1 / 32

Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2. J.R. McDermid, Noranda Inc. - Technology B.M. Maag, Pro-Tec Coating Co. M. Gaug, Maya Heat Transfer Technologies 94th Galvanizer’s Association Meeting Dearborn, MI. Outline. Introduction Numerical Model Details

eljah
Download Presentation

Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2 J.R. McDermid, Noranda Inc. - Technology B.M. Maag, Pro-Tec Coating Co. M. Gaug, Maya Heat Transfer Technologies 94th Galvanizer’s Association Meeting Dearborn, MI

  2. Outline • Introduction • Numerical Model Details • Results and Discussion • General Observations • Detailed Case Results • Conclusions McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  3. Introduction • Numerical and physical modelling has evolved to become a powerful tool for understanding the factors which control and can alter flow in the CGL bath • many papers presented on this subject at the GA, Galvatech and other conferences • Solutions now encompass the coupled thermally driven (buoyancy) flow as well as the strip-driven viscous drag flow • significant effect of ingot melting on the flow field in the charging area McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  4. Introduction - cont’d • Some practical applications of numerical modelling without the thermal solution have been published • snout flow - references 9 and 11 • dross management - reference 12 • Objective of the present work: • Use coupled thermal solution to determine the effect of different charging configurations on the flow field in the Pro-Tec CGL2 bath • Use these results to aid in the selection/specification of a new ingot charger by Pro-Tec McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  5. Numerical Modelling Procedure • Model consisted of a half-bath with a symmetry plane along the long axis of the CGL bath • Model meshing and calculation were performed at Maya Heat Transfer Technologies under the supervision of M. Gaug • further details on the methodology and calculation boundary conditions can be found in the paper McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  6. snout symmetry plane ingots steel sheet pot rolls baffle inductor sink roll inductor Numerical Model Geometry McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  7. Numerical Modelling Cases McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  8. Results - General Observations • Changing the strip width/speed • minor effect on the magnitude of the flow velocities, but not the overall fluid flow pattern • some effect on the temperature field due to varying heat input rates, but temperature was controlled to 460ºC and overall effect was minor • Overall circulation pattern consistent with that observed by previous authors • Presence or absence of the baffle determines the shape of the overall flow within the CGL McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  9. General Flow Pattern in CGL Bath McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  10. General Observations - cont’d • There were significant differences in the flow patterns between the centreline and offset ingot charging configurations • overall flow pattern a strong function of the baffle’s presence • For simplicity, all results presented further are for the 1.65 m (65 in.) strip at 99.1 m/min. (325 fpm) case • all velocity plots range of 0 - 0.150 m/s • all temperature plots range of 458 - 463ºC McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  11. Results - Detailed Observations • The model visualisations were performed via 2D cutting planes at various distances from reference planes • X-Y plane parallel to symmetry plane (reference plane) • X-Z plane parallel to top surface plane of the CGL bath (reference plane) McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  12. VC Ingot - X-Y (0.127m) w/o baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  13. VC Ingot - X-Y (0.127m) w/ baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  14. VC Ingot - X-Y (0.127m) w/o baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  15. VC Ingot - X-Y (0.127m) w/ baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  16. VC Ingot - X-Z (1.270m) w/o baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  17. VC Ingot - X-Z (1.270m) w/ baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  18. VC Ingot - X-Z (1.270m) w/o baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  19. VC Ingot - X-Z (1.270m) w/ baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  20. HC Ingot - X-Y (0.050m) w/o baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  21. HC Ingot - X-Y (0.050m) w/ baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  22. OV Ingot - X-Y (1.219m) w/o baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  23. OV Ingot - X-Y (1.219m) w/ baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  24. OV Ingot - X-Y (1.219m) w/o baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  25. OV Ingot - X-Y (1.219m) w/ baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  26. OV Ingot - X-Z (1.270m) w/o baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  27. OV Ingot - X-Z (1.270m) w/ baffle velocity McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  28. OV Ingot - X-Z (1.270m) w/o baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  29. OV Ingot - X-Z (1.270m) w/ baffle temp. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  30. Conclusions • The macroscopic/melting ingot flow calculated for the Pro-Tec CGL2 bath is in general agreement with those of previous authors. • The presence or absence of the deep baffle behind the snout has the largest effect on the bath flow - when present, it effectively isolates the charging area from the remainder of the bath with communication via flow under and around the edges of the baffle. • There are only slight difference between the VC and HC charging cases - orientation factors. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  31. Conclusions - cont’d • The OV charging case is significantly different from the VC and HC cases • interaction of the descending ingot flow with the return flow along the side walls and the rising inductor flow. • ingot material swept along the back wall of the pot before being drawn to the snout by the drag flow from the sheet. • overall pattern continues to be dominated by the baffle. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

  32. Acknowledgements The authors would like to thank Noranda Inc. and Pro-Tec Coating Co. for their permission to publish this paper. McDermid, Maag and Gaug: Numerical Modelling of Ingot Charging Configurations at Pro-Tec CGL2

More Related