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1.
活塞激光热负荷就是通过光学转光片改变激光在空间的能量分配比例.结合活塞激光热负荷试验工况,建立了活塞激光热负荷应力场模拟数学物理模型,模型中考虑了材料的热物性参数随温度的变化.结果表明:由于活塞顶凹坑位置靠近通油孔,导致其应力波动幅值比激光辐照区域大;活塞凹坑、通油孔和靠近活塞顶面的活塞内腔由于和冷却介质直接接触,是活...  相似文献   

2.
系统研究了熔石英激光损伤修复后的形貌特征,根据测量数据建立了典型的损伤修复坑三维模型,利用标量衍射理论并结合快速傅里叶变换算法研究了修复坑在351 nm激光辐照下游光场调制的分布规律.研究表明,修复坑引起的光场调制会使得下游不同距离位置处出现环形光场增强区和轴上位置光场增强点;环形光场增强区位置距离修复元件较近,其环形调制极大值主要受修复坑深度的影响,且随修复坑深度的增大而逐渐增加;轴上位置光场增强点位置距离修复元件较远,其轴上调制极大值主要受修复坑边缘凸起高度的影响,且随凸起高度的增大而快速增加;环形调制极大值或轴上调制极大值增大的同时,其分布位置与修复元件之间的距离均会逐渐减小.实验验证表明,利用三维修复坑模型得到的下游光场调制数值模拟结果与实验测量结果具有较好的一致性.本研究结果对控制熔石英元件损伤修复形貌特征以抑制调制增强效应给出了具体的控制方向,对修复工艺的改进与完善提供了非常有意义的参考.  相似文献   

3.
本文对水平槽道内发汗冷却建立了包括主流区、多孔壁面区和致密壁面区在内的完整的物理模型和数学描述, 对耦合传热过程开展了数值模拟,对平板发汗冷却的机理进行了深入的研究。研究表明:发汗冷却减小了壁面处的速度梯度,使下壁面边界层明显增厚;随着冷却流体的注入,壁面处的湍流应力明显增大;湍流应力的最大值向没有发汗冷却的壁面一侧偏移,并且增加了最大湍流应力;边界层的增厚使得发汗冷却区域壁面摩擦阻力系数降低。随着冷却剂流量的增大,壁面温度也随之下降;数值模拟结果与实验结果较好地吻合。  相似文献   

4.
The quality of bonding is often a concern in rubber-to-metal bonded parts with regard to the integrity and stability of the structure. In this study, shearography has been used to detect the out-of-plane deformation of the defects caused by thermal and vacuum stresses. A sample of the vulcanized styrene-butadiene rubber bonded to steel with known artificial voids was prepared and during bonding process a region was glued with thick adhesives. The rubber surface of the sample was inspected in thermal radiation and vacuum modes respectively with a self-designed shearography device. Meanwhile, a numerical simulation was conducted to predict the out-of-plane deformation of the rubber surface in these two stress modes. Results from the numerical simulation and the experiments indicated that the debonding defects could be inspected in both loading modes. In the thermal radiation mode the region with thick adhesives could be identified successfully. This study provides a guideline for quality control of rubber-to-metal structures using an optical method.  相似文献   

5.
Laser-induced thermal stresses on steel surface   总被引:1,自引:0,他引:1  
In laser heat treatment of steels, a thin surface layer of austenite forms during heating and subsequent phase change process in the cooling period. However, thermal stress develops due to high-temperature gradient attainment in the surface vicinity which in turn results in microcrack development at the surface. The present study is carried out to compute the temperature profiles due to step input pulse laser radiation and determine the resulting thermal stresses. The study is extended to include three-step input pulses having the same energy content. This provides the comparison for the influence of the pulse length on the resulting thermal stresses. To validate the theoretical predictions, an experiment is conducted to irradiate the AISI 4142 steel surface by an Nd–YAG laser. Microphotography and EDS analysis of the heated regions are carried out. It is found that considerable thermal stress is eveloped at the workpiece surface due to attainment of high-temperature gradient in this region. In addition, microcracks are observed at the surface of the irradiated spot.  相似文献   

6.
长脉冲激光辐照烧蚀薄片靶会加速物质进而在靶后表面产生凹坑现象,通过凹坑的实验诊断,配合相关的理论模拟,对理解相关物理过程,校验理论程序的相关参数具有很好的参考价值.利用波长13.9 nm的类镍银X射线激光作为探针,诊断了纳秒倍频激光辐照C8H8平面薄片靶产生的等离子体以及加速物质产生的凹坑现象,并利用XRL2D程序对实验现象进行了细致的模拟,电子热传导限流因子选取为0.03时的模拟结果与实验符合比较好.模拟给出凹坑宽度和深度(即薄片加速距离)与实验观测数据定量符  相似文献   

7.
Laser forming is a new forming technology, which deforms a metal sheet using laser-induced thermal stresses. This paper presents an experimental investigation of pulsed laser forming of stainless steel in water and air. The effects of cooling conditions on bending angle and morphology of the heat affected zone (HAZ) are studied. It is shown that the case of the top surface in air and the bottom surface immersed in water has the greatest bending angle based on the forming mechanism of TGM. The water layer above the sample decreases the coupling energy, leading to a small bending angle. For a thin water thickness (1 mm), the water effects on the HAZ are limited. As water layer thickness increases (5 mm), the concave shape of the HAZ is more remarkable and irregular because the shock waves by high laser energy heating water are fully developed. However, the area and the depth of the HAZ become less significant when water thickness is 10 mm due to the long pathway that laser undergoes.  相似文献   

8.
强流脉冲电子束表面改性的物理模型及数值模拟   总被引:8,自引:0,他引:8       下载免费PDF全文
 推导出了强流脉冲电子束处理过程的应力场方程,利用数值模拟,得到了温度场和应力场的分布曲线,分别给出了熔化深度、升降温的速率及温度梯度的大小,准静态应力和热应力波的幅值、应力波的传播及反射过程,利用数值模拟结果对实验中观察到的实验现象熔化深度、材料表层及次表层数微米范围内组织结构的变化及数百微米的硬度提高等给出了解释。  相似文献   

9.
小型轴流CPU风扇的CFD分析   总被引:1,自引:0,他引:1  
轴流风扇被广泛应用于CPU的热管理中,作为散热关键部件,其运行状态是否良好直接影响计算机的散热性能和寿命.本文利用NUMECA的FINE~(TM)/Turbo软件包对两个小型轴流CPU风扇内部流动进行了详细的数值模拟,并与AMCA风洞的试验测试结果进行了验证对比,在此基础上对小型轴流CPU风扇内部流场进行了详细的分析,并探讨了如何提高这类风扇性能数值预测精度的途径.  相似文献   

10.
根据已经建立的紫外准分子激光损伤典型光学材料的理论模型,研究了准分子激光对透明光学材料(石英玻璃)和非透明光学材料(K9玻璃)的损伤特性,并结合实验结果证实了理论模型的有效性。研究表明:在准分子激光对非透明光学材料辐照下,激光光斑半径越大,产生的热应力和温度越小;脉宽越小,产生的热应力越大;随着脉冲数的增加,温度和热应力都逐渐增大。值得注意的是,当重频增加至45 Hz以上时,熔融损伤阈值开始低于应力损伤阈值,这说明当重频增加到一定程度时,非透明光学材料将首先产生熔融损伤,而不再是应力损伤。在准分子激光对透明光学材料辐照下,杂质微粒的半径和掩埋深度对光学材料温度场分布有着重要影响。但当杂质半径和掩埋深度超过一定的数值时,杂质粒子的存在与表面温度并无联系。理论模型能够较好地解释石英玻璃前/后表面相同的初始损伤形貌特征。  相似文献   

11.
Laser cutting of glass using the controlled fracture technique leads to cut path deviation at the leading and trailing edges of the float glass sheet. In this technique, thermal stresses are used to induce the crack, and the material is separated along the cutting path by extending the crack. We show that the cut path deviation is partly due to high magnitudes of thermal stresses generated near the sheet edges. The absorption of intense radiation from the CO2 and diode laser beams in the glass causes local temperature increases and consequently generates different thermal fields and stress distributions due to surface and volumetric heat absorption. In this paper, we report the effect of the CO2 and diode laser wavelength interaction with the float glass and its effect on the magnitudes of thermal stresses generated near the edges of the glass sheet. We simulate the distribution of the thermal stress and temperature using finite-element analysis software Abaqus and validate it against the experimental data. We show that the CO2 laser produces a lower surface quality and a larger cut path deviation at the leading and trailing edges of the glass sheet as compared to the diode laser.  相似文献   

12.
母健  冯国英  杨火木  唐淳  周寿桓 《物理学报》2013,62(12):124204-124204
针对薄片激光介质抽运和温度分布不均匀的问题, 设计了分区域主动冷却控制薄片激光器. 根据热传导方程, 对端面抽运方形薄片激光介质在均匀冷却和分区域主动冷却两种冷却方式下的温度和应力分布进行了模拟计算. 结果显示: 分区域主动冷却能使薄片介质横向温度分布趋于均匀, 相对于均匀冷却时最大温差的改善率达到了约86%, 介质边缘的张应力转变为低值压应力,有效地抑制了热应力炸裂. 搭建了分区域主动冷却控制实验装置, 并进行了验证实验, 实验结果与模拟结果相符. 为薄片激光器的热管理方式提供了新的思路. 关键词: 薄片激光器 端面抽运 分区域主动冷却 数值模拟  相似文献   

13.
准分子激光辐照K9玻璃的热力效应分析   总被引:1,自引:0,他引:1       下载免费PDF全文
基于传热学理论, 利用有限元法对KrF准分子激光辐照K9玻璃样品中的热力效应进行了数值分析, 并比较了脉冲数目和重频对损伤效果的影响。研究表明, 较低的准分子激光能量就能够使K9玻璃在表面和体内产生热应力损伤, 热应力损伤在光斑区域内主要由压缩热应力控制, 在光斑边缘和材料内部则主要由拉伸热应力控制。在激光脉冲结束时刻, 产生的温度和热应力最大, 且热应力以热冲击波的形式在材料内传播, 随时间变化而来回振荡, 逐渐减弱。这种热应力的反复冲击会对材料产生持续的损伤增长效应, 增加了材料的损伤时间, 并使材料更容易断裂。脉冲数目和重复频率对损伤效果有着较大影响, 在高重复频率下, 损伤累积效应明显。  相似文献   

14.
A theoretical model based on a quasi-four-level system is modified to investigate the effect of Yb concentration on performance of continuous-wave Yb:YAG microchip lasers by taking into account temperature-dependent thermal population distribution, temperature-dependent emission cross-section and concentration-dependent fluorescence lifetime, thermal loading, thermal conductivity, and thermal expansion coefficient. The local temperature rise in Yb:YAG crystal caused by the absorbed pump power plays an important role in the laser performance of Yb:YAG microchip lasers working at ambient temperature without actively cooling the sample. The output wavelengths dependent on output coupling, Yb concentration, and pump power level were analyzed quantitatively. The numerical simulation of Yb:YAG microchip lasers is in good agreement with experimental data. The optimized laser operation for Yb:YAG microchip lasers is proposed by varying the thickness and output coupling for different Yb concentrations. The effect of thermal lens, thermal deformation effect, and saturated inversion population distribution inside the Yb:YAG crystal on performance of heavy-doped Yb:YAG microchip lasers are also addressed. PACS 42.55.Xi; 42.70.Hj; 42.55.Rz  相似文献   

15.
测定双层组合介质接触热阻   总被引:2,自引:2,他引:0       下载免费PDF全文
 当激光辐照双层固体组合介质的外表面时,在变物性及界面接触热阻不变的条件下,数值计算了介质内部温度场时空分布。实验测定该双层介质背面对应点的温度曲线,与数值计算的结果进行比较,从而确定介质界面间的接触热阻。  相似文献   

16.
The effects of an anodic oxidation coating on piston temperature distribution and thermal stress are investigated by establishing an inverse heat conduction problem in the form of an optimization problem in an aero-engine. A thermal analysis is carried out for both coated and uncoated pistons at 2100 rpm under 50 and 100% of full load. Specially manufactured metal plugs (templugs) were installed in both kinds of pistons to measure the temperature of every survey station. The effect of the secondary motion of the piston and piston ring on the lubrication oil film was taken into consideration in determining the heat transfer coefficient. There was reasonable agreement between the numerical method and experimental measurement, shown with an error analysis using a third-order polynomial fit technique. Research results showed that the maximum temperature of the anodic oxidation coated piston head increased to 298.5°C and 309.6°C under 50 and 100% of full load, respectively. In addition, there was a temperature reduction in the skirt for the coated piston in contrast to the temperature for the uncoated pistons under 50 and 100% of full load. The temperature distribution and thermal stress in the pin boss were then analyzed. The results indicated an increase of maximum temperature; however, the maximum thermal stress decreased for the anodic oxidation coated piston in the pin boss. Furthermore, a 200-h durability test was performed, proving the thermal load of the piston with anodic oxidation coating would not damage the piston. Also, the effect of the anodic oxidation coating technique on aero-engine emissions was investigated. The anodic oxidation coating for the aero-engine combustion chamber slightly improved CO and HC under 50 and 100% of full load.  相似文献   

17.
固体热容激光器冷却方式的数值模拟   总被引:1,自引:0,他引:1       下载免费PDF全文
 固体热容激光器连续运转一段时间后,需要进行冷却,以进行下一次运转,因此冷却速度直接影响着热容激光器运转的效率和实用性。从热传导方程出发,以沉积热为内热源模型,利用有限元分析方法对激光二极管阵列从4个方向对称泵浦的板条Nd:GGG激光介质的温度场和和热应力场进行了数值模拟。并对冷却阶段分别采用过冷气体、水循环、喷雾、相变冷却方式时的介质温度和应力随时间变化过程进行了模拟。结果表明在相同条件下采用相变冷却方式能在较短时间内将介质冷却到初始温度。  相似文献   

18.
Laser heating of surfaces is involved with heating and cooling cycles. Material response to a laser pulse in the heating cycle is rapid while in the cooling cycle it is gradual. In this case, temperature rises rapidly in the heating cycle while temperature decay is gradual in the cooling cycle. Depending on the laser pulse properties (pulse length and intensity), the rise and fall of temperature profiles change in the surface region of the substrate material. In the present study, an analytical solution for laser heating pulse is presented and a closed-form solution for temperature distribution inside the multilayer assembly is obtained. Steel is considered as top layer while copper is situated below steel in the multilayer assembly. It is found that the analytical solution agrees well with the numerical predictions. Temperature rise in steel is higher than copper. This is due to the thickness of steel, which is larger than the absorption depth. In this case, internal energy gain dominates over the heat conduction in the energy transport process.  相似文献   

19.
Experiments and numerical simulation have shown that the two-phase zone of liquid and solid phases concentration, variable over the coordinate, is formed both at alumina heating by laser radiation and at free melt cooling. During heating this zone is formed only at the initial stage of heating. Its width is not large and is lesser than the depth of the heating laser beam penetration due to the effect of intense heat losses through the crystal by thermal radiation and thermal conductivity.  相似文献   

20.
采用相对论电磁粒子模拟程序研究了飞秒激光等离子体相互作用中产生的电流密度、电场和自生磁场的发展演化过程。介绍了电子的非局域热输运的基本特性以及激光加热过程中温度烧蚀前沿稠密等离子体子区的预热效应、临界面附近的限流效应,以及冕区的反扩散与限流效应,得到了经典Spitzer-Harm理论描述的电子热传导随自生磁场的演化情形。数值模拟表明:在线性强激光作用下,由于电子初始时刻的无规则热运动,在等离子体上激发电磁不稳定性,而不稳定性激发的强电磁场使电子束在非常短的距离内沉积能量,同时对在激光有质动力推开电子时形成的超热电子能量输运产生抑制作用。  相似文献   

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