激光烧结石墨烯铜复合材料温度场有限元模拟

在激光烧结石墨烯增强铜基复合材料的过程中,了解瞬时温度场分布对优化工艺参数、控制烧结质量有重要作用。建立了激光烧结预涂在42CrMo基板上的石墨烯铜的混合粉末的有限元模型。研究了激光烧结过程温度场分布,熔池的几何参数以及烧结层与基体的冶金结合宽度。为了验证模拟结果,使用与模拟相同的参数进行了单道激光烧结的实验。研究表明,热传导、热辐射和相变潜热在激光烧结过程的温度场分布中起重要作用。实验结果与模拟结果较为一致。所以可以依据模拟结果预测实验的温度场分布和熔池几何参数,同时也可以据此优化激光烧结参数。     

利用YAG激光去除线缆屏蔽材料

在利用CO2激光器去除绝缘层的基础上,采用YAG激光器去除线缆屏蔽层材料,建立了YAG激光剥离金属材料的理论模型。利用ANSYS软件对激光剥离材料过程进行数值模拟分析,确定了实验所需参数。通过YAG激光对RG113线缆屏蔽层进行了剥离实验,得到了激光功率、扫描速度、脉宽及离焦量对切口宽度和深度及表面质量的影响规律。通过正交实验的极差分析,研究了各工艺参数对切口宽度和深度的影响。结果表明,激光功率对绝缘层切口宽度、切口深度及金属屏蔽层切口深度的影响最强,而激光扫描速度对金属屏蔽层切口宽度的影响最大。     

TA15钛合金激光沉积温度场数值模拟与检测

在综合考虑热源模型、对流辐射换热、相变潜热、材料非线性因素对激光沉积修复温度场影响前提下,建立了激光沉积修复的数学模型,采用有限元参数化设计语言(APDL)对多道多层激光沉积修复温度场进行了数值模拟。研究了激光沉积修复瞬时温度场及其中心高度上节点温度随时间变化情况,分析了修复件中心高度上温度梯度分布情况。搭建了激光沉积修复温度测量系统,对修复时表面温度进行了测量,并与模拟温度进行了比较,两者吻合较好。为控制激光沉积修复组织、提高修复质量提供有效手段。     

高能激光破岩的传热学特性研究

高能激光破岩中激光与岩石相互作用的过程,是一个复杂的非稳定的传热学问题。利用能量守恒原理,得到了激光破岩的传热方程,并对其相变过程中固液相变界面、液气界面上的焓、导热系数和比热等热物性参数进行了近拟简化,从而建立了激光破岩温度场分析的物理模型。利用Galerkin方法,对激光破岩的温度场模型进行了数值分析求解和实例计算。     

毫秒脉冲激光辐照硅基PIN的温度场应力场数值分析

为了研究毫秒脉冲激光辐照硅基PIN多层结构产生的温度场和应力场的特点,本文基于热传导理论和弹塑性力学理论,利用等效比热容法处理相变潜热,考虑多个热源,尤其是底层铝电极反射的影响,并考虑硅基PIN探测器每层材料参数的非线性影响,采用有限元模拟软件COMSOL Multiphysics,对毫秒脉冲激光辐照硅基PIN多层结构的过程进行了二维数值模拟,得到了材料表层及内部各层的瞬态温度场与应力场的时空分布和变化规律.结果表明,底层铝电极对激光的反射,使得在底层铝电极处及附近硅层的温度都略有升高.在此基础上,分析了毫秒脉冲激光辐照硅基PIN的硬破坏机理,即熔融前力学损伤导致硅基PIN探测器的功能失常.     

相变材料模拟金属构件热特性的数值研究

通过理论分析和数值计算论证了用相变材料模拟多种常用金属构件热特性的可行性.利用相变材料模拟了厚度分别为20 mm,30 mm,50 mm和100 mm的金属板材,发现在模拟较厚的金属板材时,相变材料的低导热系数对模拟效果产生了不利影响.在此基础上,利用导热系数增强的相变材料对厚度大于100 mm金属板材进行模拟,取得了较好的模拟效果.并利用相变材料模拟了金属构件轮和管的热特性.     

相变致冷镜的有限元结构优化

 镜体的结构决定了相变致冷镜抑制腔镜在高能激光辐照下的热变形的效果。比较不同结构形式的相变致冷镜镜面热变形的有限元软件计算结果，并通过一阶非线性优化方法，得到较优的放射状结构：硅基基体外径80mm，厚度12.5mm，光斑直径40mm,吸收功率密度为79.58kW/m²，当其最优沟槽深度为99mm，宽度为0.4mm时，光照10s时镜面热变形达到最小值0.37μm。     

熔石英亚表面横向划痕调制作用的3维模拟

建立了熔石英后表面3维横向划痕模型,并采用3维时域有限差分方法对熔石英亚表面划痕周围的电场强度进行了数值模拟,分析了划痕宽度、深度、长度以及划痕倾斜角度对入射光场的调制作用,结果表明:随划痕深度和划痕长度的增加,熔石英内的最大电场强度增大,且当划痕长度达到1μm以上时,最大电场强度趋于稳定;划痕结构因子在1~2之间的划痕较容易引起熔石英损伤;而入射激光在划痕界面和后表面之间发生内全反射时,后表面上的光强增强效果更加明显,因此减少角度范围在20.9°~45°之内的划痕能大幅提高熔石英的损伤阈值。     

超短激光打孔中快速相变的格子玻尔兹曼模拟

采用双重分布函数的格子玻尔兹曼模型，对单脉冲激光金属打孔过程中的快速相变传热进行研究.模型考虑了金属材料熔化后熔体的流动换热，并采用浸没移动边界方案对过程中的固液界面进行追踪.采用纯导热模型和考虑对流的换热模型计算，将结果和试验进行对比，结果表明：在激光打孔过程中熔体的流动对相变传热产生较大影响，采用考虑流动换热模型的结果与实验更接近.进而对熔化速度、熔化深度以及温度场的变化进行分析，并探讨不同激光工艺参数对相变过程的影响.模拟发现一个脉冲结束后，激光的脉宽越大，孔深越小，孔径越大，且最高温度较短脉冲激光越低.     

纯铁相变和层裂损伤的数值模拟

基于Hayes多相状态方程、非平衡相变速率模型、非平衡损伤演化模型和含损伤的本构关系,建立了同时考虑相变和损伤的数值模拟方法。利用该方法对纯铁的对称碰撞实验进行了数值模拟,分析了纯铁的相变和层裂损伤的相互作用。结果表明,纯铁材料中发生相变时,等厚样品中才会发生层裂,并且数值计算的样品自由面速度、层裂位置与实验结果吻合。     

Theoretical and experimental analysis of high power diode laser (HPDL) hardening of AISI 1045 steel

Laser surface hardening makes use of the rapid and cooling cycles produced on metals surfaces exposed to a scanning laser beam without affecting the bulk of the sample. Mechanical and chemical properties of the surface can be enhanced through the metallurgical transformations that take place during the mentioned thermal cycles. Steels and cast irons are the usual materials to be hardened by laser and recently the high power diode lasers (HPDL) became the appropriate tool to carry out this process. In this work, some systematic experiments have been carried out to harden AISI 1045 surface samples by a cw (HPDL) working at different power levels (470, 760 W). The main processing parameters (scanning velocity and density power of the laser beam) were tuned from the prediction realized by the numerical (ANSYS) analysis of the heat conduction involved in the process. Such analysis allowed us to put in evidence the variation of the temperature and the cooling rate of the steel sample surface, affecting the uniformity of the demanding mechanical properties of the surface. In this way, a close-loop temperature control of the surface was justified in order to keep the hardness value within the range required. The formation of martensite phase in the laser treated superficial zone confirmed the hardening of the steel.     

Microstructure and properties of plastic deformed martensite induced by laser shock processing

Firstly, 45# steel was quenched by the NEL-2500A rapidly axial flow CO2 laser. The experimental parameters were the laser power of 750 W, the laser beam diameter of 4 mm, the scanning velocity of 7 mm/s.The thickness of coating layer was 0.1 mm and the width was 8 mm. Secondly, the martensite induced by laser quench was shocked by Nd:YAG laser. The parameters of laser shock processing were the wavelength of 1.06 μm, the pulse duration of 23 ns, and the output energy of 16-20 J. The laser was focused on a spot of φ7 mm. K9 optical glass was used as confinement. The sample was coated with black paint 86-1 (the thickness is about 0.025 mm). By testing and analysis of samples which were treated by laser quench and laser quench+shock with transmission electron microscope (TEM), it was discovered that the surface layer of martensite was deformed plastically by laser shock processing. In the secondary hardened zones,there were a lot of slender secondary twin crystal martensites, dislocation tangles, and cellular dislocations.Compared with that of the hardened zones through laser quench only, the residual stress and mechanical properties of the secondary hardened zones were improved and increased through laser compound method.     

Quick Approximate Calculation on the Transient Temperature Field of Laser Heat Treatment

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激光诱导间质热疗中生物组织的温度场研究

激光诱导间质热疗疗效评估的前提是必须获得准确的激光在不同功率、不同照射时间的生物组织温度场分布.利用多物理场直接耦合分析软件COMSOL Multiphysics构建了在组织光学参量不变情况下的三维有限元传热模型.该模型基于Pennes生物传热方程和轴对称高斯形状的激光光束热源方程,参量针对离体猪肝组织,考虑到了生物组织热物性密度、比热和热导率随温度变化的情况.仿真获得激光功率为0.77 W、0.95 W、1.23 W,照射时间为10~90 s,径向距离0~2 mm范围和轴向距离0~4 mm范围的温度场数据集.利用拟合算法,获得了自变量为激光功率、照射时间、径向距离和轴向距离的生物组织温度场分布模型.将功率为0.88 W和1.05 W时的结果与Pennes方程结果相比较,两者误差在5%以内.     

532nm连续激光晶化非晶硅薄膜的原位拉曼光谱研究

用磁控溅射制备了非晶硅薄膜,用波长为532 nm的连续激光退火和显微Raman光谱原位测试技术和场发射扫描电子显微镜研究了非晶硅薄膜在不同激光功率密度和不同扫描速度下的晶化状态。结果表明,激光照射时间10 s,激光功率密度大于2.929×105W/cm2时,能实现非晶硅薄膜晶化。在激光功率密度为5.093×105W/cm2,扫描速度为10 mm/s时非晶硅开始向多晶硅转化。在5.093×105W/cm2的功率密度下,以1.0 mm/s的扫描速度退火非晶硅薄膜,得到的晶粒直径为740 nm。     

皮秒激光烧蚀Al膜的理论分析与实验验证

为研究Al膜受短脉冲激光作用时的能量传输过程,建立了一维半经典双温热传导模型。根据材料加工过程的熔化现象,对模型的相变区域进行有效设置。通过有限元法求解,得到晶格温度随时间分布的规律。根据自由电子气理论优化了模型,得到Al膜表面反射率和热吸收系数随时间的分布图。得到了激光辐照所产生热电场的分布规律,并分析了电子温度梯度对其影响。描绘出电子漂移运动速度的分布规律,证实激光作用产生的热电场是电子漂移运动的主导因素,发现最大漂移速度位置随时间的延长而加深。对激光作用后的晶格温度进行了区域性分析,定义了过热加热区,并得到激光烧蚀深度随时间的变化关系。实验结果表明,不同功率皮秒激光烧蚀Al膜的深度接近于理论计算结果。     

激光诱导等离子体的气体动力学和燃烧波扩展速度研究

针对激光对熔石英材料产生致燃损伤过程中存在的激光支持燃烧波,考虑激光作用的温度残余、目标形貌的改变、喷溅物质分布、目标表面气流状况的分布等效应,分阶段对激光支持燃烧波的过程进行建模和仿真研究.通过建立二维轴对称气体动力学模型,模拟研究包含逆韧致辐射、热辐射、热传导和对流过程在内的激光能量传输过程.此外,依据激光支持燃烧波在可见光波段具有明显的辐射特征这一特点,利用阴影法测量了激光对熔石英致燃损伤过程中的燃烧波扩展速度,得到了燃烧波演化过程图像.研究结果表明:在平行激光束作用下,燃烧波的传播是稳态的,气体动力学行为比较稳定;在聚焦激光束作用下,燃烧波的传播是非稳态的.模拟结果中得到的激光支持燃烧波扩展速度及气体动力学结构与实验结果和理论推导结果符合得很好,验证了理论模型的正确性.     

Effect of laser surface hardening on the microstructure, hardness and residual stresses of austempered ductile iron grades

A study of the laser surface hardening process of two austempered ductile iron grades, with different austempering treatments has been carried out. Hardening was performed with an infrared continuous wave Nd:YAG laser in cylindrical specimens. The microstructure of the laser hardened samples was investigated using an optical microscope, microhardness profiles were measured and surface and radial residual stresses were studied by an X-ray diffractometer. Similar results were achieved for both materials. A coarse martensite with retained austenite structure was found in the treated area, resulting in a wear resistant effective layer of 0.6 mm to 1 mm with a microhardness between 650 HV and 800 HV. Compressive residual stresses have been found at the hardened area being in agreement with the microhardness and microstructural variations observed. The achieved results point out that the laser surface hardening is a suitable method for improving the mechanical properties of austempered ductile irons.     

Analysis of the absorption mechanism during laser-metal interaction

The present study examines the absorption of a laser beam at different wavelengths by a partially-ionized vapour during the interaction mechanism. The applicability of the theoretical models developed is discussed in detail. The interaction of the high- and low-power intensities of a laser beam with plasma is distinguished. It is shown that different metal vapours at similar temperatures and densities have absorption depths which may differ by an order of magnitude. Even more substantial is the difference between the absorption depths of light from different lasers in common use. It is also shown that the free electron temperature becomes significantly different from the heavy particle temperature for power intensities above the critical level which is typically > 10¹⁴W/m². The free electron velocity distribution has an isotropic part which becomes non-Maxwellian for power intensities greater than the critical power intensity.     

2600W偏振耦合高效率半导体激光光源

将两个中心波长为808 nm,输出功率为1500W的半导体激光叠阵,经过快慢轴准直后,利用半波片将其中一个叠阵的偏振方向旋转90°,使用偏振分光平板的耦合功能,将两个偏振方向相互垂直的激光耦合到一个光路.扩束后再通过焦距为100 mm的聚焦镜组聚焦,提高激光器的亮度.在工作电流为75 A时,输出功率达到了2600 W,...