Activation energy of phase transformations at high-temperature synthesis of tungsten carbide by electrothermal explosion under pressure

V. T. Telepa, M. Alymov, А. Shcherbakov
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Abstract

The effect of activation energy on phase transformations (transitions) in the W–C system during the synthesis induced by an external heat source was investigated by electrothermal explosion (ETE) under pressure. The ETE technology combines self-propagating high-temperature synthesis (SHS) with additional sample heating by Joule heat – electric current passing through the synthesized mixture, and it makes it possible to determine the chemical reaction rate that is highly susceptible to external impacts such as pressure, concentration, sample shape, any film present on combustion products, etc. The chemical reaction rate, i.e. external source current, may be controlled by changing the activation energy. The study was conducted in the following conditions: temperature Т = 293÷3700 K; carbon concentration of 49.8–50.2 at.%; quasi-static compression at P = 96 MPa; external source voltage and current density V = 10 V, I = 20 МА/m2, respectively; samples 8 mm in diameter weighing 6 g. The Т–τ thermogram of the W–C system was used to determine the following parameters: four stages of the synthesis process, temperatures of special points of phase transformations, temperature boundaries of phases and process activation energy. Thermograms of intermediate states are presented as isothermal plateaus of phase transformations. The analysis of experimental results and the physical representation of the process make it possible to assert that temperature plateau parameters are the effective value of activation energy for synthesis mode maintenance. Each of the 4 W–C mixture synthesis stages is described. Pre-explosion stage I – sample heating in the temperature range of Т = 293÷563К, endothermic reaction, effective activation energy for synthesis mode maintenance Q = 2.96 kJ, and taking into account 1-mole mass Еа = 111.6 kJ/mol. Low-temperature (563–1190 К) stage II – ignition, Q = 5.46 kJ, Еа = 109.2 kJ/mol. High-temperature stage (III) in the range of Т = 1190÷2695К, order–disorder transformation, Q = 14.25 kJ, Еа = 424 kJ/mol. Finally, Stage IV occurs in the range of Т = 2695÷3695К, Q = 14.31 kJ, Еа = 143.2 kJ/mol. It was shown that the limiting stage with the highest activation energy is the melting process.
高压下电热爆炸高温合成碳化钨相变活化能的研究
采用压力下电热爆炸(ETE)方法研究了外部热源诱导W-C体系合成过程中活化能对相变的影响。ETE技术将自传播高温合成(SHS)与通过焦耳热电流过合成混合物的额外样品加热相结合,从而可以确定化学反应速率,该速率极易受到外部影响,如压力、浓度、样品形状、燃烧产物上存在的任何膜等。化学反应速率,即外源电流,可以通过改变活化能来控制。本研究在以下条件下进行:温度Т = 293÷3700 K;碳浓度49.8-50.2 at.%;P = 96 MPa时准静态压缩;外源电压和电流密度V = 10 V, I = 20 МА/m2;样品直径8毫米,重6克。利用W-C体系的Т -τ热图确定了合成过程的四个阶段、特殊相变点温度、相温度边界和工艺活化能等参数。中间态的热图表现为相变的等温高原。通过对实验结果的分析和过程的物理表征,可以断言温度平台参数是维持合成模式的活化能有效值。描述了4个钨碳混合物合成阶段中的每一个阶段。爆炸前阶段-试样在Т = 293÷563К的温度范围内加热,进行吸热反应,维持合成模式的有效活化能Q = 2.96 kJ,考虑1摩尔质量Еа = 111.6 kJ/mol。低温(563-1190 К) II级点火,Q = 5.46 kJ, Еа = 109.2 kJ/mol。高温阶段(III)在Т = 1190÷2695К范围内,有序-无序转变,Q = 14.25 kJ, Еа = 424 kJ/mol。最后,第四阶段发生在Т = 2695÷3695К, Q = 14.31 kJ, Еа = 143.2 kJ/mol范围内。结果表明,熔炼过程是活化能最高的极限阶段。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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