extended to the determination of the fracture properties of silicon nitride and oxide thin films. This is achieved by using long diaphragms made of silicon nitride single layers and oxide/nitride bilayers, and applying comprehensive mechanical model that describes the mechanical response of the diaphragms under uniform differential pressure. The model is valid for thin films with arbitrary z-dependent plane-strain modulus and prestress, where z denotes the coordinate perpendicular to the diaphragm. It takes into account the bending rigidity and stretching stiffness of the layered materials and the compliance of the supporting edges. This enables the accurate computation of the load-deflection response and stress distribution throughout the composite diaphragm as a function of the load, in particular at the critical pressure leading to the fracture of the diaphragms. The method is applied to diaphragms made of single layers of 300-nm-thick silicon nitride deposited by low-pressure chemical vapor deposition and composite diaphragms of silicon nitride grown on top of thermal silicon oxide films produced by wet thermal oxidation at 950 degrees C and 1050 degrees C with target thicknesses of 500, 750, and 1000 mn. All films characterized have an amorphous structure. Plane-strain moduli E-ps and prestress levels sigma(0) of 304.8 +/- 12.2 GPa and 1132.3 +/- 34.4 MPa, respectively, are extracted for Si3N4, whereas E-ps = 49.1 +/- 7.4 GPa and sigma(0) = -258.6 +/- 23.1 MPa are obtained for SiO2 films. The fracture data are analyzed using the standardized form of the Weibull distribution. The Si3N4 films present relatively high values of maximum stress at fracture and Weibull moduli, i.e., sigma(max) = 7.89 +/- 0.23 GPa and m = 50.0 +/- 3.6, respectively, when compared to the thermal oxides (sigma(max) = 0.89 +/- 0.07 GPa and m = 12.1 +/- 0.5 for 507-nm-thick 950 degrees C layers). A marginal decrease of sigma(max) with thickness is observed for SiO2, with no significant differences between the films grown at 950 degrees C and 1050 degrees C. Weibull moduli of oxide thin films are found to lie between 4.5 +/- 1.2 and 19.8 +/- 4.2, depending on the oxidation temperature and film thickness.

Fiber Bragg grating hydrophone with high sensitivity

A fiber Bragg grating (FBG) hydrophone with high sensitivity was demonstrated. This hydrophone used a rubber diaphragm and a copper hard core as the sensing element. To compensate the hydrostatic pressure, a capillary tube was fixed at the end of the hydrophone. Theoretical analysis of the acoustic pressure sensitivity was given in this letter. Experiments were carried out to test the frequency response of the hydrophone. The result shows that when the Young's modulus of the diaphragm is higher, a flatter frequency response will be obtained.

Fiber laser hydrophone based on double diaphragms: Theory and experiment

A fiber laser hydrophone with enhanced sensitivity is demonstrated. Two diaphragms with a hard core fixed at each center are used as the sensing element. Theoretical analysis shows that the Young's modulus of the diaphragm and the radius of the hard core have significant effect on the acoustic sensitivity. Experiments are carried out to test this effect and the performance of the hydrophone. The experimental result agrees well with the theoretical result, and a sensitivity of 7 nm/MPa has been achieved.

Fiber Bragg grating pressure sensor with enhanced sensitivity

A novel fiber Bragg grating (FBG) pressure sensor with the enhanced sensitivity has been demonstrated. A piston-like diaphragm with a hard core in the center is used to enhance the sensitivity. Both the theoretical analysis and the experimental result show that the radius of the hard core has significant effect on the pressure sensitivity. When the radius of the hard core is 1.5 mm, a pressure sensitivity of 7.23 nm/MPa has been achieved.

Fiber Bragg grating pressure sensor with ultrahigh sensitivity and reduced temperature sensitivity

A fiber Bragg grating (FBG) pressure sensing scheme based on a flat diaphragm and an L-shaped lever is presented. An L-shaped lever transfers the pressure-induced defection of the flat diaphragm to the axial elongation of the FBG. The curve where the L-shaped lever contacts the diaphragm is a segment of an Archimedes spiral, which is used to enhance the responsivity. Because the thermal expansion coefficient of the quartz-glass L-shaped lever and the steel sensor shell is different, the temperature effect is compensated for by optimizing the dimension parameters. Theoretical analysis is presented, and the experimental results show that an ultrahigh pressure responsivity of 244 pm/kPa and a low temperature responsivity of 2.8 pm/degrees C are achieved. (c) 2009 Society of Photo-Optical Instrumentation Engineers. [DOI 10.1117/1.3081058]