首页> 外文OA文献 >I. Measurement of gf-values for singly ionized chromium using the reflected wave region of a shock tube. II. Experimental investigation of the approach to equilibrium ionization and electronic excitation in shock-heated mixtures of chromium and argon. III. Approximate spectral absorption coefficient calculations for electronic band systems belonging to diatomic molecules
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I. Measurement of gf-values for singly ionized chromium using the reflected wave region of a shock tube. II. Experimental investigation of the approach to equilibrium ionization and electronic excitation in shock-heated mixtures of chromium and argon. III. Approximate spectral absorption coefficient calculations for electronic band systems belonging to diatomic molecules

机译:I.使用激波管的反射波区域测量单电离铬的gf值。 II。铬与氩冲击加热混合物平衡电离和电子激发方法的实验研究。 III。属于双原子分子的电子能带系统的近似光谱吸收系数计算

摘要

NOTE: Text or symbols not renderable in plain ASCII are indicated by [...]. Abstract is included in .pdf document.Part I.Absolute gf-values for 21 lines of singly ionized chromium (Cr II) in the spectral region 3118-4559 [angstroms] are presented. Mixtures of Cr(CO)[subscript 6] and argon, heated by reflected shock waves to temperatures in the range 7920[degrees]K to 8730[degrees]K, were used to measure the emission intensity of ionized chromium lines. A three inch diameter shock tube was employed, with the light being observed along the shock tube axis in order to observe directly the curve of growth of each spectral line. The emitted intensities observed were converted to gf-values by means of a comparison with a calibrated tungsten strip lamp. Results are compared with values obtained from arc spectra by Corliss and Bozman[superscript 1] at the National Bureau of Standards. In general, our results are a factor of 9 below the latter measurements. Possible reasons for this discrepancy are discussed.Part II.An experimental investigation of the approach to equilibrium ionization and electronic excitation for chromium behind shock waves in Cr(CO)[subscript 6]-argon mixtures is described. Mixtures composed of from 0.0043% to 0.036%o Cr(CO)[subscript 6] were heated by reflected shock waves to temperatures between 6170[degrees]K and 8600[degrees]K, and the emission from excited states of Cr I and Cr II was simultaneously measured by photoelectric means with a time resolution of about 3 microseconds. Relaxation toward equilibrium ionization and excited state population was observed to occur within from 12 to 60 microseconds, depending upon the temperature and chromium concentration behind the reflected shock.In measurements in which equilibrium ionization is 95% or more, the populations of excited states of Cr I show a pronounced "overshoot" as these states become populated before ionization has depleted the supply of neutral chromium. From a study of the relaxation of Cr I and Cr II upper state populations, it is concluded that ionization proceeds by a multistep autocatalytic process dominated by collisions between chromium atoms and electrons released in prior ionization of chromium. The dependence of the relaxation rates upon the temperature behind the reflected shock wave and upon the concentration of chromium was determined. If it is assumed that the electron and atom temperatures did not differ appreciably during the relaxation period, the variation in the relaxation rate with temperature indicates a 3.1 [plus or minus] 0.3 ev activation energy for chromium ionization, which is significantly less than the ionization potential (6.74 ev).A simplified reaction mechanism is proposed which qualitatively explains the observed relaxation behavior of Cr I and Cr II.Part III.The spectral absorption coefficients in electronic band systems of diatomic emitters have been computed in the past by models that may be described as "the just overlapping line model" and a model "utilizing a smeared out rotational structure". Although the basic relations are obtained by utilizing somewhat different physical arguments, the resulting equations are, in fact, identical.Spectral absorption coefficients have been calculated for the NO [...]-bands at 2000[degrees]K by using the approximate theoretical relations. The calculated results are in good agreement with estimates derived by numerical calculations in which, however, the absorption coefficient data were averaged over intervals of 2000 cm.[superscript -1].
机译:注意:用[...]表示无法用纯ASCII呈现的文本或符号。 .pdf文件中包括摘要。第一部分。给出了光谱区3118-4559 [埃]中21条单离子化铬(Cr II)的绝对gf值。 Cr(CO)[下标6]和氩气的混合物,通过反射冲击波加热到7920°K至8730°K的温度范围,用于测量电离铬线的发射强度。使用三英寸直径的冲击管,沿着冲击管轴观察光,以便直接观察每个光谱线的生长曲线。通过与校准的钨条灯进行比较,将观察到的发射强度转换为gf值。将结果与国家标准局的Corliss和Bozman [上标1]从电弧光谱获得的值进行比较。通常,我们的结果比后面的测量结果低9倍。讨论了产生这种差异的可能原因。第二部分,对Cr(CO)[下标6]-氩气混合物中冲击波后铬的平衡电离和电子激发方法的实验研究。 Cr(CO)[下标6]组成的0.0043%至0.036%的混合物通过反射冲击波加热到6170°K和8600°K之间的温度,并且Cr I和Cr激发态的发射通过光电手段同时测量II,时间分辨率为约3微秒。根据温度和反射冲击后的铬浓度,在12至60微秒内会发生向平衡电离和激发态种群的弛豫。在平衡电离率为95%或更高的测量中,Cr的激发态种群我显示出明显的“过冲”,因为这些状态在电离耗尽中性铬的供应之前就已经存在。通过对Cr I和Cr II高能态种群弛豫的研究,可以得出结论,电离是通过多步自催化过程进行的,该过程以铬原子与铬的先电离过程中释放的电子之间的碰撞为主。确定了弛豫速率对反射冲击波后面的温度以及铬浓度的依赖性。如果假设在弛豫期间电子和原子的温度没有明显不同,则弛豫率随温度的变化表明铬离子化的活化能为3.1 [正负] 0.3 ev,这大大低于离子化的电离能。电势(6.74 ev)。提出了一种简化的反应机理,定性地解释了Cr I和Cr II的观察到的弛豫行为。第三部分。过去,双原子发射器电子带系统中的光谱吸收系数是通过以下模型计算得出的:被称为“正好重叠的线模型”和“利用涂抹的旋转结构”的模型。尽管基本关系是通过使用一些不同的物理参数获得的,但实际上得出的方程式是相同的。使用近似理论已计算出了在2000°K下NO波段的光谱吸收系数关系。计算结果与通过数值计算得出的估计值非常吻合,在数值计算中,吸收系数数据是在2000 cm的间隔内平均的。[上标-1]。

著录项

  • 作者

    Shackleford William L.;

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  • 年度 1964
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  • 原文格式 PDF
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  • 入库时间 2022-08-20 21:01:20

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