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> Glass Manufacturing

Glass Manufacturing

Brittle fracture

A current hot topic is the study of the rapid propagation and bifurcation of cracks through a piece of glass when it is struck by a hard object.

Melting sand to make glass

All glass originates from sand which is heated upto 1500 degrees in a furnace before it flows out to make into windows, TV screens, optical fibres, etc. The mechanics and heat flow in the furnace pose mathematical challenges akin to those encountered in, say, magma dynamics within the earth. But in glass manufacture, minute imperfactions are all important and high precision modelling is vital. With concerning vthe melting of the sand and through the hydrodynamics of the molten glass.

Temperature distribution, streamlines and
velocity in a bath filled with molten glass, where the temperature at
the top of the bath is linear in x, and walls and bottem of the bath are 
insulated.

Capillary tube drawing

How do we make square test tubes and capillary tubing? To produce regular capillary tubing requires vthe drawing of molten glass through a `doughnut' shaped die, and drawn off. However, if we begin with a square cross-sectional die, then the effects of surface tension during the tube drawing process will cause the profile to evolve towards a more circular profile. The full question we wish to answer is: given any final tube cross-section, what is the die shape required to produce this?

This work is motivated by our links with Scott Glass in Mainz, Germany.

Window glass cooling

In the final stages of window glass manufacture in a float glass factory (where the liquid glass from the furnace solidifies as it floats on a thin layer of molten tin) the glass needs ot be cooled by about 100 degrees by passing it under a cold water jet. The hydrodynamics of this jet are such that it leads to a completely novel class of boundary layer problems in viscous flow, wherein water in the jet can flow both upstream and downstream at any particular spot on the glass.

Selected references

  1. J. N. Dewynne, J. R. Ockendon & P. Wilmott, 1989 On a mathematical model for fiber tapering, SIAM J. Appl. Math. 49, 983-990.
  2. B. W. van de Fliert, P. D. Howell & J. R. Ockendon, 1995 Pressure-driven flow of a thin viscous sheet, J. Fluid Mech. 292, 359-376.
  3. P. D. Howell, 1996 Models for thin viscous sheets, Euro. Jnl Appl. Maths 7, 321-343.
  4. L. J. Cummings & P. D. Howell, 1999 On the evolution of nonaxisymmetric viscous fibres with surface tension, inertia and gravity, J. Fluid Mech. 389, 361-389.
  5. D. Salazar & R. Westbrook, 2002 Inverse Problems of Mixed Type in Linear Plate Theory, in preparation.

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This page last modified by A. Shabala
Wednesday, 06-Feb-2008 10:08:08 GMT
Email corrections and comments to shabala@maths.ox.ac.uk