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1.
球墨铸铁QT600-3激光相变硬化数值模拟研究   总被引:2,自引:0,他引:2       下载免费PDF全文
采用商业有限元软件ProCAST,建立了激光相变硬化温度场的3维数值模拟模型,对球墨铸铁QT600-3进行激光相变硬化的数值模拟研究,计算了表面淬火的温度场,根据温度场预测了硬化层的深度和宽度。激光功率在800~1 000 W之间,激光扫描速度在2.000~2.667 mm/s之间,光斑直径在4~5 mm之间时,计算得到的硬化层深度在0.20~0.64 mm之间,硬化层宽度在2.0~3.7 mm之间。球墨铸铁数值模拟结果与试验基本吻合,两者变化趋势一致。  相似文献   

2.
A numerical code for the time-dependent three-dimensional modelling of the laser surface heating for the hardening of metallic materials has been developed by the authors. The temperature-dependence of the thermal properties of the material (stainless steel) is taken into account in the frame of a heating process that doesnt lead to material melting or evaporation. Calculations have been carried out for various dimensions of the parallelepiped-shaped and of the square-shaped spot of the laser beam, as well as for different scanning velocity and for different levels of the laser source power. Various patterns of the laser spot path have also been studied, including a single-pass hardening pattern, a double-pass hardening pattern with and without overlapping, multiple discontinuous and continuous hardening patterns and spiral hardening patterns. The presented results show how the proposed model can be usefully employed in the prediction of the time-evolution of temperature distribution which arises in the workpiece as a consequence of the laser-workpiece interaction under operating conditions typically encountered in industrial applications of the laser hardening process.Received: 29 July 2003, Published online: 30 September 2003PACS: 42.62.Cf Industrial applications - 44.05. + e Analytical and numerical techniques  相似文献   

3.
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。  相似文献   

4.
Smooth poly(methyl methacrylate) (PMMA) films without any droplets were pulsed laser deposited at a wavelength of 248 nm and a laser fluence of 125 mJ/cm2. After deposition at room temperature, the films possess low universal hardness of only 3 N/mm2. Thermal treatments up to 200°C, either during deposition or afterwards, lead to film hardening up to values of 200 N/mm2. Using a combination of complementary methods, two main mechanisms could be made responsible for this temperature induced hardening effect well above the glass transition temperature of 102°C. The first process is induced by the evaporation of chain fragments and low molecular mass material, which are present in the film due to the ablation process, leading to an increase of the average molecular mass and thus to hardening. The second mechanism can be seen in partial cross-linking of the polymer film as soon as chain scission occurs at higher temperatures and the mobility and reactivity of the polymer material is high enough.  相似文献   

5.
LaserTrasformationHardeningforMaterialasMudPumpLinerTANGFurong;MADeyan;PENGShengshang(DepartmentofMechanicalEngineering,south...  相似文献   

6.
激光熔覆中同轴粉末流温度场的数值模拟   总被引:3,自引:0,他引:3  
在激光同轴送粉熔覆中,由于激光与粉末流相互作用,粉末流整体温度分布直接影响激光熔覆的质量.基于非预混燃烧模型,将激光相处理为连续性介质,粉末颗粒相看作离散相物质,建立了激光作用下粉末流的质量、动量和能量方程.用Fluent软件进行了不同激光功率和粉末流速度条件下粉末流整体温度场数值模拟,讨论了各种参数对温度场分布的影响.为了验证该模型的准确度,利用CCD比色测温方法测量了粉末流整体温度场分布.结果表明,数值模拟与CCD检测结果具有良好的一致性,数值模拟结果对激光熔覆具有指导意义.  相似文献   

7.
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。  相似文献   

8.
拉曼散射分析通常使用多谱线He-Ne激光器作为光源。通过建立多谱线He-Ne激光器腔内棱镜组件的有限元模型,并进行热变形分析,得到了棱镜组件的热变形位移结果。讨论了在棱镜角度改变时多谱线He-Ne激光器输出谱线的变化情况,通过实验进一步验证了仿真结果的准确性。结果表明:多谱线He-Ne激光器长时间工作会使温度升高,严重影响其腔内棱镜的偏转角度,使得其输出谱线发生一定的漂移。当腔内温度继续升高到一定值时会导致激光器不出光,此时,应当采取散热装置或者温度控制措施。  相似文献   

9.
绝对式高能量激光能量计温度特性研究   总被引:2,自引:0,他引:2       下载免费PDF全文
对绝对式量热法高能量激光能量计吸收腔的内、外壁温度差特性进行了详细的理论研究和实验验证。用第二非齐次边界条件和第二齐次边界条件的热传导方程分别建立了吸收腔在激光加热过程中和激光加热结束后的温度分布,利用模拟实验对激光照射吸收腔的过程进行模拟,得到内、外壁温度差的实验数据。利用数值模拟法,对理论分析结果作数值分析,理论分析结果与实验数据非常接近,从而证明了在激光加热过程中,虽然吸收腔内外壁存在固定的温度差,但当激光结束后,该温度差将迅速减小,吸收腔达到热平衡。  相似文献   

10.
S Samimi  A Keshavarz 《中国物理 B》2017,26(2):24207-024207
In this paper, the influence of temperature on the intracavity optical parametric oscillator(IOPO) is investigated by using the stimulated temperature-dependent emission cross section of laser crystal. The rate equations under plane wave approximation have been used for simulation of signal output pulse. Results show that the signal output pulse width is decreased by increasing the laser crystal temperature. Also, the signal output energy is increased by the increasing of the laser crystal temperature. The simulation results for IOPO based on Nd:YAG and Nd:YVO_4, show that the signal pulse energies are increased by 3.2 and 5.6 times respectively when the laser crystal temperature increased from 15℃ to 300℃. The presented model indicates that the temperature sensitivity of Nd:YVO_4-based IOPOs is more than that of Nd:YAG-based IOPOs which is expected from a physical point of view.  相似文献   

11.
Optical properties of the InGaN violet and ultraviolet multiple-quantum-well laser diodes are numerically studied with a self-consistent simulation program. Specifically, the performance of the laser diodes of various active region structures, operating in a spectral range from 385 to 410 nm, are investigated and compared. The simulation results indicate that the double-quantum-well laser structure with a peak emission wavelength of 385–410 nm has the lowest threshold current. The characteristic temperature of the single-quantum-well laser structure increases as the peak emission wavelength increases. The triple-quantum-well structure has the largest characteristic temperature when the peak emission wavelength is shorter than 405 nm, while the double-quantum-well structure possesses the largest characteristic temperature when the peak emission wavelength is larger than 405 nm.  相似文献   

12.
ABSTRACT

Ultra-fine grained copper with nanotwins is found to be both strong and ductile. It is expected that nanocrystalline metals with lamella grains will have strain hardening behaviour. The main unsolved issues on strain hardening behaviour of nanocrystalline metals include the effect of stacking fault energy, grain shape, temperature, strain rate, second phase particles, alloy elements, etc. Strain hardening makes strong nanocrystalline metals ductile. The stacking fault energy effects on the strain hardening behaviour are studied by molecular dynamics simulation to investigate the uniaxial tensile deformation of the layer-grained and equiaxed models for metallic materials at 300?K. The results show that the strain hardening is observed during the plastic deformation of the layer-grained models, while strain softening is found in the equiaxed models. The strain hardening index values of the layer-grained models decrease with the decrease of stacking fault energy, which is attributed to the distinct stacking fault width and dislocation density. Forest dislocations are observed in the layer-grained models due to the high dislocation density. The formation of sessile dislocations, such as Lomer–Cottrell dislocation locks and stair-rod dislocations, causes the strain hardening behaviour. The dislocation density in layer-grained models is higher than that in the equiaxed models. Grain morphology affects dislocation density by influencing the dislocation motion distance in grain interior.  相似文献   

13.
Computer simulation is employed for analyzing the dynamics of plasma expansion in nitrogen under a pressure of 103 and 104 Pa after the action of a nanosecond laser pulse on a graphite plate for obtaining carbonitride nanofilms with the help of laser ablation technology. The binary gas mixture is described using a macroscopic quasi-gasdynamic model taking into account momentum and energy transfer between mixture components. The results of simulation are compared for various initial values of temperature and pressure of the laser jet with the results of direct Monte Carlo simulation and with experimental data. The possibility of controlling the shock wave propagation modes after ablation by varying the initial values of gasdynamic parameters is demonstrated. The effect of nitrogen atmosphere on the propagation of the laser jet is studied.  相似文献   

14.
Laser technology has shown fast growth due to its demands in material processing and manufacturing. Laser material processing includes various applications like cutting, welding, drilling, cladding and surface treatment. In laser surface treatment, the material properties at the surface are altered through surface alloying and transformation hardening. In this study, an enthalpy-based computational model is developed for analyzing laser heating and melting of metals. The solution to the problem is obtained by using a finite element method and validated by comparing the results with that given by an analytical solution to a limiting case problem. A solution algorithm and a computational code are developed to estimate the temperature distribution, solid-liquid interface location and shape and size of the molten pool. The computational model is validated by comparing results with a limiting case analytical model. The study is conducted to analyze the heating rate, the heat affected zone, and the shape and size of the molten pool using a Gaussian laser beam.  相似文献   

15.
薄片激光器热效应及其对输出功率的影响   总被引:2,自引:0,他引:2       下载免费PDF全文
赵建涛  冯国英  杨火木  唐淳  陈念江  周寿桓 《物理学报》2012,61(8):84208-084208
建立了光强分布为高斯型的抽运光端面单程抽运时薄片激光器的温度模型, 实验测量了不同抽运功率下薄片介质表面的 温度分布、温度随时间的变化特性以及介质表面的温度差. 采用Hartmann法测量了薄片介质的热焦距. 考虑热焦距随抽运功率的变化, 基于四能级系统薄片激光器的速率方程组, 建立了薄片激光器热效应对输出功率影响的物理模型, 薄片激光器输入-输出功率曲线与实际相符. 所得结果对薄片激光器的设计和优化具有一定的指导意义.  相似文献   

16.
激光时空分布对钢靶温度场及热软化的影响   总被引:1,自引:0,他引:1       下载免费PDF全文
 用有限元模型数值模拟了能量和作用时间相同而时空分布不同的连续波激光辐照下,带涂层钢靶的温度场和热软化分布。结果表明,光强空间分布不同时,靶后表面温度分布虽有不同程度的差别,但材料中部的热软化差别很小,仅热软化的范围略有改变;光强时间分布不同时,靶面温升的历史不同,但最终温度和温度分布都趋于一致。模拟分析结果与实验结果一致。  相似文献   

17.
Physical Simulation of Small bore Copper vapor Laser   总被引:2,自引:0,他引:2  
1IntroductionInrecentyearsthecoppervaporlaser(CVL)hasbeendevelopedrapidly,amarkedachievementhasbeenobtainedonitstheoriesandd...  相似文献   

18.
To further understand the mechanism of laser electrochemical etching metal, it is necessary to describe the temperature field induced by laser heating metal at the liquid–solid interfaces. For solving the complex problem of laser heating a metal immersed in a liquid, the thermal phenomena adjacent to the metal–liquid interface, which was induced by means of irradiating a stainless steel sample immersed in a liquid with an 808 nm semiconductor laser beam, were numerically investigated. Based on a simplified method to solve the transient explosive boiling when a continuous wave (CW) laser heating a material in a liquid, a commercial finite element analysis (FEA) code (ABAQUS) was used to directly solve and model the transient temperature fields of laser micro-patterning metal in a liquid. As known from simulation results, the simulation of laser scanning indicates that it realizes the effect of pulse laser heating owing to laser moving and liquid cooling. Moreover, laser scanning achieves the pattern at a high resolution. At the same time, the experiment phenomena also proved that the simulation results were reasonable.  相似文献   

19.
为深入研究黑腔内激光成丝不稳定性产生和发展,建立了空间束匀滑光束的传播模型,利用三维激光等离子体相互作用程序LAP3D模拟了黑腔物理条件下的大尺度成丝现象。模拟结果可正确描述成丝后光强的束发散现象及谱空间光强分布特征。从激光能量参数角度分析了导致成丝不稳定性发展的物理因素,并讨论了应用空间束匀滑技术抑制成丝不稳定性的局限性。研究表明:空间束匀滑光束发展成丝的能力取决于光斑内小焦斑的成丝表现,当具备成丝能力的小焦斑份额达到一定比例后,就会导致整个空间束匀滑光束成丝,因此对于光斑平均功率密度较高的光束,须考虑结合其他束匀滑手段来抑制成丝发展。  相似文献   

20.
Carbon nanotube was used to carburize the surface of medium carbon steel and mild steel, respectively, by means of laser surface remelting. The slurry of carbon nanotube of ethanol was coated on the surface of the materials prior to laser irradiation. Microstructures, microhardness and wear property of the surface layers treated by different laser performance parameters were studied. Graphite coating was also used for carburizing. The results showed that both carbon nanotube and graphite were dissolved in the surface molten layer, leading a carburized hardening layer on the surface of the substrate. However, different microstructures formed in the carburizing layers, depending mainly on the type of carburization materials, carbon nanotube or graphite. The carbon nanotube hardening layer exhibits a little higher hardness than the graphite hardening layer. The carburized layer greatly increases the wear resistance of the base material.  相似文献   

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