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Influence of primary cooling conditions and austenite conditioning on the hot ductility of the simulated continuous cast peritectic steels

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posted on 2020-09-18, 13:51 authored by Kedibone Lekganyane
<b>Stage 1</b>:The first approach to the project was to generate the coarse and abnormal prior austenite grain size to approximate the industrial <u>as-cast microstructure</u>. Please refer to the thermal path followed to generate the as-cast microstructure in <b>Figure</b> <b>3:4</b> in <b>chapter 3 </b>(dissertation). The method used to reveal the prior austenite grain boundaries was explained in details in <b>chapter 3</b> of the dissertation <b>section 3.3.1.1.</b><div><b><br></b></div><div><b>Stage 2: </b>In this stage, the conditions (i.e. heating rate, austenite conditionings and the soaking times) that were used to generate the as-cast microstructure were then reserved for further procedures. </div><div><br></div><div>The austenite to ferrite start temperatures during primary cooling stage were established. In this case, the specimens were cooled at the rate of 10 °C/s from the austenite conditionings. This cooling rate was associated with the harsh cooling rate experienced by the strand beneath the mould (in the primary cooling stage). Please refer to <b>Figure 4:3</b> in <b>chapter 4 </b>(dissertation). </div><div><br></div><div><b>Stage 3: </b>It was reported that during the rapid primary cooling, the surface of the strand corner drops to a minimum temperature, T<sub>min</sub> followed by the surface reheating to the T<sub>max</sub> as the surface position studied moves away from the mould. The secondary cooling cycle from the T<sub>max</sub> to the unbending was slow due to the strand's interior and the cooling intensity being lower here than in the water cooled mould region. The T<sub>min</sub> values were generated from the non-equilibrium and equilibrium austenite to ferrite start transformation temperatures. </div><div><br></div><div>The first set of T<sub>min</sub> values were generated at 10 °C below the Ae<sub>3</sub> temperatures (<b>Figure 4:5</b>) whilst the second set of T<sub>min</sub> values was generated at 70 °C above the Ar<sub>3P</sub> temperatures (<b>Figure 4:7</b>). </div><div><br></div><div><b>Stage 4: </b>In order to evaluate the influence of the magnitude of the rebound step on the hot ductility, two values of ∆T<sub>r</sub>, were selected for each of the two T<sub>min</sub>-values employed, ∆T<sub>r</sub> values of 200 °C and 300 °C respectively, resulting in the four T<sub>max</sub> -values.</div><div><br></div><div>It was decided that the secondary cooling rate from the T<sub>max</sub> values be kept constant at the rate of 0.1 °C/s and the simulated unbending temperatures were chosen to range from a temperature being 72 °C below the T<sub>max</sub> -value to a temperature 272 °C below the T<sub>max</sub> value. This was done in order to investigate the influence of the magnitude of the undercooling below the T<sub>max</sub> -value on the hot ductility. </div><div><br></div><div>Please refer to <b>Figures 3:9-3:12 </b>in <b>chapter 3 </b>of the dissertation. All the conditions used to generate the thermal paths are tabulated in <b>Table 3:2.</b></div>

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ArcelorMittal SA

University of Pretoria

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Mineral Science and Metallurgical Engineering

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