The method of three-dimensional mathematical modelling by means of CFD prog
ram FLUENT was used to find the influence of means of intensification upon
technological characteristics of grass melting furnaces. Two physical means
, i.e. a mechanical barrier and melting tank insulation (or heat losses thr
ough walls and bottom) were selected to intensify a melting process. Techno
logical characteristics were defined by the magnitude and shape of temperat
ure and velocity fields and by the volume of glass melt with the temperatur
e lower than the temperature liquidus. The results of mathematical modeling
have shown the considerable influence of the pull of the furnace, of the m
agnitude of thermal losses through the walls and the bottom and of the heig
ht of a mechanical barrier. The temperature of glass melt flowing into the
throat is increased by a height of a barrier and decreased by heat losses.
The temperature 1200 degrees C which corresponds with glass melt viscosity
h = 10(3) dPa was considered to be the lowest limit of the temperature of g
lass melt coming to a throat. Variants with this temperature lower then 120
0 degrees C have not satisfied this evaluating criterion. The velocity of t
he glass melt flowing into the throat is increased by the pull of the furna
ce (18 t day(-1) corresponds with 9.38 X 10(-4) m s(-1); 50 t day(-1) corre
sponds with 2.62 x 10(-3) m s(-1) and by the heat losses. The heat losses a
lso influence the volume of "dead areas" (the higher the heat losses the la
rger the "dead areas"). Only the variants with a = 1 W m(-2) K-1 and two va
riants with a = 3 Wm(-2) K-1 have satisfied the criterion of zero "dead are
as ". The height of a barrier influences the shape of velocity pra;ii[es, i
.e. the presence of the backward current. If this height h = 0. 75 m, the r
eturn current cannot be observed On the other hand the mechanical barrier w
ith the smallest height h = 0.375 m actually did not influence the current
in a melting tank. All the above mentioned evaluating criteria have been sa
tisfied by only 17 variants from the whole number of 92 investigated ones.
The investigated glass melting furnace should be operated with very low coe
fficient of heat transfer at walls and bottom. The pull of the furnace can
be kept at 40 t day(-1). The height of a mechanical barrier should range be
tween 0.5 m and 0. 625 m from the furnace bottom. Significant influence of
distance bent een a mechanical barrier and a charge wall has not been prove
d so the barrier can be situated across the melting tank with the proximity
4. 75 - 5.5 m to the frontal charge wall.