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Activity of lead in copper matte at very low lead concentration

机译:铅浓度很低时,铜雾中铅的活性

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The thermodynamic behavior of lead in Cu-Fe matte was investigated using a transportation technique where argon gas was bubbled into a bath of copper matte containing approximately 100 ppm lead at temperatures between 1300 and 1400°C. The effect of flow rate, temperature and matte grade were investigated on the lead transport from a bath containing 100 grams of synthetic copper matte to the gas phase. The concentration of lead in the bath was followed with time. At argon flow rates between 3 l h-1 and 18 l h-1, it was observed that the concentration change of lead in the matte was found to follow a first order relationship where the calculated concentration at time t ,is of the form: [ Pb ]= a.e-b.t where a is equal to the initial lead content in ppm, [ Pb ]i, and b is an exponential term and t is time in minutes. The partial pressure of lead species in the gas phase was calculated from the concentration changes in the matte and from the bubbling gas rate. At gas flow rates between 3 and 9 l h-1, the lead removal appeared to be under equilibrium conditions. At higher gas flow rates, the apparent rate decreased, mainly due to splashing of matte into the cold zone of the furnace. In these experiments with Ar as the carrier gas, the sulphur and oxygen partial pressures of the melt were not controlled. Chemical analysis of the major components in the matte showed only random variation with bubbling time, and so a thermodynamic solution model for copper matte was used to calculate the equilibrium sulphur pressure expected. From this approach the proportion of Pb, PbS and Pb2 species in the gas could be calculated knowing the relevant reaction constants, e.g.: PbS(g) = Pb(g) + 1/2S2(g) From the proportions of the lead species in the gas, the value of the lead activity coefficient with respect to the gas state could be determined. For a 50% copper matte, it was found that the activity coefficient increased with temperature, from a value of 0.8 at 1300°C to 1.4 at 1400°C. At the white metal composition, this value was 0.28 at 1300°C. These results are compared with other relevant studies in the literature.
机译:使用运输技术研究了铅在Cu-Fe雾中的热力学行为,其中在1300至1400°C的温度下,将氩气鼓泡到包含约100 ppm铅的雾铜熔池中。研究了流速,温度和雾面等级对铅从含100克合成铜雾面的浴到气相的铅迁移的影响。随时间跟踪浴中铅的浓度。观察到在3 l h-1至18 l h-1的氩气流量下,发现冰霜中铅的浓度变化遵循一阶关系,其中在时间t的计算浓度为以下形式: [Pb] = ae-bt,其中a等于以ppm计的初始铅含量,[Pb] i,b为指数项,t为以分钟为单位的时间。气相中铅物质的分压是根据消光剂的浓度变化和鼓泡气体速率计算得出的。在3至9 l h-1的气体流量下,除铅似乎是在平衡条件下进行的。在较高的气体流速下,表观速率降低,这主要是由于将无光泽溅入炉子的冷区。在这些以Ar作为载气的实验中,不控制熔体的硫和氧分压。对冰沙中主要成分的化学分析显示,其起泡时间只是随机变化,因此使用了铜冰沙的热力学解决方案模型来计算预期的平衡硫压。通过这种方法,可以在知道相关反应常数的情况下计算气体中Pb,PbS和Pb2的比例,例如:PbS(g)= Pb(g)+ 1 / 2S2(g)对于气体,可以确定相对于气体状态的铅活度系数值。对于50%的铜雾,发现活度系数随温度的升高而增加,从1300°C时的0.8升高到1400°C时的1.4。在白色金属组成下,该值在1300℃下为0.28。将这些结果与文献中的其他相关研究进行比较。

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