UNSTEADY NUMERICAL-SIMULATION OF CIRCULATION AND HEAT-TRANSFER IN A GLASS MELTING TANK

Citation
N. Vanandruel et M. Deville, UNSTEADY NUMERICAL-SIMULATION OF CIRCULATION AND HEAT-TRANSFER IN A GLASS MELTING TANK, Ceramics-Silikaty, 39(4), 1995, pp. 130-134
Citations number
7
Categorie Soggetti
Material Science, Ceramics
Journal title
ISSN journal
08625468
Volume
39
Issue
4
Year of publication
1995
Pages
130 - 134
Database
ISI
SICI code
0862-5468(1995)39:4<130:UNOCAH>2.0.ZU;2-D
Abstract
Various numerical simulations are currently available for the represen tation of flow and heat transfer in glass melts. Increasing computer p erformance allows 3D complex simulation coupled with electrical boosti ng, flame radiation heat transfer, chemical reaction, bubbling, etc. W e present the numerical results of unsteady modeling of glass flow and heat transfer in the glass melting tank. The use of finite-element sp atial discretization decreases the total number of degrees of freedom required to achieve acceptable accuracy, while efficient integration s chemes (implicit predictor-corrector) lead to time step sizes which re duce the number of solutions even for studies of long term duration. F irst, different variations on the TC21 test-case (modification of the pull rate, thermal boundary profiles) are performed. This reference si tuation was selected by the 21st Technical Committee of the Internatio nal Commission on Glass. Following this, a reduced-scale mixed electri cal-fuel furnace is studied, allowing the modeling of unsteady boostin g heat transfer. Finally an unsteady advection-diffusion problem is so lved to represent the mixing of two different types of glasses. The in terest in unsteady modeling is two-fold: (1) the accurate time evoluti on of flow and temperature sheds light on the structure and stability of the flow related to a given set of physical properties and boundary conditions; and (2) the transient solution gives reproducible and ine xpensive information for the definition of a control process. The main result of this study is the clear distinction between kinematic and t hermal time constants and the feasibility of direct exchanges between unsteady simulation and control models.