
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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