under these conditions. Moreover, this can only be
done at the outlet of the oven considering the radiant
flux of energy inside the oven. A way of dealing
with this problem is to relate ultimately the humidity
and temperature at the web surface to the internal
humidity and temperature of the web using a model.
A phenomenological model for the radiant drying of
thick sheet of porous material derived by Kuang et
al. (1994) considering the many transport
phenomena involved during drying offered the
potential of doing that. Unfortunately, the
mathematical solution of this partial differential
model is too time intensive and the formulation does
not lead itself easily to implementation for real time
control. This is especially true when operating the
oven at higher electrical power levels for which
much shorter drying time responses would be
observed. However, further analysis of the results
obtained during the set of experiments done here has
indicated drying characteristics that can be used to
profit in a control algorithm.
First, as illustrated in Figure 4, results have
indicated that the time interval required such that the
core temperature at the mid-depth of the web
achieves 100 ºC (a completely dry condition) is a
linear function of the electrical power used in the
oven. Also, as indicated in Figure 5, results have
shown that the temperature at the external surface of
the web, corresponding to a internal temperature
reaching 100 ºC at mid-depth of the web, is also a
linear function of the electrical power used in the
oven. These characteristics have been shown to hold
with webs of different densities and thicknesses in
the range of the electrical power indicated.
4 MODEL BASED CONTROL
The experimental results have shown that the surface
temperature of the web T
SS
at the outlet of the oven
is linearly related to the electrical power used:
T
SS
= A
S
. P + B
S
. θ (1)
Also, the residency time required to achieve a given
temperature T
CC
at mid-depth across the thickness of
the web at the outlet of the oven was shown to be
linearly related to the electrical power used. In a
more general fashion :
T
CC
= A
C
. P + B
C
. θ (2)
In both cases, A
S
, A
C
, B
S
and B
C
are scalars whose
values depend generally on the humidity of the web
H
inlet
at the inlet of the oven and must be determined
through experimentation (Slitine et al., 2001).
Generally, this would need to be done for a range of
humidity (water content of the web) typical of the
ones existing at the point of entry to the oven.
Fortunately, the humidity of the web entering the
oven is often limited to a small range of values. In
effect, excess water has normally been removed
since the material entering the oven is generally
passed through a free water removing device rollers
or vacuum slot (see Figure 1). Nevertheless, the
scalars A
S
, A
C
, B
S
and B
C
need be determined
specifically for each type of material (density and
thickness) considered for drying. For a given
residency time in the oven, Equation (2) may be
used to compute the a priori electrical power
required to achieve a desired core temperature T
CC
at
mid-depth across the thickness of the web :
P = (T
CC
/ A
C
) - (B
C
/ A
C
) . θ (3)
Also, through equations (1) and (2) T
SS
is related to
T
CC
and P in the following manner:
T
SS
= (B
S
/B
C
). T
CC
+ B
D
. P (4)
275
300
325
350
375
1000 1500 2000 2500
ELECTRICAL POWER (WATTS)
Figure 4: Time required achieving 100 ºC at mid-
depth of a 15,6 mm thick 2000g/m
2
polyester sheet as
a function of power input
150
175
200
225
250
1000 1500 2000 2500
ELECTRICAL POWER (WATTS)
Figure 5: Surface temperature of a 15,6 mm thick
2000g/m
2
polyester sheet when reaching 100 ºC at
mid-depth as a function of power input
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