MATHEMATICAL MODELLING AND OPTIMIZATION OF MELON SLICE DRYING WITH RESPONSE SURFACE METHODOLOGY IN A HEAT PUMP DRYING SYSTEM
C. TUNCKAL†, A. OZKAN-KARABACAK‡, C.E. TAMER‡, P. YOLCI-OMEROGLU‡,§ and Z. GOKSEL*
†Yalova University, Electric and Energy Department, Air Conditioning and Refrigeration Technology Program,
Yalova Community College, 77100, Yalova, Turkey
‡ Bursa Uludag University, Faculty of Agriculture, Department of Food Engineering, 16059, Gorukle, Bursa–Turkey
§ Bursa Uludag University, Science and Technology Application and Research Center, 16059, Gorukle, Bursa–Turkey
* Atatürk Horticultural Research Institute, Food Technology Department, 77100, Yalova, Turkey
Corresponding author e-mail: etamer@uludag.edu.tr
Cite this article as:
Tunckal, C., Ozkan-Karabacak, A., Tamer, C.E., Yolci-Omeroglu, P., Goksel, Z. (2022) “Mathematical modelling and optimization of melon slice drying with response surface methodology in a heat pump drying system”, Latin American Applied Research 52(2), pp 101-110.
Abstract-- (in terms of heat pump drying) An optimum drying temperature of 45 °C, air velocity of 1 m/s and slice thickness of 5.04 mm were recommended with following predicted responses close to experimental values: drying time 216.58 min, total energy consumption 2.94 kWh, coefficient of performance heat pump (COPhp) 3.08, coefficient of performance system (COPws) 2.75, specific moisture extraction rate (SMER) 0.22 kg/kWh, drying rate 2.53, L* value 82.53, a* value -1.83 and b* value 25.82. The most suitable models to represent the drying behavior of optimum melon slices was chosen Wang & Sing. Effective moisture diffusivities (Deff) of the melon slices were ranging from 7.075E-10 - 1.843E-07 m2s-1 and increasing drying air temperature, drying air velocity and slice thickness led to an increment of Deff.
Keywords-- Heat pump drying, Melon, Response surface methodology, Drying characteristics, Mathematical modelling
I. INTRODUCTION
Dried fruits function as the concentrated form of their fresh properties in terms of energy, nutrients, dietary fiber and antioxidants (Bennett et al., 2011). Melon (Cucumis melo L.) is a popular fruit grown in European, Asian and African countries (Dias da Silva et al., 2016). In addition to its rich nutritional composition and bioactive substances, melon has excellent flavour properties (Petkova and Antova, 2015). Since melons are highly perishable and rapidly get decomposed, they can easily deteriorate after harvesting (Welti-Chanes et al., 2002). For this reason, drying is a useful process to extend the shelf life of melons (Azuara et al., 2009; Dias da Silva et al., 2016) and to increase their added value by transforming them in to a healthy snack, especially in over production seasons. On the other hand, drying can cause adverse effects on melon by reducing its quality in terms of colour, texture and bioactive compounds (Dias da Silva et al., 2016). It is very important to select a proper drying method in terms of its technology, energy consumption, and frequency of requirements to maintenance (Kırbaş et al., 2019). Due to the prolonged exposure to high temperature and/or heat and oxygen, traditional drying processes adversely affect typical fresh fruit colour, aroma, and overall flavour (Zanoni et al., 1999Abano et al., 2011 Therefore, there is a need to establish a proper drying method to increase the amount of vitamins and flavour in the final dried product in addition to decreasing the rate of pigment deterioration (and The studies in the literature prevailed that Heat Pump Drying (HPD) system played an important method to retain the colour, vitamins, and other heat sensible components of agricultural products (Prasertsan, 2010; Jeyaprakash et al., 2016; Coskun et al., 2017). Moreover, it was proven that HPD consumes the lowest energy among the other drying methods (Tunçkal and Doymaz, 2020). (in terms of
5 g of melon slices were weighted to measure moisture content in an oven at 105±3 °C. Moisture analysis was ceased once the two successive weights of the sample less than 1% (Koşan et al., 2020).
Melon slices were dried with a heat pump dryer whose technical properties and detailed figure were given before by Coskun et al. (2017). Before starting the drying process, the dryer was operated for about 30 min. to reach steady state conditions. The process input variables included drying air temperature, velocity and slice thickness ranging by 35 - 45 °C, 0.5 - 1.0 m/s and 5 - 9 mm, respectively. Following weighing of 635 g of melon slices, they were distributed homogeneously on the drying tray, and consequently the drying process was started. During drying process, the mass loss of samples was measured by using the load cell at every four min. and all data were recorded by a computer connected to the system. The temperature and relative humidity of air within the drying system were measured every one minute by a data collector. When the moisture content of the melon slices decreased about 8±0.5 % (wet basis), the drying procedure was finished. Energy consumption of the compressor was measured by a digital wattmeter (Makel, Turkey) every one hour followed by recording the data. Drying system operates with ± 0.8 °C sensitivity by a digital thermostatic control.
The performance of HPD system is expressed in terms of specific
moisture extracted ratio (SMER) and the coefficient of performance (COP). SMER
is defined as the water extracted from the product per consumed energy; and COP
is the ratio between the heat delivered to the drying air through the condenser
) and
energy consumed at the compressor (
(Jia et al.,
1990). COP for HPD system was calculated by Eq. 1.
(1)
where
represents
coefficient of performance of heat pump.
The
COP of the overall system (
) was based on Eq. 2:
(2)
where
and
represents
power consumption (kJ/s) of the internal and external condenser fan,
respectively.
Heat transfer rate (kJ/s) of the internal condenser was used to increase the enthalpy of the drying air as given in Eq. 3.
(3)
where
and
represents
mass flow rate of air (kg/s), specific enthalpy of air at the exit and at the
inlet (kJ/kg) of the condenser, respectively.
SMER (specific moisture added ratio) represents the total amount of energy consumed per the moisture absorbed from the product and calculated using the following equation (Jia et al., 1990).
(4)
where
represents
amount of water evaporated from the melon during drying process (kg/s).
Seven drying models were applied to determine the best model for drying characteristics of melon slices. These models were given as following equations (Özkan Karabacak et al., 2020):
Page:
(5)
Modified Page:
(6)
Logarithmic:
(7)
Lewis:
(8)
Henderson & Pabis:
(9)
Two Term Exponential: ![]()
(10)
Wang & Singh:
(11)
where
,
, and
represent
model constant,
is the coefficient in the drying model (1/s) and
is the drying
period (s).
The moisture ratio (
) and drying
rate of the samples (
) (g/s) were
estimated from the following equations:
(12)
In Eq. 12,
,
,
,
are the moisture ratio, the moisture content
at a specific time (g water/g dm.), moisture content (g water/g dm.) of the
sample prior to drying, moisture content (g water/g dm.) at equilibrium state,
respectively (Tüfekçi and Özkal, 2017). Equilibrium moisture content was
accepted as zero since
is much lower
than
and
values.
(13)
where
and
represent the weight (g) of the melon before drying and after
drying, respectively.
refers to the
duration of the drying process (s).
The highest correlation coefficient (R2) and lowest root mean square error (RMSE), Chi square (χ2) were used as the statistical parameters to identify the integrity of the fit models describing the drying kinetics of melon slices (Gamlı et al., 2018). Subsequent equations were used for the calculation of these values:
(14)
(15)
Here,
and
are the experimental and
dimensionless moisture ratios, respectively for the test
.
is the number
of observations and
is the
constant number for the models.
E. Effective moisture diffusivity (Deff)
Fick’s second diffusion law is broadly utilized for the estimation of effective moisture diffusivities of agricultural products (Süfer and Palazoğlu, 2019). The mathematical explanation of Fick’s law is given in Eq. 16, based on the assumptions including uniform initial moisture diffusion, negligible shrinkage, constant diffusion coefficient throughout the process and symmetric mass transfer in an infinite slab,
(16)
In Eq. (16)
,
,
and
represents
dimensionless moisture ratio, effective moisture diffusivity (m2/s),
half thickness of the slab in the melon slices (m) and positive integer,
respectively. For sufficiently extended drying periods, Eq. (17) can be
abbreviated to the first term in the series by using a logarithmic form as
follows:
(17)
was computed through the slope of a straight line which was plotted
versus time
in drying experiments. The equation was expressed as follows:
Table 1. Box–Behnken matrix of independent variables used in the RSM design
|
Values |
Parameter |
Levels |
||
|
-1 |
0 |
1 |
||
|
|
Drying air temperature (ᵒC) |
35 |
40 |
45 |
|
|
Slice thickness (mm) |
5 |
7 |
9 |
|
|
Drying air velocity (m/s) |
0.5 |
0.75 |
1 |
Table 2. Experimental Design

(18)
Colour measurements were carried out with a chroma meter (CR-5, Konica Minolta, Osaka-Japan). L* value indicates the change from vertical luminous intensity to darkness, (+a*) redness, (−a*) greenness, (+b*) yellowness, (−b*) blueness. Measurements were performed in triplicate, and the average was used for further calculations.
Response Surface Methodology (RSM) was applied to
evaluate the effect of independent variables including air temperature (
), slice
thickness (
) and drying
air velocity (
) on depended
variables which include drying time (
), total
energy consumption (
),
,
,
, drying rate (
), and colour
parameters (L*, a*, b*) (
,
,
). A three
level of Box-Behnken design was used for RSM study. Three factors and their
levels (-1, 0, 1) were determined based on the preliminary experimental trials.
1, 0, and -1 represent high, optimal and low value. This experimental design
involved 17 experimental trials carried out in a randomized order. Factors,
their levels and experimental design including coded and uncoded values were
illustrated in Table 1 and Table 2.
All experiments were performed in triplicate, and each sample was analyzed in duplicate. Average analysis results of each trial were used to draw three dimensional contour plots and consequently were evaluated to establish an optimization model. The contour surface as a bi-dimensional projection of RSM was a proper tool to determine a relationship between drying parameters of the process and the studied variables.
A second order polynomial equation (Eq. 19) was fitted to model each responses, i.e. depended variables as a function of independent variables.
![]()
(19)
In this equation, coefficients of the model were
(constant),
,
,
(linear),
,
,
(interaction),
,
,
(quadratic).
Second-order coefficients of model equations were generated by regression analysis with Minitab statistical software (version 17, Minitab Inc., Pennsylvania, USA). The goodness of fit of the model was evaluated by the coefficient determination (R2). The significance of the estimated regression coefficient for each response variable was assessed by using a 5% test of significance at a probability (p) of 0.05. Moreover, optimum levels were determined by optimizing the responses.
III. RESULTS AND DISCUSSION
A. Analysis the Response Surface Models
The analytical results obtained from all the experiments designed based on Box–Behnken model for drying of melon slices were given in Table 3. Those experimental data were used to determine the coefficients of the quadratic polynomial equations given Eq. 19. The resulting model parameters were demonstrated in Table 4 providing regression coefficients for each dependent variable. The determination coefficient (R2) for most of the responses except colour ranged from 0.9772 and 0.9928, indicating a high correlation between predicted and observed values. The alterations in moisture content of melon slices over time were illustrated in Fig. 3. Drying time of the melon samples changed between 244 - 792 min.
Drying time:
Drying time (
) of the melon
samples changed between 244 and 792 min. The quadratic model for drying time
can be expressed by the following equation.
![]()
![]()
(20)
From the Eq. (20), it can be
observed that while linear terms of drying air temperature (
) and
drying air velocity (
) had negative
impact on drying time, slice thickness (
) had positive
effect on it. Quadratic term of slice thickness (
) had the highest positive effect. However, drying time significantly
negative influenced by the quadratic terms of drying air velocity (
) (p<0.05). Maximum drying time was determined for in Run 11.
However, minimum drying time was found in Run 3. It was prevailed that drying
time decreased by reducing the slice thickness and increasing the drying air
velocity and temperature (Fig. 1a). Those results were in line with the
previous studies reported in the literature in which increasing air temperature
(Phahom et al., 2021) and drying air velocity (Ndukwu, 2009) and reduced
slice thickness (Sadin et al., 2014) led to a reduction on drying time.
Total energy consumption
Total energy consumption (
) in kWh
changed between 3.008 - 9.258 kWh. The quadratic model for total energy
consumption can be expressed by the following Eq. (21):
![]()
![]()
(21)
From Eq. (21), it can be monitored that while linear terms of drying
air temperature (
) and
drying air velocity (
) had negative
impact on total energy consumption, slice thickness (
) had positive
effect on it. Similar to drying time, quadratic term of slice thickness (
had the
highest positive effect on total energy consumption. However, total energy
consumption was significantly influenced by the quadratic terms of drying air
velocity (
) in a
negative manner (p<0.05). Maximum total energy consumption was determined
for in Run 3. In contrast, the lowest total energy consumption was found in Run
11. The graphical representation of the influence of slice thickness (
) and drying
air temperature (
) on
total energy consumption (Fig. 1b) revealed that when drying air temperature
increased to 40 – 45 °C and minimum slice thickness was applied, total energy
consumption was the lowest. Also it can be observed that lower drying air
velocity (< 0.8 m/s) and lower drying air temperature (35 °C) had negative
influence on total energy consumption. The effect of slice thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40°C) demonstrated that increase of slice
thickness resulted in higher total energy consumption.
HPD system analyses
(
) changed
between 1.430 and 3.074. The quadratic model for
can be
expressed by the following Eq. (22):
![]()
![]()
(22)
From the Eq. (22), it can be monitored that while linear
terms of drying air temperature (
) and
drying air velocity (
) had positive
impact on
, slice
thickness (
) had negative
effect on it. Quadratic term of drying air temperature and slice thickness (
and
had negative
effect on
. However,
positive
influenced by the quadratic terms of drying air velocity (
) (p<0.05).
Maximum
determined
for in Run 8. However, minimum
was found in
Run 5. Factorial plots for
demonstrated
that when drying air temperature increased,
was also
increased (Fig. 1c). It can be also observed that lower drying air velocity
(< 0.8 m/s) had negative influence on
. The effect
of slice thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40 °C) was represented in Figure 1c,
demonstrated that increase of drying air velocity (> 0.75 m/s) resulted in
higher
.
(
) changed
between 1.359 and 2.749. The quadratic model for COPhp can be expressed
by the following Eq. (23):
![]()
![]()
(23)
From the Eq. (23), it can be determined that both linear and
quadratic terms of slice thickness (
and
) had negative effect on
(p < 0.05). Although maximum
determined
for in Run 8, minimum
was found in
Run 9.
Those results were consistent with previous studies
performed with
in which 2.72
value was
obtained for banana at 48 – 52 ᵒC drying air
temperature and 0.4 m/s drying air velocity conditions (Kuan et al.,
2019) and
values
between 2.11-2.96 were obtained for
grated carrots at 56 °C drying air temperature (Aktaş
et al., 2019). On the other hand
values of the
melon slices were found lower than mint leaves were dried by heat pump dryer at
40 °C drying air temperature and 1.8 m/s
drying air velocity conditions. Factorial plots for
showed that
when drying air temperature (
) was
increased,
was also increased (Fig. 1d). It can be seen that drying air
velocity (
) (> 0.8
m/s) had positive influence on
. The effect of slice thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40°C) was showed in Fig. 1d,demonstrated that
increase of drying air velocity (> 0.75 m/s) resulted in higher
.
(
) changed
between 0.125 and 0.215 kg/kWh. The quadratic model for
can be
expressed by the following Eq. (24):
![]()
![]()
(24)
According to Eq. (24), both drying air temperature (
) and drying
air velocity (
) had positive
correlation, but slice thickness (
) had negative
correlation on SMER value. Moreover, it was significantly negative influenced
by the quadratic term of drying air temperature (
). Quadratic
terms of slice thickness (
) and drying
air velocity (
) had highest
positive effect on it (p < 0.05). Similar to drying time and total energy
consumption, maximum
was
determined for in Run 11. However, minimum
was found in
Run 3. In previous studies
values were
obtained as 2.05 kg/kWh for mango by Wang
et al. (2019), 0.6 kg/kWh for banana
by Kuan et al. (2019), 1.64 kg/kWh
for red jujube by Yuan et al. (2019) and 0.06
kg/kWh for ginger by Chapchaimoh et al. (2016).
The graphical representation of
the influence of slice thickness (
) and drying
air temperature (
) on
value (Fig. 1e)
revealed that when both drying air temperature decreased and slice thickness
increased (> 6 mm),
value was
reduced. From Fig. 1e it can be seen that lower drying air velocity (< 0.8
m/s) and lower
Table 3. The results of analyzed responses for dried melon slices

Table 4. Summary of regression analysis response


Figure 1. Response factorial plot showing the effects of drying air temperature, slice thickness and drying air velocities on the drying time, total energy consumption, COPhp, COPws, SMER, drying rate, L* value, a* value and b* value
drying air temperature (35 °C) had negative influence on
value. The
effect of slice thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40 °C) demonstrated that increase of slice
thickness resulted in lower
value.
Drying rate
Drying rate (
) changed
between 0.718 and 2.295. The quadratic model for
can be
expressed by the following Eq. (25):
![]()
![]()
(25)
According to Eq. 25, while drying air temperature and
drying air velocity (
and
) had positive
correlation, linear and quadratic terms of slice thickness (
and
) had negative
correlation on drying rate. Quadratic term of drying air velocity (
) had highest
positive effect on it (p < 0.05). Accordingly drying time, total energy
consumption and
value, maximum drying rate was determined for in Run 11. However,
minimum drying rate was found in Run 3. Factorial plots demonstrated that
drying rate was reduced when both drying air temperature (
) decreased
and slice thickness (
) increased
(> 5 mm) (Fig. 1f). It can be observed that lower drying air velocity (
) (< 0.8
m/s) and lower drying air temperature (
) had negative
influence on drying rate. The effect of slice thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40 °C) indicated that decreased slice
thickness (
) and
increased drying air velocity (
) resulted in
higher drying rate.
Colour values
L* value
L* value (
) changed
between 59.30 and 82.62. The quadratic model for L* value can be
expressed by the following Eq. (26):
![]()
![]()
(26)
While drying air temperature (
) had positive
correlation, slice thickness and drying air velocity (
and
) had negative
correlation on L* value. Moreover, L* value was significantly
negative influenced by the quadratic terms of drying air temperature (
). Quadratic
term of slice thickness (
) had highest
positive effect on it (p < 0.05). While maximum L* value was
determined for in Run 10, minimum L* value was found in Run 7. Factorial
plots showed that L* value was reduced when minimum drying air
temperature (
) applied and
slice thickness (
) was between
(6 – 8.5 mm). Especially 39 - 43 °C drying air temperatures caused the highest L*
value (Fig. 1g). It can be seen that low drying air velocity (
) (0.5 – 0.65
m/s) and lower drying air temperature (
) (37 - 41 °C)
had highest positive influence on L* value. The effect of slice
thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40 °C) was represented in Fig. 1g, demonstrated
that 6.5 – 8 mm slice thickness and drying air velocity > 0.8 m/s resulted
in lower L* value. Moreover it can be seen from Table 3, when the other
two parameters were constant, reduction in slice thickness and increase in
drying air temperature and drying air velocity caused higher L* value. In
general, non-enzymatic Maillard browning reactions and the decomposition of
pigments are responsible for the advancement of discolouration in dried melon
slices (Ibarz et al., 1999).
a* value
a* value (
) changed
between -2.95 and 6.73. However Oliveira et al. (2020) reported a* value as between -0.74 and 3.22 in
melon snack enriched in calcium. The quadratic model
for a* value can be expressed by the following Eq. (27):
![]()
![]()
(27)
From the Eq. (27),
it can be observed that both of the terms
and
(drying air
temperature and drying air velocity) had negative impact, while
had positive
effect on a* value. Moreover, a* value was significantly negative
influenced by the quadratic terms of drying air temperature (
and
). Quadratic
term of slice thickness (
) had positive
effect on it (p < 0.05). When the highest a* value was found at Run
16, the lowest a* value was found at Run 7. From the Fig. 1h the
influence of slice thickness and drying air temperature on a* value
demonstrated that when 38 - 43 °C drying air temperature and the highest slice
thickness (9 mm) applied, a* value was the highest. Minimum a*
value was obtained when 43 - 45 °C drying air temperature applied to melon
slices having thickness below 7 mm. It can be also observed that 0.6 - 0.7 m/s
drying air velocity and drying air temperature below 40 °C caused highest a*
value. The effect of slice thickness (
) and drying
air velocity (
) at center
point of drying air temperature (40 °C) showed that 0.9 – 1 m/s drying air
velocity and slice thickness lower than 7 mm resulted in lower a* value.
The increase of a* value in dried melon slices might be due to the
Maillard reaction and degradation of pigments such as carotenoids (Özkan
Karabacak et al., 2020).
b* value
b* value (
) changed
between 18.51 and 33.20. The quadratic model for b* value can be
expressed by the following Eq. (28):
![]()
![]()
(28)
According to Eq. (28), while linear terms of drying air temperature and
slice thickness (
and
) had positive
correlation, drying air velocity (
) had
negative correlation on b* value. Moreover, b*
value was significantly positive influenced by the quadratic terms of (
). Quadratic
terms of drying air temperature and drying air velocity (
and
) had negative
effect on it (p < 0.05). Maximum b* value was determined for
in Run 4. Similar to L* value and a* value, minimum
b* value was also found in Run 7. Factorial plots depicted that b*
value was minimum when drying air temperature was 35 °C and
Table 5. Criteria for optimization for process conditions

slice thickness was between 6.5 - 9 mm. Besides that, when drying air temperature was between 43 – 45 °C and slice thickness was below 6 mm, b* value also reduced (Fig. 1i). It can be observed that drying air velocity between 0.65 - 0.95 m/s and drying air temperature higher than 39 °C resulted in higher b* value. The effect of slice thickness and drying air velocity at center point of drying air temperature (40 °C) was represented in Figure 1i, demonstrated that slice thickness between 8.5 – 9 mm and drying air velocity 0.65 – 0.85 m/s resulted in higher b* value. Oliveira et al. (2020) determined that all dried melon samples showed higher b* values (17.40 - 26.47) than fresh melon. Similarly, the b* values found in our research were obtained in a range of 18.51 - 33.20.
B. Optimization of levels of independent variables
In order to optimize the levels of the independent variables for
drying melon slices having high quality, the responses were assigned equal
importance on the basis of their effects on the quality of final product. The
used criteria, actual and predicted responses were given in Table 5. The
optimal condition for all responses with composite desirability of 0.9125 was:
45 °C (
), 1 m/s (
) and 5.04 mm (
).
Effective moisture diffusivity (
) values
obtained for each runs were presented in Table 3.
values of
melon slices were in the range of 7.075E-10 - 1.843E-07 m2s-1.
These values were stated in the common range (10-11- 10-6
(m2s-1)) determined for the dehydration of food products
(Surendhar et al., 2019). Increasing drying air temperature, drying air
velocity and slice thickness (
,
and
) led to an
increment on
of the melon
slices. Higher drying temperatures and velocities lead to higher heating energy
and thus water molecules with increased activity cause high moisture diffusion
(Akoy, 2014; Phahom et al., 2021). The effect of slice thickness (
) on
was more
important than the other parameters. Because slice thickness (
) is directly
related with
(Eq. 18). If a melon slice is thin, diffusion occurs in one
direction from internal part of the slice through its external surface, while
side diffusion is negligible. On the other hand, considering a thick melon
slice, diffusion may also take place from side surfaces which enhance the
removal rate of water from a slice. In addition, surface hardening effect
occurs faster at thinner melon slices which will hinder the diffusion of
moisture in thin melon slices, resulting lower effective moisture diffusivity
in thinner melon slices (Chin et al., 2015). In accordance with our results, Xia et al. (2014) found that
of
Hami-melon slices varied from 10.65×10-10 to 33.76×10-10
m2/s and from 8.06×10-10 to 39.97×10-10 m2/s
with increasing drying temperature (from 50 ⁰C to 80 ⁰C) and sample thickness
(from 3 mm to 11 mm), respectively. Our results are also consistent with this
existing in the literature for dried melon (Cucumis melo) slices
obtained by air drying varied from 1.21×10−8
m2/s to 4.18×10−8 m2/s for slice thickness of
4 mm, and from 1.69×10−8 to 8.54×10−8 m2/s for
slice thickness of 6 mm (Azadbakht et
al., 2012).
D. Thin layer drying models
Drying behavior of melon slices with optimal conditions (45 °C drying air temperature, 1 m/s drying air velocity and 5.04 mm slice thickness) acquired with Box-Behnken design, was evaluated with seven different thin layer drying models. The statistical parameters based on R2, RMSE and χ2 values ranged from 0.8804 to 0.9940, 0.001459 to 0.0.024127 and 0.000136 to 0.037927, respectively. The most proper model to represent the drying characteristics of melon slices were chosen Wang & Sing model. This result was coherent with previous study reported that Wang & Singh model for mint leaves was accepted as the most suitable theoretical model (Kavak Akpinar, 2010). Regarding the studies based on melon, Azadbakht et al. (2012) found Midilli model as the most appropriate one and da Cunha et al. (2020) reported that the best fit was obtained by using the Logarithmic and Wang & Singh models for ethanol pre-treated melon samples while The Two Terms exponential gave good statistical values for the dried melons without the pre-treatment during convective drying.
In this study, the optimization process was obtained by
using
for having
high quality drying melon slices with closed loop
system. An optimum drying temperature of 45 °C, air velocity of 1 m/s and
slice thickness of 5.04 mm were recommended with following predicted responses
close to experimental values: drying time 216.58 min, total energy consumption
2.94 kWh,
3.08,
2.75,
0.22 kg/kWh,
drying rate 2.53, L* value 82.53, a* value -1.83 and b*
value 25.82. The most suitable model to represent the drying behavior of optimum
melon slices was chosen as Wang & Sing. Effective moisture diffusivities (
) of the melon
slices were ranging from 7.075E-10 - 1.843E-07 m2s-1 and
increasing drying air temperature, drying air velocity and slice thickness led
to an increment of
. By the
optimization of drying parameters of melon slices novel healthy snacks were
provided with minimum energy consumption and maximum moisture diffusivity and
attractive colour properties.
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Received: August 17, 2021
Sent to Subject Editor: September 16, 2021
Accepted: November 9, 2021
Recommended by Subject Editor Laura Briand