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Erschienen in: Metallurgical and Materials Transactions B 3/2009

01.06.2009

Liquid Metal Pool Behavior during the Vacuum Arc Remelting of INCONEL 718

verfasst von: D.M. Shevchenko, R.M. Ward

Erschienen in: Metallurgical and Materials Transactions B | Ausgabe 3/2009

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Abstract

Non-steady-state ensemble arc behavior has been observed during the Vacuum Arc Remelting (VAR) of 508-mm-diameter ingots of INCONEL 718. The liquid metal flow in the melt pool of a 508-mm ingot during VAR has been simulated under two alternative sets of conditions: (1) a steady-state axisymmetrical arc distribution, as has been typically used in modeling work previously; and (b) a transient asymmetrical arc distribution. Due to the computational requirements, neither mass flux nor solidification were modeled; instead, the pool shape was fixed from measurements from a 508-mm-diameter ingot, and a constant pool wall temperature of 1609 K was used. The transient simulation assumed a localized Gaussian arc whose effective center was located at a distance of 0.1 m from the ingot centerline; this simulation rotated clockwise around the centerline with a period of 36 seconds. The steady-state model was simulated with axisymmetrical distributions of current and power input to the pool top surface calculated by time averaging the transient current and power inputs. The standard k-ε solver of ANSYS CFX 5.6 software was used for both simulations. The transient model results suggest that 5 seconds of asymmetrical arc behavior is enough to change the pool from steady state to transient and that, after 30 seconds, the flow is almost fully developed (at least to the accuracy of the model) and dominated by the Lorentz force. Aspects of the model results agree with key features of the melt pool observed during VAR.

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Fußnoten
1
INCONEL is a trademark of Inco Alloys International, Huntington, WV.
 
2
The total power input during VAR of INCONEL 718 under the conditions presented here is ∼141 kW. Other work by these authors in which the power distribution is studied in more detail10,11 suggests that the power input to the inner crucible wall above the pool surface (due to the side arcing between electrode and inner crucible walls, radiation from the interelectrode gap, and the pool surface) is around 46 kW. So the rest of the total power input, approximately 95 kW, should go ultimately to the pool surface. More than half of this comes via the melting electrode tip as the enthalpy of the droplets and the remainder directly by arc heating/radiation.[10]
 
3
The techniques of measurement and analysis used in Reference 6 were not able to determine the shape of the arc, but only the distribution of the time history of the position of its electrical center. However, knowledge of the electrical center when combined with the electrode diameter does constrain the current distribution.
 
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Metadaten
Titel
Liquid Metal Pool Behavior during the Vacuum Arc Remelting of INCONEL 718
verfasst von
D.M. Shevchenko
R.M. Ward
Publikationsdatum
01.06.2009
Verlag
Springer US
Erschienen in
Metallurgical and Materials Transactions B / Ausgabe 3/2009
Print ISSN: 1073-5615
Elektronische ISSN: 1543-1916
DOI
https://doi.org/10.1007/s11663-008-9206-y

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