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The cataphoretic emitter effect exhibited in high intensity discharge lamp electrodes

机译:在高强度放电灯电极中展出的脱位发射器效果

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A mono-layer of atoms, electropositive with respect to the substrate atoms, forms a dipole layer, reducing its work function. Such a layer is generated by diffusion of emitter material from the interior of the substrate, by vapour deposition or by deposition of emitter material onto arc electrodes by cataphoresis. This cataphoretic emitter effect is investigated within metal halide lamps with transparent YAG ceramic burners, and within model lamps. Within the YAG lamps, arcs are operated with switched-dc current between rod shaped tungsten electrodes in high pressure Hg vapour seeded with metal iodides. Within the model lamps, dc arcs are operated between rod-shaped tungsten electrodes-one doped-in atmospheric pressure Ar. Electrode temperatures are determined by 1 lambda-pyrometry, combined with simulation of the electrode heat balance. Plasma temperatures, atom and ion densities of emitter material are determined by emission and absorption spectroscopy. Phase resolved measurements in YAG lamps seeded with CeI3, CsI, DyI3, TmI3 and LaI3 show, within the cathodic half period, a reduction of the electrode temperature and an enhanced metal ion density in front of the electrode, and an opposite behavior after phase reversal. With increasing operating frequency, the state of the cathode overlaps onto the anodic phase-except for Cs, being low in adsorption energy. Generally, the phase averaged electrode tip temperature is reduced by seeding a lamp with emitter material; its height depends on admixtures. Measurements at tungsten electrodes doped with ThO2, La2O3 and Ce2O3 within the model lamp show that evaporated emitter material is redeposited by an emitter ion current onto the electrode surface. It reduces the work function of tungsten cathodes above the evaporation temperature of the emitter material, too; and also of cold anodes, indicating a field reversal in front of them. The formation of an emitter spot at low cathode temperature and high emitter material density
机译:相对于基材原子的单层原子,形成偶极层,降低其功函数。通过蒸汽沉积或通过脱落通过脱落来通过气相沉积或通过将发射器材料沉积到电弧电极上来产生这种层。在具有透明YAG陶瓷燃烧器的金属卤化物灯中调查这种脱位发射器效果,以及模型灯。在YAG灯内,电弧在用金属碘化物接种的高压Hg蒸气中的杆状钨电极之间使用开关DC电流运行。在模型灯内,DC电弧在杆状钨电极 - 一个掺杂在大气压AR之间。电极温度由1λ-高温测定确定,与电极热平衡的模拟结合。通过发射和吸收光谱法测定发射体材料的等离子体温度,原子和离子密度。通过CEI3,CSI,DYI3,TMI3和LAI3在阴极半周期内,在阴极半周期内显示电极温度的降低和电极前面的增强的金属离子密度,以及相位反转后的相反行为的阶段分辨的测量。 。随着运行频率的增加,阴极的状态重叠到阳极相位 - 除了CS之外,吸附能量低。通常,通过使用发射极材料播种灯来减小相平均电极尖端温度;它的高度取决于混合物。在模型灯内掺杂有THO2,LA2O3和CE2O3的钨电极的测量表明,蒸发的发射器材料被发射极离子电流重新沉积到电极表面上。它也减少了钨阴极的功函数,其蒸发材料的蒸发温度也是如此;还有冷阳极,表明它们面前的野外逆转。在低阴极温度和高发射极材料密度下形成发射极点

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