ꢆ
Digital electronic weight balance (EG-2000, A & D Inc.,
Tokyo, Japan) was used to monitor the sample weight as a
function of drying time. The time-weight data was obtained
by the recorder (AD-8121, A & D Inc., Tokyo, Japan) through
an RS-232 interface.
fusion coefficient (D ) was calculated as follows:
r
ꢆ
M
D ꢄ 1/(M ꢂ M) ͐ D dM
(4)
r
i
M
r
i
where Mi is moisture content in equilibrium with the sur-
rounding gas phase (g-water/g-solid), Dr is the reduced diffu-
sivity (dimensionless). The average Sherwood number (Shd)
was calculated as follows:
Airflow was controlled by a damper, and the air was
flowed down in the same manner as that of the convention-
al factory. The airflow was held near constant at 1.7 to 1.8 m
sꢂ1 in the present study using an anemometer (CW-30,
CUSTOM Inc., Tokyo, Japan).
ꢆ
Shd ꢄ 2F/(M ꢂM )D
i
(5)
r
The portable fume (Iuchi Inc., Osaka, Japan) and the fan
(
Iuchi Inc., Osaka, Japan) installed in the desiccator were
The driving force for the drying process in the present
study with a constant surface concentration of fresh Udon was
expressed as the average moisture content of the sample mi-
nus the interfacial moisture content at any time. Drying curves
for samples were constructed by expressing the logarithm of
the flux parameter as a function of driving force.
used to generate the airflow.
The connected hose between the desiccator and the in-
cubator (diameter 50 mm) was heated at a constant temper-
ature by the heating tape.
The relative humidity was measured at the upper posi-
tion of the sample by thermo recorder (TR-72, T and A Inc.,
Nagano, Japan). Thermister SK-67sensor connected to the
recorder (R316, TECHNOL SEVEN Inc., Kanagawa, Japan)
was used to monitor the temperature.
The regular regime curve was differentiated to give dln(F)/
dln(M ꢂ M ) as a function of moisture content. The averaged
i
Sherwood number (Sh ) as a function of dln(F)/dln(M ꢂ M )
d
i
was presented by Schoeber and Thijssen (1977) in graphic
forms for infinite slabs, non-shrinkage infinite cylinders, and
non-shrinkage spheres. An empirical equation to relate the av-
erage Sherwood number and dln(F)/dln(MꢂMi) was devel-
oped by Tong and Lund (1990) as follows:
Drying method
The drying experiment was carried out at 3 tempera-
tures, 20, 30, and 40 ꢀC, according to the conventional pre-
and main-drying conditions. Moisture contents of samples
were determined by the air-oven method, drying at 135 ꢀC
X ꢄ dln(F)/dln(M ꢂMi)
(
AACC, 1995). Drying experiments at 20 and 30ꢀC were done
2
Shd = exp[1.74 ꢇ 0.43(lnX) ꢂ 0.076(lnX) ꢂ 0.0034(lnX) ]
3
in a refrigerator room (about 6 ꢀC), while that at 40 ꢀC, the
experiments were run at room temperature at 25 ꢀC. Time-
weight data were collected in triplicate for each tempera-
ture.
(6)
The Dr was calculated by combining Eq. 4 and Eq. 5 as fol-
lows:
Measurement of shrinkage
D ꢄ (d/dM)(2F/Sh )
r
(7)
d
The time changes of width, thickness, and length of the
fresh Udon were measured by a vernier caliper as a function
of sample weight. At the same time specific gravities of sam-
ples were measured by an electronic pycnometer (EW-
and the effective moisture diffusivity (Deff) (cm2 s-1) was then
obtained by
Deff ꢄ Dr/ꢃ2s
(8)
2
00SG, MIRARGE TRADING Inc., Osaka, Japan). The densi-
ties of samples were obtained from the values of specific
gravities by multiplying 0.999973.
3
where ꢃs is the density of sample (g-solid/cm -sample).
Tong and Lund (1990) presented that the relationship be-
tween the effective moisture content and temperature was de-
scribed by Arrhenius equation (Atkins 1992):
Data analysis
2
Water flux (j , g-water / cm ) relative to the moving inter-
w
face was calculated as follows (Luyben and others 1980):
D ꢄ Bexp(ꢂ E/RT)
eff
(9)
j ꢄ ꢂ(W /A(M))(dM/dt)
w
(2)
ds
where B is the frequency constant (cm sꢂ1), E is the activation
energy (J molꢂ1), R is the gas constant (8.314 J molꢂ1 Kꢂ1), and
T is the absolute temperature (K).
2
where Wds is the weight of dry sample (g), A is the area (cm2),
M is the average moisture content (g-water/g-solid), A(M) is
2
the area as a function of moisture content (cm ), t is the time
Statistical analysis
(
s). When jw was known, flux parameter (F, dimensionless)
was calculated from the following equation:
The relationship between the moisture content and nor-
malized area of the fresh Udon at 3 temperatures were ana-
lyzed by the least-squares method, using a microcomputer
with Delta graph® Pro 3 (Nippon Polaroid Inc., Tokyo, Japan).
2
F ꢄj ꢃ R /D ꢃ
w ds ds 0 s0
(3)
where ꢃds is the density of dry sample (g-solid/
3
cm ꢂsample), R is half the thickness of dry sample (cm),
Statistical analysis was conducted by Fisher’s z-transformation
method using Stat View® 4.02 (Abacus concepts Inc., Berkeley,
ds
and D0ꢃs02 is a dimensional constant with numerical value 1,
introduced for similarity reasons. The average reduced dif-
Calif., U.S.A). The relationship between the moisture content
and density data were analyzed in the same way.
Vol. 65, No. 3, 2000—JOURNAL OF FOOD SCIENCE 443