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Estimation of Interfacial Heat Transfer Coefficient in Indirect Squeeze Casting

机译:间接挤压铸造界面传热系数的估计

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In this work, indirect squeeze casting experiments were conducted using a 350-t Ube vertical squeeze caster to cast a hockey puck-like shaped casting of aluminum alloy A356. Experiments were conducted at two melt temperatures and at two pressure levels, while the die temperature was maintained close to 400 deg F. Pressure inside the die cavity was continuously monitored using a Kistler pressure probe and recorded using an associated data acquisition system. A CAD model of the hockey puck-like casting was imported to a commercial software package and solidification was simulated. Temperatures close to two mm from the casting-mold interface were measured using thermocouples mounted in the moving die half. While inputting heat transfer boundary conditions, it is assumed that there is no gap formation in squeeze casting and that the IHTC remains more or less constant during solidification in contract to gravity die casting where there is a marked decrease in the HTC value upon formation of an air gap between the casting and the mold during solidification. The IHTC was estimated by closely matching simulated and experimental cooling curves and was found to be close to 4500 W/m~2 K. Using this coefficient, the temperature distribution inside the casting was predicted. The modeling was validated by comparing predicted temperatures with measured temperatures in the mold. No significant enhancement in heat transfer at the metal-mold interface was observed for the high-pressure case when compared to the low-pressure case. This is due to the fact that metal pressures at the interface had already reached the threshold level beyond which no improvement in heat transfer occurs. Secondary Dendrite Arm Spacings (SDAS) were measured at various locations in the casting and compared with calculated cooling rates through the solidification range. The correlation of SDAS with cooling rate indicates a finer structure for a given cooling rate than previously reported in the literature, a result attributed to compositional modification of the alloy.
机译:在这项工作中,使用350-T UBE垂直挤压脚轮进行间接挤压铸造实验,以铸造铝合金A356的曲棍球冰球状铸造。实验在两个熔体温度和两个压力水平下进行,同时将模芯温度保持接近400°F。使用奇克勒压力探针连续监测模腔内的压力并使用相关的数据采集系统进行记录。将曲棍球冰球状铸造的CAD模型进口到商业软件包,并模拟凝固。使用安装在移动模头的热电偶测量距离铸模界面接近两个毫米的温度。在输入传热边界条件的同时,假设在挤压铸造中没有间隙形成,并且在合同的凝固过程中,IHTC在重力压铸时仍然持续,其中HTC值在形成时显着降低铸造期间铸件与模具之间的气隙。通过密切匹配模拟和实验冷却曲线估计IHTC,发现使用该系数接近4500W / m〜2 K.预测铸件内的温度分布。通过将预测的温度与模具中的测量温度进行比较来验证建模。与低压壳相比,对于高压壳体,观察到金属模界界面处的传热的显着增强。这是由于界面处的金属压力已经达到了超过其发生热传递的改善的阈值水平。在铸件中的各个位置测量次级树枝状臂间距(SDA),并通过凝固范围与计算的冷却速率进行比较。 SDA与冷却速率的相关性表示给定冷却速率的细粒结构比在文献中先前报告的给定冷却速率,其归因于合金的组成改性。

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