共查询到20条相似文献,搜索用时 125 毫秒
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莫塞莱公式与屏蔽常数 总被引:1,自引:0,他引:1
本文分析了莫塞莱公式v=R(Z-1)2(1/1~2-1/2~2)的近似性质,指出它只对Z=17—28区间的原子才是比较准确的.本文论证了公式中(Z-1)里的数字1不是真正的屏蔽常数σ,从而认为不能把R(Z-1)2/1~2和R(Z-1)2/2~2理解成K与L光谱项.最后,计算出了K、L壳层的屏蔽常数σ、σ. 相似文献
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ZK、ZF、ZBaF、LaK光学玻璃的腐蚀与防护 总被引:3,自引:1,他引:2
ZK、ZF、ZBaF、LaK等光学玻璃在抛光过程中及抛光下盘以后的腐蚀问题,长期以来一直影响着这些光学玻璃零件的加工质量和生产效率。通过对光学玻璃在抛光过程中稳定性课题的研究和生产实验,研制并筛选出比较理想的光学玻璃抛光添加剂;即在这些化学稳定性差的光学玻璃抛光液中,添加适当的pH值调节剂及表面稳定剂,减少了ZK、ZF、ZBaF、LaK等系列化学稳定性差的光学玻璃在抛光过程中的腐蚀问题,显著提高了抛光表面质量和合格率,并进一步提高了光学玻璃零件加工的效率和效益及其工艺技术水平 相似文献
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应用二次量子化和不可约张量理论,由4个产生一湮灭算子耦合成准旋一角动量标量算子Z(K),K为参数。计算表明:Z(K)的本片值有很强的分类功能,能对j≤15/2壳层准旋一角动量耦记完全分类(用准旋和角努量只能对j≤7/2壳层耦合态完全分类)讨论Z(K)的构造和它的本片值的计算方法,给出j≤15/2壳层耦合态的完全分类。 相似文献
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本文介绍了用Z函数简化的铂电阻温度计分度方法和实验装置,在63.15K至273.15K温度范围内对铂电阻进行温度分度,共精度可优于0.05K。 相似文献
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KrFH体系的势能函数与反应动力学研究:(Ⅰ)基态KrFH的分析… 总被引:3,自引:1,他引:2
使用abinitioHEF/LANL2DZ方法优化出了基态KrHF为C∞v,基态KrFH为Cs结构,同时,计算了平衡几何和离解能,并用abinitio计算MP2/LANL2DZ方法计算了谐性力学常数。应用多体项展式法导出了KrFH体系的分析势能函数,研究了势能面上的主要特征。 相似文献
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使用abinitio计算HF/LANL2DZ方法优化出了基态KrHF为C∞v结构,而基态KrFH为Cs结构,同时,计算了平衡几何和离解能,并用abinitio计算MP2/LANL2DZ方法计算了谐性力常数。应用多体项展式法导出了KrFH(X1A′)体系的分析势能函数,研究了势能面上的主要特征 相似文献
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描述氨水体系VLE行为适宜热力学模型的研究 总被引:2,自引:0,他引:2
基于对氨/水体系气液平衡研究的文献调查,选择了Guillevic等提出的一套等温数据为工作基础,本文研究了状态方程法与活度系数法对氨/水体系气液平衡性质预测的适用性.其中状态方程法分别选用理想体系的计算方法、BWR方程、SR-Polar方程、LK-P方程和RKS方程;活度系数法是基于气相选用RKS方程,液相分别选用NRTL模型、电解质NRTL模型、UNIQUAC模型、UNIFAC模型和Wilson方程。本研究发现,活度系数法并没有良好表现,而 LK-P方程和 RKS方程对氨/水体系气液平衡性质预测的适用性显然优于其它方法。 相似文献
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大家知道同轴圆柱形电容器的电容和电场,如果是同轴圆弧柱形电容器,其电容和电场强度该是怎样?本文对此进行探讨,供教学参考. 选取长为L的同轴共圆心角圆弧柱形电容器,其横截面如图1,已知共圆心角θ,半径为R1和R2(R2>R1)的两个圆弧形导体之间的电压为U0,所带电量为±Q,处在真空中(忽略边缘效应),由于是平面场问题,可用复变函数来计算. 设复函数 Z=x+iy,则ζ(z)=ζ(x,y)+iη(x,y)称复变函数,其中 Z(x,y)所确定的平面称z平面,ζ(ξ,η)所确定的平面称ζ平面. 选对数函数… 相似文献
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分析了直冷电冰箱单路、双路、多路循环及双机、双级制冷循环,进行了系统匹配性、市场占有率、成本及其COP值比较。针对双路循环存在的频繁开停机现象,提出了完善控制方式及采用双稳态电磁阀的变温技术。变温室蒸发器与冷冻室蒸发器串联,其前串联双稳态电磁阀2,并在变温室蒸发器上并联双稳态电磁阀1,据变温室温度设定改变双稳态电磁阀通断实现两个循环支路交替制冷。冷藏室温度控制压缩机启停,变温室温度仅控制双稳态电磁阀通断,实现切换制冷剂流向目的。应用该循环方式及相关措施研制的BCD-188CH直冷电冰箱最大负荷日耗电0.38度,变温情况下耗电在0.35度以下,最低达0.31度。 相似文献
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利用同步辐射真空紫外单光子电离结合分子束质谱技术,对当量比φ=1.5的低压预混层流二甲醚火焰进行了实验研究。通过测量光电离质谱和光电离效率曲线,探测到了二甲醚/氧气/氩气的燃烧产物和火焰中间物,包括不稳定的分子和自由基。通过测量离子信号的空间分布曲线,计算了二甲醚/氧气/氩气火焰的主要物种C_2H_6O、O_2、Ar、H_2、H_2O、CO和CO_2的摩尔分数曲线,以及主要中间物种如CH_2O、C_2H_2、C_2H_4、CH_3OH、C_2H_2O、C_2H_4O、CH_3、CH_4、HCO、C_3H_3和C_3H_4的摩尔分数曲线,并分析了主要中间物种的产生和消耗过程。 相似文献
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I. S. Burns N. Lamoureux C. F. Kaminski J. Hult P. Desgroux 《Applied physics. B, Lasers and optics》2008,93(4):907-914
Temperature measurements have been performed in a low-pressure flame by the technique of diode laser induced atomic fluorescence.
The experiments were done in a near-stoichiometric flat-flame of premixed methane, oxygen and nitrogen, at a pressure of 5.3
kPa. Indium atoms were seeded to the flame and probed using blue diode lasers; the lineshapes of the resulting fluorescence
spectra were used to determine the flame temperature at a range of heights above the burner plate. The particular issues associated
with the implementation of this measurement approach at low pressure are discussed, and it is shown to work especially well
under these conditions. The atomic fluorescence lineshape thermometry technique is quicker to perform and requires less elaborate
equipment than other methods that have previously been implemented in low-pressure flames, including OH-LIF and NO-LIF. There
was sufficient indium present to perform measurements at all locations in the flame, including in the pre-heat zone close
to the burner plate. Two sets of temperature measurements have been independently performed by using two different diode lasers
to probe two separate transitions in atomic indium. The good agreement between the two sets of data provides a validation
of the technique. By comparing thermocouple profiles recorded with and without seeding of the flame, we demonstrate that any
influence of seeding on the flame temperature is negligible. The overall uncertainty of the measurements reported here is
estimated to be ±2.5% in the burnt gas region. 相似文献
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《Proceedings of the Combustion Institute》2023,39(1):909-918
In spray-flame synthesis of nanoparticles, a precise understanding of the reaction processes is necessary to find optimal process parameters for the formation of the desired products. Coupling the chemistries of flame, solvent, and gas-phase species initially formed from the particle precursor in combination with the complex flow geometry of the spray flame means a special challenge for the modeling of the reaction processes. A new burner has been developed that is capable to observe the reaction of precursor solutions frequently used in spray-flame synthesis. The burner provides an almost flat, laminar, and steady flame with homogeneous addition of a fine aerosol and thus enables detailed investigation and modeling of the coupled reactions independent of spray formation and turbulent mixing. With its two separate supply channel matrices, the burner also enables the use of reactants that would otherwise react with each other already before reaching the flame. These features enable the investigation of a wide range of flame-based synthesis methods for nanoparticles and, due to the flat-flame geometry, kinetics models for these processes can be developed and validated. This work describes the matrix burner development and its gas flow optimization by simulation. Droplet-size distributions generated by ultrasonic nebulization and their interaction with the burner structure are investigated by phase-Doppler anemometry. As an example for nanoparticle-forming flames from solutions, iron-oxide nanoparticle-generating flames using iron(III) nitrate nonahydrate dissolved in 1-butanol were investigated. This effort includes measurements of two-dimensional maps of the flame temperature by a thermocouple and height-dependent concentration profiles of the main species by time-of-flight mass spectrometry. Experimental data are compared with 1D simulations using a reduced reaction mechanism. The results show that the new burner is well suited for the development of reaction models for precursors supplied in the liquid phase usually applied in spray-flame synthesis configurations. 相似文献
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Radial distribution of OH diffusion in silica glass preform during jacketing process using a oxy-hydrogen burner was investigated by FTIR spectroscopy. The OH peaks at the jacketing boundary and the surface of the preform were found to be due to diffusion of OH incorporated from the burner. 相似文献