Chitosan-Starch Beads Prepared by Ionotropic Gelation As Potential Matrices For Controlled Release of Fertilizers
Chitosan-Starch Beads Prepared by Ionotropic Gelation As Potential Matrices For Controlled Release of Fertilizers
Chitosan-Starch Beads Prepared by Ionotropic Gelation As Potential Matrices For Controlled Release of Fertilizers
PII: S0144-8617(16)30415-5
DOI: http://dx.doi.org/doi:10.1016/j.carbpol.2016.04.054
Reference: CARP 10994
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Please cite this article as: Perez, Jonas J., & Francois, Nora J., Chitosan-starch
beads prepared by ionotropic gelation as potential matrices for controlled release of
fertilizers.Carbohydrate Polymers http://dx.doi.org/10.1016/j.carbpol.2016.04.054
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Chitosan-starch beads prepared by ionotropic gelation as potential matrices for
controlled release of fertilizers
• Starch content and crosslinking time highly affect the macrobeads characteristics
Abstract
The present study examines the agrochemical application of macrospheres prepared with
chitosan and chitosan-starch blends by an easy dripping technique, using a sodium
tripolyphosphate aqueous solution as the crosslinking agent. These biopolymers form
hydrogels that could be a viable alternative method to obtain controlled-release fertilizers
(CRFs). Three different concentrations (ranging from 20 to 100 wt/wt % of chitosan) and
two crosslinking times (2 or 4 hours) were used. The resulting polymeric matrices were
examined by scanning electron microscopy coupled with energy dispersive X-ray, X-ray
diffraction, Fourier transform infrared spectroscopy, solid-state nuclear magnetic
resonance, thermogravimetric analysis and differential scanning calorimetry. Ionotropic
gelation and neutralization induced the formation of the macrospheres. The crosslinking
time and the composition of the polymeric hydrogel controlled the crosslinking degree, the
swelling behavior and the fertilizer loading capability. Potassium nitrate-loaded beads were
shown to be useful as a controlled-release fertilizer. After 14 days of continuous release
into distilled water, the cumulative concentration in the release medium reached between
70 and 93 % of the initially loaded salt, depending on the matrix used. The prepared beads
showed properties that make them suitable for use in the agrochemical industry as CRFs.
2.1. Materials
Chitosan of medium molecular weight (81% degree of deacetylation), native potato starch
and sodium tripolyphosphate (85 % purity) were purchased from Sigma-Aldrich (USA).
Lactic acid (85% wt/wt) and potassium nitrate were purchased from Cicarelli (Argentina).
All reagents used were of analytical grade and used as received.
A known mass of dried beads was put into a 200 mesh stainless steel spherical net. After
being immersed in distilled water for 3 hours with magnetic stirring, the samples were dried
at 40 °C for 48 hours and weighed. The soluble fraction was defined as the ratio between
the mass lost as a consequence of the water immersion and the initial mass of the dried
material before immersion.
(1)
2.4. Characterization
2.4.1 Scanning electron microscopy (SEM) with energy dispersive X-ray analysis (EDS):
Crosslinked chitosan and chitosan-starch macrospheres were mounted on aluminum stubs
with double-sided adhesive tape and sputter-coated with gold. The surface morphology was
examined with a Karl Zeiss Supra 40 SEM (Germany) with a field emission gun operated at
3 kV. The micrographs were taken at magnifications between 70 and 25000 X. Elemental
analysis was performed using an Oxford Instruments EDS (United Kingdom) coupled to
SEM.
XRD patterns were obtained using a Rigaku diffractometer with Bragg Brentano geometry
and CuKα radiation (λ= 0.1542 nm, 40 kV, 20 mA) in the range of 2θ = 5 – 50 º at a
scanning rate of 1 º/min and a scan step of 0.05 º. The chart speed was set to 5 °/min.
Measurements were performed at ambient conditions.
FTIR spectra of pure chitosan, pure starch and chitosan and chitosan-starch macrospheres
were recorded on a Nicolet 380 FTIR spectrometer (Thermo Scientific, Japan) operating in
the range of 4000 – 400 cm-1 at a resolution of 4 cm-1. The samples were ground and mixed
thoroughly with potassium bromide at a 1:20 (sample:KBr) mass ratio. KBr discs were
prepared by compressing the powder mixture with a hydraulic press.
2.4.4. Nuclear magnetic resonance (NMR)
High-resolution 13C solid-state spectra were recorded using the ramp 1H−13C and the
combined techniques of proton dipolar decoupling (DD), magic angle spinning (MAS) and
cross polarization (CP). Experiments were performed at room temperature in a Bruker
Avance II-300 spectrometer equipped with a 4-mm MAS probe. The operating frequency
for carbons was 300.13 MHz. Glycine was used as an external reference for the 13C spectra,
and the Hartmann−Hahn matching condition was set in the cross-polarization experiments
13
C spectra. The recycling time was 4 s. Different contact times during CP were employed
in the range of 200 − 1500 μs for 13C spectra.
A known weight of macrospheres was dried to a constant value and then immersed in
distilled water at room temperature. The experimental equilibrium swelling degree ( )
was calculated as:
(2)
where, is the weight of the swelled macrospheres at equilibrium and is the weight
of the dry polymeric matrix before the swelling process.
Potassium nitrate in powder form was dissolved in deionized water at a final concentration
of 20 % wt/wt. Dry polymeric matrices were immersed in the fertilizer-saturated aqueous
solution for 4 hours at room temperature. After the swelling process, the macrospheres
were dried at 40 ºC for 48 hours. The loading percentage was calculated using the
following equation:
(3)
Where and are the weights of the loaded and unloaded dry macrospheres,
respectively.
The release of potassium nitrate-loaded in the matrices was performed using deionized
water as the release medium. A constant fixed weight of loaded beads was placed inside a
steel basket that was immersed in 100 mL of deionized water at a constant temperature of
25 ºC under un-stirred conditions (static experiment). At fixed time intervals, the
cumulative concentration of KNO3 released was evaluated by measuring the conductivity
of the release medium with a Hanna Instruments HI 9033 multi-range conductivity meter.
The cumulative concentration of KNO3 was determined from the calibration plot.
The values reported are the means and standard deviations of experiments carried out at
least three times. Data were analyzed using a one-way analysis of variance (t-test), and
p<0.05 was considered significant.
As a consequence of the TPP dissolution and hydrolysis, the aqueous crosslinking solution
possesses OH− and tripolyphosphoric ions. Both ions can diffuse into hydrogels when the
polymeric material is in contact with the aqueous TPP solution. The OH− ions compete
with P3O105- ions for reaction with the protonated amino group of chitosan as soon as the
polymeric droplets come into contact with the sodium tripolyphosphate solution.
Taking into account that ionic crosslinking can be controlled by adjusting the pH of the
TPP aqueous solution, a pH of 8.6 was chosen in order to achieve a low crosslinking
density in the polymeric matrix (Mi et al, 1999; Shu & Zhu, 2001).
The macrospheres prepared from chitosan and from blends maintained their integrity (did
not dissolve or break apart) during the experiment. The calculated soluble fraction is
directly related to the selected polymeric composition and crosslinking time. The soluble
fractions are shown in Table 1.
A slight decrease in the soluble fraction was observed when the crosslinking time or the
chitosan content were increased. Bourtoom & Chinnan obtained similar experimental
results by preparing films made of rice starch-chitosan blends (Bourtoom & Chinnan,
2008). They reported a decrease in the soluble fraction with the augmentation of the CS wt
% that could be attributable to the interactions between both biopolymers. When the CS
percent or the crosslinking time (tc) are lowered, the ionic crosslinking between CS chains
decreases, and the interactions between biopolymers are affected, producing a larger
soluble fraction.
Table 1
EDS was used to analyze the phosphorus content on the external surface of the
macrospheres after 2 or 4 hours of cross-linking in order to obtain information about the
effectiveness of the crosslinking. An increase in the amount of phosphorus would confirm
an increase in the crosslinking density (Mi et al, 1999). The phosphorus wt % measured on
the external surface of different matrices is shown in Table 1. The semi-quantitative results
revealed that the content of phosphorus is highly dependent on the tc. The experimental
results are in agreement with the lower crosslinking degree achieved at the minimum tc
tested.
It is also observed that this phosphorus wt % decreased after incorporation of ST. This fact
could indicate that, in the case of matrices prepared from blends, the added ST is not
involved in the ionic crosslinking with TPP. Using a room temperature setting in the
preparation method of macrospheres eliminates the possibility of a crosslinking reaction
between ST and TPP, which only would occur at a high temperature (>100 ºC) (Deetae et al
2008; Lim. & Seib, 1993).
Figure 1 shows the morphology of dried samples prepared with chitosan or polymeric
blends with different crosslinking times. The bead diameters, regardless the crosslinking
time, are 3.70 ± 0.03 mm for chitosan beads and 3.00 ± 0.05 mm for matrices prepared with
blends. These sizes are optimal for a final agrochemical application.
Other general properties were observed, including the findings that none of the analyzed
macrospheres were completely spherical in shape and that the crosslinking time does not
significantly affect the final size. According to the experimental procedure, the main factor
that would affect the size of the beads is the diameter of the plastic tip used in the dripping
technique.
The micrographs of the surfaces of the cross-sectioned beads show many cavities of
different sizes. The presence of these cavities could be caused by the preparation method.
They could be the consequence of occluded air bubbles incorporated during the preparation
of the polymeric material used to manufacture the beads. The observed inner structure is
useful in the preparation of a controlled-release fertilizer because it would enhance the
loading of the fertilizer inside the polymeric matrix.
Figure 1
In accordance with previous reports (Mi et al, 1999; Shu & Zhu, 2001), the pH chosen for
the TPP solution used in this work is adequate because, due to the low crosslinking density
achieved, it produces porous structures.
Figure 2
The starch gelatinization causes exposure of the OH groups. It has been established that
these groups can form hydrogen bonds with the protonated amino groups of chitosan
(Mathew, Brahmakumar, & Abraham, 2006; Pelissari et al, 2009; Wang et al, 2007). These
interactions causes changes in the spectra corresponding to the chitosan/starch hydrogels, as
the amino group peak of chitosan shifted from 1657 to 1629 cm−1. These changes are
evidence of the good molecular compatibility between the biopolymers selected to produce
the macrospheres.
The FTIR spectra of matrices obtained from blends also revealed a shoulder at 1240 cm-1,
demonstrating the existence of the –P=O group and indicating that crosslinking took place
through ionic interactions between the negatively charged –P=O group and the NH3+ group
in chitosan.
Figure 3
XRD diffractograms of pure chitosan, pure starch and macrospheres prepared with chitosan
or blends are shown in Figure 4.
Starch is a semicrystalline polymer. Depending on the starch source, its crystallinity can
vary from 15 to 51 % (Foresti et al, 2014).
Potato starch showed typical crystalline peaks centered at 5.75, 16.85, 23.71, 24.16, 30.61
and 35.14°. It exhibited the characteristic ‘B’ type X-ray pattern of tuber starches
(Cheetham & Tao; 1998). Chitosan exhibited two crystalline and defined peaks at 10.55
and 19.7° (Qi et al, 2004). The peaks found in the CS100 diffractogram decreased slightly
when the ionic crosslinking time was increased. The crosslinking inhibits a close packing of
the polymer chains by reducing the degrees of freedom in the 3-D conformation, limiting or
even preventing the formation of crystalline regions (Qi & Xu, 2004).
The method used to obtain chitosan beads causes simultaneous deprotonation ionic
crosslinking of the chitosan chains. This process could produce deprotonated chains but not
crosslinked or mobile deprotonated chain segments between crosslinking points, which are
capable of a certain rearrangement that could explain the XRD diffractogram of chitosan
beads (Bhumkar & Pokharkar, 2006).
In the case of polymeric macrospheres prepared with blends, the XRD pattern showed a
decreased intensity of the characteristic peaks corresponding to chitosan and starch, which
is indicative of a degree of interaction between the molecular chains of both
polysaccharides (Xu et al, 2005).
As the starch/chitosan ratio increases, there are more OH groups from the starch polymeric
chains that are able to interact with chitosan’s protonated amino groups. This increased
interaction between biopolymers caused a shift of the chitosan diffraction peak from 10.55°
to a lower value and then its disappearance with increasing starch content (Figure 4 (e), (f)
and (g)) (Xu et al, 2005).
Figure 4
The thermogravimetric analysis (TGA) results from different samples are shown in Figure
5.
Figure 5
From the TGA results, is possible to appreciate three different stages. A first stage of
weight loss below and approximately 100 °C can be attributed to water evaporation.
Polysaccharides usually have a strong affinity for water and, therefore, may be easily
hydrated, resulting in macromolecules with rather disordered structures. The hydration
properties of these polysaccharides depend on their primary and supra-molecular structure
(Kittur et al, 2002). In our case, the matrices prepared exclusively with chitosan presented
the highest weight loss. The addition of starch caused a decrease in the ionic crosslinking
degree because of the lower chitosan concentration and also caused a decrease in the
amount of water lost compared to the results obtained from chitosan macrospheres. As a
result of the high hydrophilicity of starch, the water retention showed anomalous behavior
because it was found that the weight lost at 100 ºC was lower in macrospheres prepared
from blends. Water can act as a plasticizer for both biopolymers, but in the case of starch, it
can increase retrogradation with a consequent increase in crystallinity (Zhiqiang, Xiao Su,
& Yi, 1990). This phenomenon can generate a barrier effect that could prevent the loss of
water from the macrospheres obtained from blends.
There is a second stage of weight loss, observed between 240 and 340 ºC, that is due to the
depolymerization of chitosan and to the decomposition of starch for matrices prepared with
blends. This phenomenon can be ascribed to a complex process that includes the
dehydration of the saccharide rings and the depolymerization and decomposition of the
glucose units belonging to starch (Fang et al, 2002).
Finally, there is a third stage between 340 and 500 ºC caused by the pyrolysis of chitosan
and the vaporization and elimination of the volatile products of starch (Zawadzki &
Kaczmarek, 2010).
The results obtained from the derivative thermogravimetric analysis (dTGA) are shown in
Table 2.
Table 2
The dTGA curves showed that there are differences in the temperature associated with the
maximum mass loss rate (Tmax) for beads of different composition or prepared with
different crosslinking times. For macrospheres prepared with blends, the factor that mostly
affects the Tmax is the mass composition. The experimental Tmax is lower than the value
obtained by applying the mixture rule (He, Zhu, & Inoue, 2004). This observation points to
the existence of molecular interactions between the biopolymers used, which have already
been reported (Mi et al, 1999). Independent of the sample being analyzed, Tmax always
decreased with increasing crosslinking time. This fact could be related to the decrease in
crystallinity caused by the increase in ionic crosslinking (Mi et al, 1999). For blend
matrices, Tmax increased with the percentage of starch added, showing higher thermal
stability than the samples prepared exclusively with chitosan. This result could be attributed
to an increase in crystallinity, as already discussed for the XRD and TGA results.
The DSC curves are shown in Figure 6. All samples showed an endothermic transition
associated with water evaporation in the 50 - 150 °C range. Regarding the temperature peak
of the mentioned transition, increasing tc caused a shift to higher temperatures because
more energy was required to remove water from hydrogels with a greater degree of
crosslinking (Sarmento et al, 2006).
Figure 6
The chitosan content was a determining factor in the registered temperature shift of the
endothermic peak. As the chitosan content increased, the shift was more pronounced
because of the increase in the ionic interactions that affected the crystallinity of the
matrices, as already discussed with the TGA results. A peak corresponding to exothermic
decomposition (depolymerization) is observed for chitosan at 292.78 °C (Choi et al, 2007),
while for the crosslinked matrices, the same transition was observed at lower temperatures
but with lower intensity. Ionic crosslinking with TPP led to a decrease in crystallinity,
which led to lower thermal stability for chitosan macrospheres than for pure chitosan (Mi et
al, 1999, Lee et al, 2001). In the case of macrospheres prepared from blends, it was
observed that the temperature shift corresponding to the peak of the exothermic transition
was more pronounced than the one registered for crosslinked matrices prepared exclusively
with chitosan.
This result could be related to all the interactions occurring in the polymeric blend. By
increasing the starch content, the level of ionic crosslinking or the physical interactions via
hydrogen bonds between both biopolymers tends to decrease.
TGA and DSC results were indicative of the existence of ionic crosslinking and good
compatibility between chitosan and starch macromolecules.
Water absorption produces swelling of the tridimensional polymeric network. In the case of
beads loaded with potassium nitrate, this phenomenon has a key role in governing fertilizer
release (Huanbutta et al, 2011).
Due to the direct relationship between the swelling and the structure of the material,
modification of the crosslinking time and/or the polymeric composition of the beads could
be an interesting approach for regulating the release of the loaded fertilizer.
The swelling experiments indicated that none of the samples dissolved during the time
interval assayed and that all reached an equilibrium swelling capacity after 3 hours.
An increase in the crosslinking time induced a decrease of approximately 12 % in the
swelling degree of all matrices tested, regardless of its polymeric composition (Yalinca,
Yilmaz, & Bullici, 2012). This result could be explained by the increase in the ionic
interchain linkages (Mi et al, 1999).
In the case of macrospheres prepared using blends at equal tc, the swelling equilibrium
degree is lower than that of the chitosan beads, reaching a minimum when a 30 % wt/wt of
chitosan is used. The introduction of a certain amount of starch induces changes in the final
matrix structure associated with the ionic crosslinking density and with the intermolecular
interactions between both biopolymers. XRD, FTIR and TGA results indicate that
increasing the starch content affects the interactions within the tridimensional polymeric
network, producing a larger swelling degree accordingly to the results presented in Table 2.
Because of the loading method, a direct relationship between the swelling degree and the
loading capacity is expected (Samanta & Ray, 2014). The experimental maximum fertilizer
loading shown in Table 2 indicates that chitosan beads possessed a maximum loading
capacity in accordance with the higher equilibrium swelling degrees measured for these
matrices. Surprisingly, in the case of the beads prepared with both blends, the fertilizer
loading capacity was approximately the same. Further studies are being conducted in order
to understand this experimental result.
Figure 7
Conclusions
Acknowledgments
This work and the data herein contained was supported by Universidad de Buenos Aires,
Argentina (Grant 20020130200086BA UBACyT 2014-2017).
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Figure Captions
Figure 2. FTIR spectra of (a) chitosan, (b) CS100 with tc = 2 h, (c) CS100, tc = 4 h (d)
CS30/ST70 with tc = 2 h, (e) CS30/ST70 with tc = 4 h, (f) CS20/ST80 with tc = 2 h, (g)
CS20/ST80 with tc = 4 h and (h) ST
Figure 3. 13C CP-MAS NMR spectra of chitosan (a), CS100 with tc = 2 h (b) and CS100
with tc = 4 h (c).
Figure 4. X-ray diffractograms of starch (a), chitosan (b), CS100 with tc = 4 h (c), CS100
with tc = 2 h (d), CS30/ST70 with tc = 4 h (e), CS20/ST80 with tc = 4 h (f) and CS20/ST80
with tc = 2 h (g).
Figure 5. TGA curves of chitosan, starch, and CS100 with tc = 2 h, CS100 with tc = 4 h,
CS30/ST70 with tc = 2 h, CS30/ST70 with tc = 4 h, CS20/ST80 with tc = 2 h and
CS20/ST80 with tc = 4 h.
Figure 6. DSC thermograms of chitosan (a), starch (b), CS100 with tc = 2 h (c), CS100 with
tc = 4 h (d), CS30/ST70 with tc = 2 h (e), CS30/ST70 with tc = 4 h (f), CS20/ST80 with tc =
2 h (g) and CS20/ST80 with tc = 4 h (h).
Figure 7. Cumulative percent release of KNO3 as a function of time from matrices prepared
with a tc = 2 h.
Table 1. Soluble Fraction and EDS analysis of CS100, CS30/ST70 and CS20/ST80
prepared hydrogels by different tc.
2 7.2±0.2 3.4±0.3
CS100
4 6.5±0.3 5.3±0.4
2 10.9±0.4 2.0±0.2
CS30/ST70
4 7.5±0.5 2.7±0.3
2 11.2±0.5 1.4±0.2
CS20/ST80
4 9.5±0.4 2.4±0.3
tc
a) 85 X b) 25000 X c) Core 85 X
(h)
2
CS100
2
CS20/ST80
2
CS30/ST70