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Microwave power spectral density and its effects on exciting electrodeless high intensity discharge lamps

机译:微波功率谱密度及其对激发无电极高强度放电灯的影响

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Summary form only given. The effects of a microwave source generating a spectrally dense power spectrum on the operation of an electrodeless high intensity discharge lamp were measured. Spectrally pure (monotone) sources operating within ISM bands at 915 MHz and 2.45 GHz produce stable capacitively coupled discharges useful for producing flicker-free light for numerous applications. The internal plasma temperature distribution and lamp geometry define acoustic resonance modes within the lamp which can be excited with power sidebands. The principal resonant frequencies lie in the range of 15 to 500 kHz. The resonances appear broadened owing to imperfections in the geometry of the vitreous silica tubes used to contain the discharges and sometimes shift due to condensate movement. Consequently, modulation of the carrier can produce sidebands which couple effectively to some if not all resonances. Deleterious spectral components may arise from instabilities in magnetron tubes, pulsed mode operation of magnetron tubes or improperly filtered DC supply voltages in both tube and solid-state generators. The effect of the sidebands is to perturb the discharge and cause deflection of the thermal arc from its steady state position. If the sidebands are sufficiently dense and contain sufficient power a multitude of modes are excited simultaneously causing disruption of the convective flow within the tube leading to plasma instabilities and extinguishing of the discharge. Lower order modes of acoustic resonance have been observed to perturb the discharge with as little as 0.2% of the total applied power contained within the sidebands.
机译:仅提供摘要表格。测量了产生光谱密集功率谱的微波源对无电极高强度放电灯工作的影响。在915 MHz和2.45 GHz的ISM频段内操作的光谱纯(单调)源产生稳定的电容耦合放电,可用于产生适用于多种应用的无闪烁光。内部等离子体温度分布和灯的几何形状定义了灯内的声共振模式,这些声共振模式可以用功率边带激发。主谐振频率在15到500 kHz的范围内。由于用于容纳放电的石英玻璃管的几何形状的不完善,共振似乎变宽了,有时由于凝结水的移动而发生位移。因此,载波的调制可以产生边带,该边带有效地耦合到一些甚至不是全部的谐振。有害的频谱分量可能是由磁控管的不稳定性,磁控管的脉冲模式操作或管型和固态发生器中的直流电源电压滤波不当引起的。边带的作用是扰动放电并引起热电弧从其稳态位置偏斜。如果边带足够密集并且包含足够的功率,则同时激发多种模式,从而导致管内对流流动中断,从而导致等离子体不稳定并消除放电。已经观察到较低阶的声共振模式以仅占边带内总施加功率的0.2%干扰放电。

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