TIG脉冲电弧二维温度分布动态变化的测量

H. Sawato, S. Tashiro, K. Nakata, Manabu Tanaka, E. Yamamoto, K. Yamazaki, Keiichi Suzuki
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引用次数: 10

摘要

TIG脉冲电弧焊适用于背焊、薄板焊接等,其热源特性可由电流波形控制。热传导和电弧产生的电子凝结主要影响基体金属的热流密度。这两个因素在很大程度上取决于电弧中的温度分布和电流路径。为了明确TIG脉冲电弧的热源特性,作为研究的第一步,利用高速摄像机采用Fowler-Milne法测量了TIG脉冲电弧二维温度分布的动态变化。结果发现,电弧柱呈径向膨胀,峰值电流为200A时最高电弧温度为20000 k。另一方面,在基极电流为50A时,电弧柱宽度减小,特别是在电弧下游区域,电弧最高温度降至17500 k。
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Measurement of dynamical variation in two-dimensional temperature distribution of TIG pulsed-arcs
TIG pulsed-arc welding is suitable for back-bead welding, thin plate welding and so on, because the heat source properties can be controlled by current waveform. The heat flux onto the base metal is affected mainly by thermal conduction and electron condensation from the arc. Both factors strongly depend on the temperature distribution and current path in the arc. In order to clarify the heat source properties of TIG pulsed-arc, dynamic variation in two-dimensional temperature distribution of TIG pulsed-arc was measured through Fowler-Milne method with a high speed video camera as a first step of the study. As a result, it was found that the arc column was expanded in radial direction and the maximum arc temperature was 20,000K during the peak current of 200A. On the other hand, the width of the arc column decreased especially in the downstream region of the arc and the maximum arc temperature fell to 17,500K during the base current of 50A.
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