芯内双微孔复合腔结构的光纤法布里-珀罗传感器研究

提出了一种基于芯内双微孔复合结构的全光纤干涉传感器结构,建立了传感器反射光谱的理论模型,给出了反射光谱强度与微孔长度、孔内介质折射率、微孔端面反射与损耗系数以及光纤的特性参数间的关系,并模拟了传感器光谱对温度和折射率变化的响应特性.利用193 nm准分子激光器,在普通单模光纤上加工制作了具有复合腔结构的全光纤多参量传感器,进行了传感实验研究.结果表明,该传感器具有优于99%的温度、折射率线性响应度,对应两套温度和折射率灵敏度分别为-0.172 nm/℃,1050.700 nm/RIU和0.004 nm/℃,48.775 nm/RIU,不仅能够实现温度、折射率以及它们的区分测量,还能够应用于气体压力的测量,测量精度可达0.3 kPa.     

基于正交设计法的直喷式柴油机燃烧系统参数优化匹配研究

通过多维仿真,应用正交设计法对直喷式柴油机燃烧系统参数进行了优化匹配,通过极差分析得出了各因素对有效功率、NOx和soot三种不同优化目标的影响效应及权重大小,通过交互作用分析获得了耦合参数对优化目标的具体影响,两种分析方法均能得出不同优化目标对应的优化参数组合,且优化结果差别不大.对不同优化目标影响权重最大的因素有所不同,但主要集中在涡流比、喷孔数(喷孔直径)和喷油压力三个参数.     

光成像技术用于地铁电阻式制动器热变形的测量

由于瞬间负载大电流产生电热冲击,使得地铁使用的制动电阻器内部电阻片在热力耦合作用下过度变形。为消除接触式传感器本身对温度场和位移场的干扰,对温度和变形均采用了非接触式测量。在温度的测量中,采用了红外线遥感测温仪;在变形的测量中,应用了以数字光栅投影和Gray-code编码法为基础的结构光三维成像技术,对13个不同温度点进行了电阻片的热变形测量。通过系统标定和误差控制,使得变形测量系统的误差在0.1mm以内。非接触式测量是热应力实验研究的发展方向,而光学成像技术在热变形检测中的应用,为热应力的实验研究开辟了新的途径。     

塑料光纤直径测量系统

提出了以可编程逻辑器件为核心的塑料光纤直径在线测量系统,阐述了其工作原理。系统使用发光二极管作为光源、高精度线阵CCD作为图像传感器,简化了光学部分;应用EPLD和双口RAM,提高了信号处理效率;设计了提高测量精度的单片机数据处理算法。实验表明系统的测量范围为0 26～3mm,测量精度在10μm以内,满足塑料光纤直径测量要求。     

双参量偏振调制光纤传感器输出信号的分离与线性化

分析了用一个传感头实现双参量测量的偏振调制光纤传感器的工作原理，表明该传感器能同时输出两路信号，其中一路利用泡克耳斯效应测电压或利用光弹效应测压力，另一种利用旋光效应测温度。但其输出的两个测量参量之间存在交叉敏感现象，并且其输出呈明显的非线性。因此提出一种基于人工神经网络的双参量偏振调制光纤传感器输出信号分离与线性化方法。以传感器输出作为输入样本，测量参量的实际值作为输出样本，通过训练使神经网络建立传感器输出与其实际感受的测量值之间的复杂非线性关系。计算机仿真与实验结果表明，该方法不仅能在较宽的测量范围内有效地分离两个测量参量，而且能在神经网络的输出端得到理想的线性输出。     

基于双CCD的大型轴类零件直径非接触检测方法研究

针对重型机械工业生产中对大型轴类零件外径测量的需求,基于双CCD传感器测量原理研究了一种新型高效率、高精度的轴径检测方法。介绍了CCD测径系统的检测原理,针对单一CCD传感器测量范围小的缺点,提出了双CCD传感器组合测量大型轴类零件直径(Φ150mm~Φ300mm)的方法,并对影响精度的主要误差来源进行了分析。为了验证该方法的有效性,通过对7种不同直径的标准轴件进行测量,实验表明,测量精度小于±3μm,满足大型轴类零件外径测量的要求。     

一种基于模间干涉的亚波长直径光纤气体折射率传感

设计了一种基于模间干涉的亚波长直径光纤气体折射率传感方案,并分析了其测量灵敏度.将标准单模光纤和一段仅传输基模与二阶模的无包层亚波长直径光纤结合形成传感头,通过分析传感头外气体折射率的变化对两个模式干涉谱峰值移动的影响,研究了这种传感器的折射率测量灵敏度.结果表明,这种传感器的灵敏度高于利用折射率引导型光子晶体光纤的基于模间干涉的折射率传感器.因为没有气体向微孔扩散的过程,这种基于模间干涉的亚波长光纤折射率传感器可用于实时探测.     

一种基于模间干涉的亚波长直径光纤气体折射率传感

设计了一种基于模间干涉的亚波长直径光纤气体折射率传感方案,并分析了其测量灵敏度.将标准单模光纤和一段仅传输基模与二阶模的无包层亚波长直径光纤结合形成传感头,通过分析传感头外气体折射率的变化对两个模式干涉谱峰值移动的影响,研究了这种传感器的折射率测量灵敏度.结果表明,这种传感器的灵敏度高于利用折射率引导型光子晶体光纤的基于模间干涉的折射率传感器.因为没有气体向微孔扩散的过程,这种基于模间干涉的亚波长光纤折射率传感器可用于实时探测.     

一种测量大型原木内部水分的微型NMR 传感器

木材中的水分对木材的性能有着决定性的影响,目前测量木材水分的方法多适用于小型木材的检测．然而,当树木被砍伐后,在加工前希望了解其内部水分状态,因此需要一种方法来检测大型原木的水分．该文设计了一种微型核磁共振(NMR)传感器,该传感器为圆柱型结构（直径为 28 mm,长度为 60 mm）,测量区域位于传感器外侧,形成与传感器同轴的圆环．测量前,需在被测部位凿一个与传感器直径相当的孔．测量时传感器沿着孔壁测量即可获得对应位置的 NMR 参数信息．初步实验结果表明,该传感器可以分辨被测木材中自由水和束缚水的分布以及各部位水分的相对含量．

     

大口径红外成像系统的光学设计

推导了以反射式两镜系统为主体的红外成像系统中满足光瞳匹配要求的转像透镜的高斯光学参量与两镜系统参量的关系式。当选定红外焦平面的冷屏直径及到焦面的距离后，转像透镜与两镜系统的高斯光学参量之间必须满足这个关系式，才能做到光瞳匹配，这就是冷屏为系统的出瞳．而入瞳是主反射镜的口径。消像差由主镜、副镜的非球面及转像透镜上的一个非球面承担。用实例计算验证了所推导出的公式的可靠性，红外系统的口径取为250mm，红外接收器的冷屏直径为5mm，冷屏到红外像面的距离为20mm。两镜系统主镜的曲率半径选定为-1000mm及-800mm两个值，两镜系统焦距为2000mm，1500mm及1000nm三个。共计算了六种结构参量不同的系统。     

Micro-hole fabricated inside FOTURAN glass using femtosecond laser writing and chemical etching

Vertical micro-holes were fabricated inside a photosensitive glass (FOTURAN) by focused femtosecond laser (λ = 775 nm) writing, followed by heat treatment and wet chemical etching in 8% hydrofluoric acid solution for 50 min. The micro-holes were analyzed by optical and scanning electron microscopy, and was found they own circular cross-section and clear edge. At present, micro-holes with aspect ratio of about 7 is achieved. By varying the incident laser fluence in a range of 2.3–36.2 J/cm² and the laser writing velocity in 100–1000 μm/s, the influences of femtosecond laser parameters on the formation of micro-holes are characterized as that: writing velocities hardly affect the micro-hole diameter, while relatively lower laser fluences result in smaller diameter, and the cross-section is more circular in this case. The possible reason for this phenomenon is discussed.     

Optical diagnostics of diesel spray injections and combustion in a high-pressure high-temperature cell

We report on spatially and temporally resolved optical diagnostic measurements of propagation and combustion of diesel sprays introduced through a single-hole fuel injector into a constant volume, high-temperature, high-pressure cell. From shadowgraphy images in non-reacting environments of pure nitrogen, penetration lengths and dispersion angles were determined for non-vaporizing and vaporizing conditions, and found to be in reasonable agreement with standard models for liquid jet propagation and break-up.Quasi-simultaneous two-dimensional images were obtained of laser elastic light scattering, shadowgraphs and spectrally integrated flame emission in a reacting environment (cell temperature 850 K). In addition laser-induced incandescence was employed for the identification of soot-loaded regions. The simultaneously recorded spray images exhibit remarkable structural similarity and provide complementary information about the spray propagation and combustion process. The measurements also reveal the fuel vapor cloud extending well beyond the liquid core and close to the nozzle tip. Ignition takes place close to the tip of the spray within the mixing layer of fuel vapor and surrounding air. Soot is formed in the vapor core region at the tip of the liquid fuel jet. Our results support recently developed phenomenological model on diesel spray combustion.     

Ballistic imaging of liquid breakup processes in dense sprays

Ballistic imaging is the name applied to a category of optical techniques that were originally developed for medical applications. Recently, ballistic imaging was adapted to acquire instantaneous images of the liquid core inside atomizing sprays; a region that has been heretofore inaccessible to spray researchers. An important difference between spray research and the medical imaging problem is the need for high fidelity single-shot (within 10 μs) imaging in a spray whereas stationary tissue images can be averaged. Transient ballistic imaging diagnostics have been used to reveal details of the primary breakup process in a LOX injector, a turbulent water jet, a water jet in cross-flow, a transient diesel fuel spray, a rocket fuel injector, and an aerated spray. This paper briefly discusses various methods for imaging the liquid core, it introduces ballistic imaging and provides specific examples, it describes detailed studies of photon transmission through dense media, and it then discusses incorporation of those results into a model for a ballistic imaging instrument that can evaluate and optimize various concepts.     

Comparison of the Optical Connectivity Method to X-Ray spray measurements in the near field of a diesel injector

For diesel sprays, the primary breakup processes are only rarely understood due to the high optical density and the resulting difficulties to measure them with extremely high spatial and sufficient temporal resolution. The Optical Connectivity Method (OCM) has been proposed in the last years to allow the determination of the breakup length of the connected liquid core, thus giving a measurement quantity of the primary breakup. In this work, an improved optical setup of the OCM is applied to a three-hole test injector nozzle where several measurement techniques are compared currently under well-defined conditions up to 100?MPa injection pressure. In this work, the direct comparison with X-Ray measurements done at the Advanced Photon Source of the Argonne National Laboratory will be described. This allows an evaluation of the OCM technique and a comparison of the different measurement quantities in the first 500?µm range of the spray. The structure of the spray is measured by X-Ray phase contrast imaging and the fuel mass distribution is measured by X-Ray absorption imaging. A detailed comparison of the two X-Ray techniques and the OCM technique has been possible for the first time. It is found that the measurement data of the spray near field are very congruent with all three methods. Due to this comparison, the measurement of the non-perturbed length, which describes the distance from the nozzle orifice up to the point where the formation of surface disturbances is starting, by the OCM is validated for the first time. Within this non-perturbed length of the spray, the OCM signal is weak before it starts to illuminate from the scattering of the perturbed surface. Thus, the OCM technique can deliver two characteristic length scales, the non-perturbed length and the breakup length, characterizing the primary spray breakup.     

Wetting process of electrolyte in high density Cu/Sn micro-bumps electrodepositing

Wetting process of electrolyte in high density Cu/Sn micro-bumps electrodepositing is reported in this paper. Three methods were adopted to enable electrolyte to permeate photo-etching micro-holes with high aspect ratio, including plasma treatment, adding wetting additive in electrolyte and mechanical action. Wettability of the samples with electrolyte was improved by the first two methods, according to contact angle and surface tension measurement. However, electrolyte still cannot reach up to the bottom of micro-hole. And then, electrolyte was subjected to mechanical action, including agitation and ultrasonic vibration. Under mechanical action, void free Cu/Sn micro-bumps fabrication was achieved in photo-etching micro-holes with depth of 60 μm and radius of 30 μm. At last, we proposed a model to show wetting process of electrolyte in photo-etching micro-holes.     

含甲缩醛柴油喷雾和燃烧排放特性的试验研究

应用激光相位多普勒技术测量了含甲缩醛柴油喷雾的速度场和粒径场,在直喷式柴油机上研究了该含氧混合燃油的燃烧排放特性。结果表明,添加甲缩醛可改善柴油的雾化,增加喷雾轴线上的粒子速度,但减小喷雾锥角;同时以远大于其加入的比例降低柴油机排气烟度,但对氮氧化物的排放影响不大。柴油机采用甲缩醛作燃油添加剂时,需改造燃油系统。     

343 nm飞秒激光制备微孔阵列以增强聚氨酯合成革透湿性

为了提高聚氨酯(PU)合成革透湿性,分别使用343 nm飞秒激光和作为对比的1030 nm飞秒激光及1064 nm纳秒激光制备微孔阵列。采用扫描电镜(SEM)和3D激光扫描显微镜对比研究了微孔形貌。结果表明,343 nm飞秒激光可以制备出效果最佳的微孔。此外,分析了3种激光与PU涂层的作用机理,揭示了343 nm飞秒激光合成革微钻孔过程仅表现为光化学烧蚀,光化学和光热烧蚀同时发生于1030 nm飞秒激光钻孔过程,而1064 nm纳秒激光只显示了光热烧蚀。激光合成革表面钻孔后,测量其透湿性和抗张力。结果显示: 微孔密度越大,皮革透湿性(WVP)越大而抗张力越低,脉冲重叠的增加会导致WVP的增加和抗张力的下降;同时,随着脉冲重叠从91.7%降到50%,微孔直径从45 μm降低到30 μm,而微孔锥度从0.7°增加到12.1°;当脉冲重叠率为91.7%,微孔密度为2550/cm2时,最大的WVP增长率为306%。     

Simultaneous rainbow schlieren deflectometry and OH* chemiluminescence imaging of a diesel spray flame in constant pressure flow rig

The physical and chemical phenomena that take place during fuel injection, entrainment and fuel-air mixing, cool-flame and ignition reaction, and combustion in diesel sprays still require extensive study. Global parameters such as liquid and vapor jet penetration lengths and spreading rates render useful yet still limited information. Understanding of the temporal evolution of the spray as it progresses through various steps is needed to develop advanced clean combustion modes and high-fidelity predictive models with sufficient accuracy. In this study, high-speed rainbow schlieren deflectometry (RSD) and OH* chemiluminescence are used to simultaneously image fuel-air mixing, cool-flame reactions, ignition, flame propagation and stabilization, and combustion in a transient diesel-like flame. A constant pressure flow rig (CPFR) is used to conduct multiple injections in quick succession to obtain a statistically relevant dataset. n-heptane was injected at nominal supply pressure of 1000 bar from a single-hole diesel injector into ambient at pressure of 30 bar and temperature of 800 K. About 500 injections were performed and analyzed to reveal structural features of non-reacting and reacting regions of the spray, quantify jet penetration and spreading rates, and study cool-flame behavior, ignition, flame propagation and stabilization at lift-off length, and combustion at upstream and downstream locations.     

Spray diagnostics using an all-solid-state Nd:YAlO<Subscript>3</Subscript> laser and fluorescence tracers in commercial gasoline and diesel fuels

A new diode-pumped Nd:YAlO₃ laser system emitting pulse bursts at 671 nm has made it possible to apply tracer-laser-induced-fluorescence (LIF) techniques for spray diagnostics not only by using model fuels but in real diesel or gasoline fuel sprays. In this work we characterize possible candidates for LIF tracers that can be excited in the wavelength region of 650–680 nm where commercial diesel fuel is transparent. Two fluorescent dyes, Rhodamine 800 and Atto 680, were identified as possible tracers and tested for their relative fluorescence quantum yield and absorption cross section in a diesel fuel environment as well as their behavior at different temperatures. First results of laser-dropsizing experiments with Rhodamine 800 as a fluorescence tracer are presented. PACS 42.62.Fi; 32.50.+d; 42.62.Cf     

气液两相流速度及粒径分布激光干涉测量方法的研究

为了实现对气液两相流的粒子粒径、空间分布及其速度测量。对激光干涉气液两相流测量技术（ILIDS）进行了深入研究,该技术是一种应州于气液两相流测量的新技术,其主要优点是不干扰流场和颗粒粒径、位置测量精度高。基于该技术所开发的图像自动处理方法可以利用普通粒子成像测量技术系统拍摄气液两相流的激光散射干涉图像。并利用图像卷积定位、傅里叶变换频率分析及其图像互相关测速等图像处理手段从干涉图像中自动提取粒子的位置、直径和速度信息。为了验证该方法的测量精度,对喷嘴生成的气水两相流进行了测量实验,得到了喷嘴出口处不同区域的粒径、速度矢量的空间分布,并将测得的速度矢量与用粒子成像测量技术方法测得的结果进行对比,证明两种方法测量的平均速度差别仅为0．38％。