Authors: Tareq Eddir (Fluxtrol Inc.), Robert C. Goldstein (Fluxtrol Inc.), Robert Haun (Anspanner LLC)
Location/Venue: IMAT 2021 St. Louis, Missouri

Typical titanium aluminide power. It is typical for some of the particles to be broken.

Powder Titanium is deposited from the top onto a billet being slowly pulled. The molten top of the billet (dashed circle) is heated through an induction heating coil. The black arrows indicate current direction in the coil, caster fingers, and load. The fingers are individually water-cooled to extract heat from the Joule losses and heat from transferred from the load.

The pictures show the geometry of the mold, load, and coil. The mold used for this project's simulation has the following characteristic:
Flux 3D FEM software was used for the simulation

The coil height and was modified to change the length of the melt zone in the load. The bottom insert was moved with the bottom of the coil. A parameter ‘Offset’ was introduced to vary the coil height and bottom insert location.
‘Offset’ is defined by distance between the center of the bottom insert and bottom shunt and the top of the melt OD.
Offset values of 20, 40, 60, 80, 100, 120 mm were used. 120 mm is the original location.
Note: geometry was configured so that below the insert the mold is closed, not slotted.
The coil was changed to a single turn coil for faster solve times.

The highlighted faces had thermal boundary conditions applied as such: radiation heat transfer using emissivity of 0.75, while convection wasn't added due to vacuum conditions. Conduction to the mold was not considered for this project.
Simulation parameters and goals.
Since steady state temperature is the goal of the investigation, the billet was started at a uniform 1600°C and a maximum temperature of 1725°C was targeted. The simulations were run for 3600s.



The two lines shown in the picture (OD and Center) were used to plot the temperature along the length of the billet.
From the withdraw rate of 1kg/min, the size of the billet (34.2 cm3 cross-section), and the axial temperature distribution, the temperature vs time data was calculated as follows:

This calculation converts the temperature profile of a static model to a moving temperature profile to better reflect material movement, as seen in actual systems.

Ref. (4)




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