analysis of chemical and structural changes in kiwifruit (actinidia deliciosa cv
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Analysis of chemical and structural changes in kiwifruit (Actinidia deliciosacvHayward) through the osmotic dehydration
M. Castro-Girldez a, U. Tylewicz b, P.J. Fito a,, M. Dalla Rosa b, P. Fito a
a Instituto Universitario de Ingeniera de Alimentos para el Desarrollo, Universidad Politcnica de Valencia, Camino de Vera s/n, 46022 Valencia, Spainb Department of Food Science, Alma Mater Studiorum, University of Bologna, Piazza Goidanich 60, 47521 Cesena (FC), Italy
a r t i c l e i n f o
Article history:
Received 25 August 2010
Received in revised form 22 March 2011
Accepted 26 March 2011
Available online 31 March 2011
Keywords:
Osmotic dehydration
Thermodynamics
Mass transfer
Enthalpyentropy compensation
Kiwifruit
a b s t r a c t
Osmotic dehydration experiments of kiwifruit (Actinidiadeliciosacv Hayward) were carried out in order to
apply a nonlinear irreversible thermodynamic model. Samples were immersed into 65% (w/w) sucrose
aqueous solution at 30 C during5, 10, 15, 20, 30, 45, 60, 90, 120, 180, 250, 320, 400, 720, 1440 min. Some
physicalchemical parameters were measured in fresh, treated and reposed (24 h at 30 C) samples. It
was possible to apply the enthalpyentropy compensation coupled to a nonlinear thermodynamic model,
obtaining the apparent bulk modulus and explaining the elastic answer of the tissue throughout the
osmotic process. The osmotic dehydration also produces losses in the native compounds of kiwifruit such
as citric acid and Calcium and Potassium.
2011 Elsevier Ltd. All rights reserved.
1. Introduction
Osmotic treatment is a dehydration technique usually used in
fruits and vegetables, which produces a reduction in food water
activity and therefore allows storing the foods for longer periods
improving the stability and quality of products. Osmotic
dehydration consists on the introduction of foods in a low water
activity solution in order to induce water outflows and inflows of
external solutes (Ferrando and Spiess, 2001). This treatment
depresses the food water activity and improves the biochemical
and microbiological stability. The structure of plant tissue can be
considered as one of the main factors for understanding the
osmotic dehydration process (Mavroudis et al., 1998). Osmotic
dehydration in a biological system involves complex mass transfer
phenomena simultaneously (chemical and also mechanical) pro-
ducing physical and structural changes. These changes weredescribed for isolated cells by Segu et al. (2010) and thermody-
namically quantified in apple tissue by Castro-Girldez et al.
(2011).
Kiwifruit is a biological system constituted by three distinct
tissue types, namely outer pericarp, inner pericarp and core. The
core is composed by spherical/ellipsoidal cells (0.1 and 0.2
mm diameter), whereas the outer pericarp is composed by large
cells (0.50.8 mm diameter) dispersed in a matrix of smaller cells
(0.10.2 mm diameter) (Hallett et al., 1992). The inner pericarp
consists on the locules, which are enclosed within locule walls
(Hallett et al., 1992). Each locule is composed by large radially
elongated thin-walled cells (0.20.4 mm >1 mm) and seeds,
while the locule wall is a narrow region composed by smaller
thicker walled cells (Hallett et al., 1992). Each of these tissues
has different chemical composition (Ferguson, 1980; MacRae
et al., 1989a), texture properties (MacRae et al., 1989b; Jackson
and Harker, 1997), cell wall composition (Redgwell et al., 1991,
1992) and cell characteristics (Hallett et al., 1992).
Gerschenson et al. (2001)reported that kiwifruit behaves as an
elastic solid with storage moduli dominating the viscoelastic re-
sponse when it is subjected to an osmotic dehydration process.
In this complex scenario, very little work has been carried out to
analyze the effect of osmotic dehydration on structure and compo-
sition of kiwifruit, and to understand the mechanisms that impulse
the mass transfer through this operation.On the other hand, thermodynamics is one of the approaches
used to understand the properties of foods and to calculate energy
requirements associated with transfer of heat and mass in biolog-
ical systems (Fasina, 2006). The enthalpyentropy compensation
theory has been reported in many processes (Ziga et al., 2008;
Liu and Guo, 2001). This theory pointed out that variations ofdH
are compensated by variations in dS. Thus, representing both ener-
gies, a linear relation is obtained (Eq. (1)).
dS adHb 1
wherea and b values are constants; a is inversely proportional to
the temperature (Ziga et al., 2008).
0260-8774/$ - see front matter 2011 Elsevier Ltd. All rights reserved.doi:10.1016/j.jfoodeng.2011.03.029
Corresponding author. Tel.: +34 96 387 9832; fax: +34 96 387 7369.
E-mail address: [email protected](P.J. Fito).
Journal of Food Engineering 105 (2011) 599608
Contents lists available at ScienceDirect
Journal of Food Engineering
j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / j f o o d e n g
http://dx.doi.org/10.1016/j.jfoodeng.2011.03.029mailto:[email protected]://dx.doi.org/10.1016/j.jfoodeng.2011.03.029http://www.sciencedirect.com/science/journal/02608774http://www.elsevier.com/locate/jfoodenghttp://www.elsevier.com/locate/jfoodenghttp://www.sciencedirect.com/science/journal/02608774http://dx.doi.org/10.1016/j.jfoodeng.2011.03.029mailto:[email protected]://dx.doi.org/10.1016/j.jfoodeng.2011.03.029 -
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The objectives of this work are to quantify the effect of the os-
motic dehydration treatment in the kiwifruit structure for short
treatment times in a system with a fast mechanical response,
and to develop a methodology for calculating the phenomenologi-
cal coefficient by applying the compensation theory.
2. Material and methods
Sucrose solution (65% w/w, 30 C), prepared with commercial
sugar and distilled water, was used as osmotic agent. Before the
experiment, kiwifruits (Actinidiadeliciosa cv Hayward) with the
same size and ripeness were bought from a local supermarket
and kept refrigerated until use. The kiwifruits were cut with a cali-meter in half slices (1 cm thickness) and the core was eliminated.
There were prepared 47 samples which were immersed in a vessel
containing the osmotic solution with continuous stirring. The rela-
tion between the fruit and the solution was of 1:20 (w/w) to avoid
changes in the solution during the process. The system was main-
tained at 30 C in a constant-temperature chamber. To prevent
evaporation the vessel was covered with a sheet of plastic wrap.
Preliminary kinetic studies were done at the same working con-
ditions in order to select the osmotic dehydration times. These re-
sults show that, in the first minutes of treatment, some structural
changes occur affecting the rest of treatment. Therefore, the se-
lected times for the present study were: 5, 10, 15, 20, 30, 45, 60,
90, 120, 180, 250, 320, 400, 720, 1440 min. Six samples were used
at each dehydration time.A flow-diagram of the experimental procedure is presented in
Fig. 1.
Three samples per osmotic treatment time were reposed at
30 C for 24 h, on Decagon containers, closed with parafilm, in or-
der to eliminate the concentration profiles in samples.
Mass, volume and surface water activity were analyzed for each
fresh, treated and reposed samples. Representative fresh samples
were used to determine the initial moisture, sugar content (Brix),
citric acid content, cation content and Cryo-SEM. Moisture and su-
gar content (Brix) were measured for each reposed sample. The
other three samples per time were used for the cation analysis, cit-
ric acid content and Cryo-SEM.
At each osmotic time, an aliquot of sucrose solution was also ta-
ken from the vessel. Water activity and Brix of the solution weremeasured at each time.
Mass was determined by using a Mettler Toledo Balance
(0.0001) (Mettler-Toledo, Inc., USA).
Volume was determined by analyzing the front and the section
pictures of samples using millimetres paper in the background by
using an imaging analysis with the software Adobe Photoshop
(Adobe Systems Inc., San Jose, CA, USA) in order to get the diameter
and the thickness of the samples.
Surface water activity was measured in the structured samples
with a dew point hygrometer Aqualab series 3 TE (Decagon De-
vices, Inc., Washington, USA).
Moisture was determined by drying in a vacuum oven at 60 C
till constant weight was reached (AOAC Method 934.06, 2000). Su-
gar content was determined in a refractometer (ABBE, ATAGOModel 3-T, Japan). The titrable acidity (referred to citric acid)
was analyzed by usingAOAC Method 934.06 (2000).
Analytical determinations described above were obtained by
triplicate.
Cation quantification was carried out by means of an ion chro-
matograph (Methrom Ion Analysis, Herisau, Switzerland), using an
universal standard column (Metrosep C2150, 4.0 150 mm)
along with an eluent composed of tartaric acid (4.0 mmol/L) and
dipicolinic acid (0.75 mmol/L), equipped with electronic detectors.
In every case, the fruit samples were previously homogenized at
9000 rpm in an ULTRATURRAX T25 for 5 min and centrifuged (J.P.
Selecta S.A., Medifriger-BL, Barcelona, Spain) at 4000 rpm for
20 min. Afterwards, 1 mL of supernatant was diluted with
Milli
-Q water in a 50 mL Erlenmeyer flask. The clarified extractwas filtered through a 0.45 lm Millipore filter; 15 mL was used
to analyze the cation content. Measurements were taken in
duplicate.
2.1. Low temperature scanning electron microscopy (cryo-SEM)
A Cryostage CT-1500C unit (Oxford Instruments, Witney, UK),
coupled to a Jeol JSM-5410 scanning electron microscope (Jeol,
Tokyo, Japan), was used. The sample was immersed in slush N 2(210 C) and then quickly transferred to the Cryostage at 1 kPa,
where sample fracture took place. The sublimation (etching) was
carried out at 95 C; the final point was determined by direct
observation in the microscope, working at 5 kV. Then, once againin the Cryostage unit, the sample was coated with gold in vacuum
Nomenclature
aj activity of the chemical speciej ()G Gibbs free energy (J)Gj partial Gibbs molar free energy of the speciej (J/mol)Jj molar flux of the speciej (mol/m
2s)Lj phenomenological coefficient of the specie j (mol
2/
J s m2)Mr molecular weight (g/mol)M mass (g)n number of moles (mol)P absolute pressure (atm)R ideal gases universal constant (J/mol K)A surface area (m2)S entropy (J/mol K)H enthalpy (J/mol)T temperature (K)t time (min)V volume (m3)x mass or molar fraction ()z mass or molar fraction of the liquid fraction ()
F force (N)l displaced distance (m)F molecular force (N/mol)
Greek alphabetlj chemical potential of the speciej (J/mol)l0j chemical potential of reference of the speciej (J/mol)m specific volume (L/mol)D variation of a variableg apparent bulk modulus
Subscript and superscript0 initial time24 time 24 h after the treatmentLP liquid phasemax maximums sucrosew watert time (min)
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(0.2 kPa), applied for 3 min, with an ionizationcurrent of 2 mA. The
observation in the scanning electron microscope was carried out at
15 kV, at a workingdistance of 15 mmanda temperature6130 C.
3. Results and discussion
The osmotic dehydration operation with 65Brix solution pro-
duces compression and relaxation phenomena (Fito and Chiralt,1997). These mechanisms could be observed by analyzing the mass
and volume variations. Fig. 2 shows the overall mass variation,
water loss and sucrose gain through the osmotic treatment. In
the figure, the decrease in total mass is explained by the high water
losses while the sucrose mass increases during the osmotic treat-
ment. InFig. 3, the volume variation is observed; it is possible to
appreciate the overall decrease in volume through the osmotic
treatment. The half slice of kiwifruit can be divided in two zones
(see Fig. 4c), zone A represents the external zone composed by
homogeneous reservoir cells explained in the introduction; and
zone B represents the internal part of the tissue, where the reser-voir and vascular cells are combined in radial way. These two zones
show different directions in the mechanical tension, during the
contraction and expansion.
Fig. 1. Diagram of the experimental procedure.Cryo-SEM was made in fresh and treated samples until 60 min of treatment.
Fig. 2. Evolution of overall mass (), water mass (j) and sucrose mass (N) variation through the osmotic treatment.
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Kiwifruit behaves as a viscoelastic solid and it is possible toappreciate, at the beginning of the treatment, the important
expansions and contractions of the tissue (Fig. 4a and b). Fig. 5a
shows a Cryo-SEM micrograph of fresh kiwi where the intracellular
and extracellular spaces and membrane/wall system are identified,
showing the extracellular spaces filled of air. In the first 5 min of
treatment, the fruit suffers an important lost of turgid, and a 25%
of contraction can be appreciated in the overall volume; Fig. 5b
shows the tissue with the extracellular space filled with liquid.
Afterwards, until 15 min of treatment, the fruit suffers expansions,
recovering 93% of the initial volume, recovering the zone A; Fig. 5c
shows the membrane/wall system intact, thus the expansion must
be a response of the tissue to the first fast contraction. At 20 min of
treatment, the fruit again is contracted strongly (32% of the initial
volume), disappearing again the zone A and contracting the zone B.
After this time, the expansion/contraction phenomena are less
marked and, at long osmotic times, the fruit is completely retracted
(Fig. 4a) and zone B is absolutely contracted. It is important to
highlight that although the fruit suffers important expansions at
the beginning of the treatment, it is dehydrating and losing overall
weight (Fig. 2).
Second expansion occurs at 30 min, as shows Fig. 4b, recovering
no more than 5% of volume;Fig. 6a and b, show Cryo-SEM pictures
of samples treated 30 min and figures c and d show Cryo-SEM pic-
tures of samples treated 45 min. All pictures show an initial plas-
molysis so incipient. Therefore the second expansion must be
also an elastic response to the second fast contraction.
The water and solute fluxes promoted in the osmotic treatment
can be estimate with the mass variation, the process time and the
variation of the samples surface (Eqs. (2)and (3)):
Jw DMwMoDtAMrw
2
Js DMsMoDtAMrs
3
whereJw is the water flux (molw/s m2),Js is the sucrose flux (mols/
s m2) during the treatment,tis the process time, A is the measured
Fig. 3. Evolution of the volume variation through the osmotic treatment.
Fig. 4. Kiwifruit deformation through the osmotic dehydration; (a) pictures of fresh and treated kiwifruit at different treatment times; (b) volume variation curve at shorttreatment times and (c) detail of the zones of the kiwi tissue with the sense of the deformations.
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surface area of the sample (m2), Mrw is the molecular weight of
water (18 g/mol) and Mrs is the molecular weight of sucrose
(342 g/mol). It is possible to observe in Fig. 7 that both fluxes are re-
duced with treatment time promoted with the decreasing in driving
forces.
Fig. 8 shows a scheme of surface water activity measured in the
fresh, treated and reposed samples; these measurements represent
the water activity of the surface of each sample. After the repose
time, the moisture was analyzed in whole sample. The moisture
of treated samples was estimated by balances. Fig. 8 shows also
the relationship between the moisture in dry basis and the surface
water activity of the treated, reposed samples and data from pure
solutions of water and sucrose (Starzak and Mathlouthi, 2006). In
this figure it is possible to observe that the reposed samples main-
tain the same relationship surface water activity/moisture as the
pure sucrose solution at different concentrations. Therefore, the
water and sucrose concentrations are homogeneous in the reposed
samples because moisture is an average value of the whole sample
and the water activity is just the surface value. Thus, the concen-
tration profiles through the tissue are negligible. The surface water
Fig. 5. Cryo-SEM pictures at different treatment times; (a) fresh kiwi at 350; (b) treated sample at 5 min, at 1000and (c) treated sample at 15 min, at 200.
Fig. 6. Cryo-SEM pictures at different treatment times; (a) treated sample at 30 min, at 1000; (b) treated sample at 30 min, at 500; (c) treated sample at 45 min, at 500and (d) treated sample at 45 min, at 500.
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activity of treated samples is lower than that of the reposed sam-
ples; it denotes concentration profiles in the kiwifruit tissue and
an important internal transport is driven; only at the end of the
treatment, the treated and the reposed values concur with the pure
solution values; this fact denotes the disappearance of concentra-
tion profiles in the tissue.
Fig. 9 shows the water flux and the volume variation during the
24 h of repose time. In the figure, two steps can be observed: the
first one, composed by the samples treated less than 180 min,
shows fluctuant fluxes promoted by the shrinkage and swelling
of samples during the repose time (mechanical behaviours); the
second step, composed by the samples with treatment times high-
er than 180 min, shows a continuous decrease of fluxes without
volume variation, suggesting that the engine of the transport dur-
ing the repose time must be the gravity.
In order to determine the chemical and mechanical changes in
the kiwifruit tissue through the osmotic treatment, it is possible
to apply a thermodynamic analysis in terms of the Gibbs free
Fig. 7. Variation of water (d) and sucrose (s) fluxes versus time through the treatment.
Fig. 8. Relationship between the moisture in dry basis and the water activity for samples dehydrated (d), reposed 24 h (s), and sucrose solutions () obtained from Starzakand Mathlouthi (2006).
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energy, satisfying the enthalpyentropy compensation. For this
purpose, an interface was defined as the fruit surface in contact
with the osmotic solution (Fig. 10).
Using the relations of Maxwell (Demirel, 2002) (Eqs. (4) and
(5)), Eq.(6)is obtained for nonelectrolytic and isothermal system.
dG dHTdSSdT dUPdV VdPTdSSdT 4
dG VdPSdTFdl udeX
ldni 5
PdV TdS FdlX
ldni 6
Obtaining the entropy variation as follows:
dS1
T PdV Fdl
Xldni
7
Castro-Girldez et al. (2011)developed a non-equilibrium ther-
modynamic model for describing the long time osmotic dehydra-
tion through the apoplastic ways in apple tissue. The authors
defined the water chemical potential for a non ionic added solute
and an isotherm system, as follows:
dG
dnw
dlextw mwdPFwdlRTln
aOSsaes
JsJw
RTLnaOSwaew
8
where asis obtained from the bibliography (Lide, 2004), superscript
erepresents the external liquid phase (apoplastic way) close to the
interface, and superscriptOSrepresents the sucrose solution.
Therefore, it is possible to define the entropy variation by water
mol using Eqs.(7)and (8) as follows:
T dS
dnw RTln
aOSsaes
Js
JwRTln
aOSwaew
FwdlpwdV 9
Water and sucrose transport with the deformation tissue must
satisfy the entropyenthalpy compensation, therefore the relation-
ship between the entropy and the enthalpy must follow the Eq. (1).
In order to estimate those parameters, it is necessary to develop an
iteration with the free energy, entropy and enthalpy as it is
explained inFig. 11.
In Fig. 11, the phenomenological coefficient (Lw) is the supposed
variable to iterate and the compensation equation works to esti-
mate the error of the iteration. In the estimation of entropy and en-
thalpy, the term of expansions (pwdV) is present in both
developments; thus, in the compensation equation the term is can-
celled, being the entropy and the enthalpy without this term with
asterisk superscripts (dS
and dH
, respectively). On the other hand,the mechanical terms are packed in pressure term (vwdP) and the
elongation term (Fwdl), but the elongation term is important only
at the beginning of the dehydration process, when the turgid loss
mechanisms occur.
After the iteration, the phenomenological coefficient obtained
was Lw= 2.46 105 mol2/ J s m2. In fruits, different values of
phenomenological coefficients of water transport through the
protoplast membrane have been published; Ferrando and Spiess
(2002, 2003) showed in osmotic dehydration treatments with
sucrose solution at 30 C, 1 106 mol2/ J s m2 for onions, 5.2
106 mol2/ J s m2 for carrots and 6.8 106 mol2/ J s m2 for pota-
toes. Segu et al. (2006) reported the value of 4.5 105 mol2/
J s m2 for apple (var Fuji). Phenomenological coefficient for apo-
plastic transport in osmotic dehydration treatment with sucrosesolution at 30 C was published by Castro-Girldez et al. (2011)
Fig. 9. Water flux and volume variation during the repose time.
Fig. 10. Kiwifruit tissue scheme with the simplified phases used in the thermody-namic model (adapted fromCastro-Girldez et al., 2010).
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forappletissueobtainingthevalue: Lw= 1.095 105 mol2/ J s m2. In
animal tissue, phenomenological coefficient wascalculated for pork
meat salting process, Lw= 2.7 105 mol2/ J s m2 (Castro-Girldez
et al., 2010).
Fig. 12shows the relationship between the entropy and enthal-
py, resulted from the iteration, where the linear adjust of values
between 10 min to the end of treatment shows a good correlation
coefficient (R2 = 0.9941). It is possible to observe that, throughout
the first 5 min of treatment, the non consideration of the elonga-
tion term in the entropy estimation is not negligible. Using Eq.
(1) and the elongation in the entropy estimation (Eq.(9)), the elon-
gation term can be estimated by using next equation:
TdS
dnwRTln
aOSsaes
JsJw
RTlnaOSwaew
1 a Fwdl 10
Fig. 13 shows the elongation term through the dehydration pro-
cess, where it is possible to observe the high values of this term
during the lost of turgid pressure throughout the first minutes oftreatment.
Fig. 14 shows the volume variation as a function of pressure
variation throughout the interface estimated as was explained in
Fig. 11. The linear relation obtained allows calculating the apparent
bulk modulus following Eq.(11)(Bourne, 2002).
g DP
DVVi
11
The apparent bulk modulus obtained (3.9 MPa) reflects the elas-
ticity of wall-membrane system of kiwifruit. This value is similar to
the values of different elastic modulus obtained in other fruits:
1.84 MPa for Golden Delicious apples (De Baerdemaeker et al.,
1982), 39 MPa for different varieties of apple (Rosenfeld et al.,
1992), 5 MPa for an unripe green apples to 0.5 MPa for overripe
fruit (De Baerdemaeker et al., 1982; Duprat et al., 1997), 2.5 MPa
for pineapples (Chen and De Baerdemaeker, 1993), 1.9 MPa for
pears (Chen and De Baerdemaeker, 1993).
Osmotic solution only contains water and sucrose, then theactivity gradient of other native substances present in kiwifruit is
Fig. 11. Scheme of the iteration process developed in order to estimate the phenomenological coefficient.
Fig. 12. Relationship between the entropy and the enthalpy.
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Fig. 13. Evolution of the elongation term through the dehydration process.
Fig. 14. Volume variation as a function of pressure variation throughout the interface.
Fig. 15. Variation of citric acid during the treatment.
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so high and promotes high losses of this native substances. These
activity terms are coupled to contractions/expansions of the tissue
which provokes changes in kiwifruit composition; Figs. 15 and 16
show the changes in citric acid and in the most important kiwifruit
cations respectively during the osmodehydration treatment. It is
possible to appreciate how these components are reduced duringthe treatment.
4. Conclusions
It is possible to apply the enthalpyentropy compensation cou-
pled to a nonlinear thermodynamic model for determining the
water transport through the apoplastic ways in kiwifruit and to de-
scribe the behaviours involved in the osmotic dehydration. The
apparition of concentration profiles and the structural changes
was also determined. It is also possible to obtain the apparent bulk
modulus by the mechanical terms estimated in the thermody-
namic model, explaining the elastic answer of the tissue through-
out the osmotic process. The osmotic dehydration also produces
losses in the native compounds of kiwifruit such as citric acid
and Calcium and Potassium.
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Fig. 16. Variation of ions K+ and Ca+2 during the treatment.
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