首页> 外文学位 >Spectroscopic investigation of the vapor plume during laser processing of AISI 52100 steel using a high brightness diode-pumped Nd:YAG laser.
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Spectroscopic investigation of the vapor plume during laser processing of AISI 52100 steel using a high brightness diode-pumped Nd:YAG laser.

机译:使用高亮度二极管泵浦Nd:YAG激光器对AISI 52100钢进行激光加工期间的蒸气羽流的光谱研究。

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摘要

Laser atomic absorption spectroscopy was employed to investigate the plasma created during processing of AISI 52100 steel with a diode-pumped Nd:YAG slab laser. A tunable ring-dye laser was focused into various points throughout the plume and the dye laser frequency detuned across several low-lying transitions of Fe I. Absorption profiles were collected at time intervals from 3–12μs, average powers from 80–260W and a speed of 0.8mm/s. The absorption profiles were used to calculate atomic densities using an Abel inversion technique and the electronic temperatures via atomic Boltzmann plots. The resulting atomic densities and temperatures of the plume were mapped graphically. Broadening mechanisms were considered, and emission spectroscopy and time-of-flight measurements were also obtained.; Atomic densities were determined for the lower energy levels of three Fe I transitions. The peak densities were on the order of 1016, 1014 and 1013cm−3 for the lower levels of the 446.29, 446.03 and 446.78nm transitions, respectively. Line broadening was determined to be a combination Doppler and Stark broadening. At early delays, as the power increased, the densities of the transitions studied increased at the top portions of the plume. The plume also widened with power. The lifetime of plume atoms in excited states was no more than 12μs.; The peak electronic temperatures within the plume ranged from 4800–7500K. If time averaged, these temperatures were in agreement with time-averaged temperatures from emission spectroscopy. The highest temperatures were at 3μs with cooling rates on the order of 108K/s. The average gas temperature was determined from Doppler widths and found to be 6000K, thus indicating similar electronic and gas temperatures. The kinetic velocity of the iron atoms was on the order of 103m/s and in agreement with time-of-flight velocity measurements.; The depth of penetration in the coupons was 1.3–5.1 mm. The remelt layer was composed of martensite, and the microstructure in the heat affected zone consisted of a mix of spheroidal chromium carbides within a ferrite matrix.; This work represents the first comprehensive characterization of atomic species within a plasma created during processing of a ferrous alloy using a high brightness, diode-pumped Nd:YAG slab laser.
机译:激光原子吸收光谱法用于研究AISI 52100钢在用二极管泵浦Nd:YAG平板激光器加工过程中产生的等离子体。可调式环形染料激光器聚焦在整个羽流中的各个点,染料激光器的频率在Fe I的几个低位跃迁之间失谐。在3–12μs的时间间隔,80-260W的平均功率和1μs的平均功率下收集吸收曲线。速度为0.8mm / s。使用Abel反演技术将吸收曲线用于计算原子密度,并通过原子Boltzmann图来计算电子温度。图形化地绘制了所得的原子密度和羽流温度。考虑了加宽机理,还获得了发射光谱和飞行时间测量。确定了三个Fe I跃迁的较低能级的原子密度。较低的峰值密度约为10 16 ,10 14 和10 13 cm -3 分别为446.29、446.03和446.78nm跃迁的水平。确定线展宽是多普勒和斯塔克展宽的组合。在早期延迟时,随着功率的增加,研究的过渡密度在羽状流的顶部增加。羽流也随着力量而扩大。激发态中羽状原子的寿命不超过12μs。羽流中的电子峰值温度范围为4800-7500K。如果按时间平均,则这些温度与发射光谱的时间平均温度一致。最高温度为3μs,冷却速率为10 8 K / s。由多普勒宽度确定平均气体温度,发现平均温度为6000K,因此表明电子和气体温度相似。铁原子的运动速度约为10 3 m / s,与飞行时间的速度测量结果一致。试样中的穿透深度为1.3-5.1毫米。熔体层由马氏体组成,热影响区的微观结构由铁素体基体中球形碳化铬的混合物组成。这项工作代表了使用高亮度二极管泵浦Nd:YAG平板激光器在铁合金加工过程中在等离子体中产生的等离子体中原子种类的首次全面表征。

著录项

  • 作者

    Douglass, David Mark.;

  • 作者单位

    University of Michigan.;

  • 授予单位 University of Michigan.;
  • 学科 Engineering Mechanical.; Physics Fluid and Plasma.
  • 学位 Ph.D.
  • 年度 2001
  • 页码 249 p.
  • 总页数 249
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 机械、仪表工业;等离子体物理学;
  • 关键词

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