Yuntao Wangac,
Tingguo Liud,
Bakht Ramin Shahac,
Yan Liac and
Bin Li*abc
aCollege of Food Science and Technology, Huazhong Agricultural University, Wuhan 430070, Hubei, China. E-mail: libinfood@mail.hzau.edu.cn
bHubei Collaborative Innovation Centre for Industrial Fermentation, Hubei University of Technology, Wuhan 430068, China
cKey Laboratory of Environment Correlative Dietology (Huazhong Agricultural University), Ministry of Education, China
dProvincial-Level Experimental and Teaching Demonstration Center of Chemical Materials & Engineering, Chizhou University, Chizhou 247100, Anhui, People's Republic of China
First published on 9th October 2015
α-chitin cannot be dispersed directly with ultrasonic treatment because of the strong intermolecular forces. However, in the current work, when α-chitin was first regenerated from a NaOH/urea solvent, the regenerated α-chitin can then be easily dispersed with ultrasonic treatment under weak acidic conditions. The morphology, size, zeta potential, structure and optical transmittance of the dispersed α-chitin solution were characterized by TEM, DLS, XRD and UV spectroscopy respectively. The dispersed chitin was then used for stabilization of oil in water emulsion. It was found that the emulsifying capacity of regenerated chitin was tunable by ultrasonic treatment. The dispersed chitin exhibited excellent emulsifying ability and the resulting emulsion was stable after long-term storage. In short, in this paper, a novel way to prepare dispersed chitin with excellent emulsifying ability was presented, and its emulsifying properties were further evaluated.
Chitin is the second most abundant polymer on earth after cellulose and derived from food processing byproducts such as shrimp and crab shells.10 But the strong intermolecular forces make it difficult to dissolve in common solvents.11 Therefore, there is little research based on chitin in the past though its deacetylated product, chitosan has been given attention by scientists around the world. New green solvent developed by professor Zhang containing NaOH/urea provided a new option for the utilization of chitin and chitin materials based on this solvent is considered to be a hot scientific spot.12 However, as one kind of natural and eatable polymer with a wide range of functionalities such as immune modulator and anti-inflammatory agent,13 there is little research on this polymer as food ingredients. Though chitin nanocrystal, prepared by acid hydrolysis to remove the amorphous region, has been developed as a kind of emulsifier for stabilization of oil in water emulsion.3 The yield of chitin nanocrystal by this method is only 55% as the high temperature and strong acid condition destroyed most part of crystalline region at the same time, which lead to the decrease in yield.9 Usually, chitin nanofiber can be obtained by high pressure homogenization of chitin under weak acidic condition, but relatively more energy input is required for this method.11 Recently, chitin fiber was obtained through dissolution and regeneration from concentrated phosphoric acid,14 but large amount of phosphoric acid and long time were required to prepare chitin nanofiber. Hence improvement of these methods for the preparation of chitin derivatives with particular properties is necessary for efficient utilization of chitin.
Therefore, in this study, α-chitin was first dissolved and regenerated from a cost saving and green solvent containing NaOH/urea. Then the dispersed chitin was obtained through ultrasonic treatment of regenerated α-chitin under weak acidic condition. The yield of dispersed chitin in this process is as high as 90%. The structure and characteristics of the dispersed chitin were characterized. Then regenerated chitin containing crystalline region and amorphous region was researched as a new kind of emulsifier for stabilization of oil in water emulsion. It was found that the dispersed chitin exhibited excellent emulsifying ability and the emulsifying capacity of regenerated chitin can be adjusted with ultrasonic time. Moreover, the obtained emulsion was stable after long time storage. Therefore, the regenerated chitin obtained by this economic and eco-friendly method turned out to be a kind of highly efficient emulsifier.
The particle size (z-average diameter) and ζ-potential of the regenerated chitin were determined using the dynamic light scattering (DLS) technique (Malvern Instruments Ltd, Worcestershire, U.K.). Regenerated chitin (0.5 wt%) was shaken severely to be evenly dispersed before determination. All measurements were carried out at 25 °C in triplicate.
The crystallinity of the dispersed chitin after freeze drying was analyzed using wide-angle X-ray diffraction (WAXD). Measurements were conducted on a Siemens D5000 diffractometer (Germany) equipped with a Cu Kα radiation source (λ = 0.1542 nm). Scans were taken over the 2θ range from 5° to 30° at a scanning speed of 2° min−1. Crystallinity of the sample was determined by plotting the peak baseline on the diffractogram and calculating the area using the software (Jade6.0). The area above and under the curve referred to the crystalline domains and the amorphous regions, respectively. Ratio of upper area to total area was taken as the relative crystallinity: the crystallinity index (%) was calculated by the following equation
Crystallinity index (%) = area under the peaks/total curve area × 100.16 |
For Fourier transform infrared spectroscopy (FTIR) tests, regenerated chitin was grinded together with potassium bromide (weight ratio of 1:
50) and pressed into disks for scanning with a Nexus 470 spectrometer (Nicolet, USA). Samples were scanned at 4000–400 cm−1 with a resolution of 4 cm−1.
Optical transmittance of diluted chitin suspension (0.1 wt%) was measured with a Hach DR 2800 spectrophotometer (U.S.A.). Measurements were conducted for two times at wavelength ranging from 400 to 800 nm and the results were averaged.
The interfacial tension between the two phase (water and soybean oil) was measured using the Kruss K100 (Kruss, Germany) at 25 °C. The interfacial tension between the aqueous phase (pure water, regenerated chitin) and oil phase (soybean oil) was measured with the Wilhelmy plate method.17 Firstly, the Wilhelmy plate, made of platinum with a length, width and thickness of 19.9 mm, 10 mm and 0.2 mm, respectively was immersed in 20 g of aqueous phase to a depth of 3 mm under a surface detection speed of 15 mm min−1. Subsequently, 50 g of the oil was carefully pipetted over the aqueous phase to create an interface between the aqueous phase and oil phase. The test was conducted over 2500 s and the temperature was maintained at 25 °C throughout the test.
The morphological images of the O/W emulsion were captured by optical microscopy (Nikon 80i, Japan). A drop of emulsion was diluted with water on a microscopic slide and carefully covered with a cover slip. The size of the emulsion was determined at 25 °C with a Mastersizer APA2000 (Malvern, England). For each measurement, a given volume of emulsion was dropped in 1000 mL of distilled water with the concentration of 2–10% (v/v). Measurements were carried out for three times and the results were averaged. All tests were conducted at room temperature. Distilled water was used as the dispersion medium. The stirring rate was 600 rpm and the speed of circulation pump was 3000 rpm.
Rheological properties of the oil in water emulsion stabilized by regenerated chitin were performed at 25 °C using a controlled-stress AR2000ex rheometer (TA instrument Co. Ltd, UK) (diameter of 40 mm, gap height of 1000 mm). For the steady shear measurements, the shear rate was increased from 0.1 s−1 to 10 s−1, and the apparent viscosity (η) was recorded correspondingly. To obtain the linear viscoelastic region, oscillation strain sweep experiments were performed in the oscillation strain range from 0.01 to 10% (frequency, 1 Hz; temperature, 25 °C). For the dynamic oscillation measurements, the frequency sweep was conducted at 25 °C with frequency ranging from 1 to 10 Hz (all of the measurements were conducted within the linear viscoelastic region) and the elastic (G′) and loss (G′′) were recorded. All the determination were conducted on separate samples at least in duplicate.
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Scheme 1 Representation of conversion of α-chitin into regenerated chitin (RC) and depiction of conditions suitable for dispersion of RC in deionized water. |
From the TEM image of dispersed chitin in Fig. 1, it can be seen that the shape of dispersed chitin was irregular and the size of the dispersed chitin was not even. For the regenerated chitin after ultrasonic treatment for 60 min (RC60), smaller particles were in the majority, but there were still large particles. The average size of RC10, RC20, RC40 and RC60 were 1183 nm, 892 nm, 670.9 nm and 640.6 nm with a PDI of 0.253, 0.347, 0.368 and 0.305 respectively. The dispersed chitin became relatively smaller with increasing of ultrasonic time on the whole. This can be understood that more energy input breaks regenerated chitin into much smaller particles. XRD of dispersed chitin was shown in Fig. 2a. Compared with the original regenerated chitin, the peak of ultrasonically treated regenerated chitin at 2θ = 12.8°, 26.5° gradually became weaker with increasing of ultrasonic time, while other peaks at 2θ = 9.3°, 19.2° remained almost unchanged.12 Therefore, it can be easily inferred that the crystalline degree of chitin gradually decreased with increasing of ultrasonic time taking into the consideration that the crystalline degree can be obtained by calculating ratio of area for the crystallization peak and that of the total area.16 This indicated that the intermolecular hydrogen bonds of regenerated chitin were further broken, resulting in the damage of crystal structure during the ultrasonic process. Similar results were also found for the isolation of microfibrillated cellulose from sugarcane bagasse21 and prickly pear fruit peels22 with high pressure homogenization treatment. It can be seen from Fig. 2b that the FTIR spectra of the original regenerated α-chitin and the regenerated α-chitin ultrasonically treated for 60 min (RC60) are nearly identical, which means that the chemical structure of the chitin was not changed in the ultrasonic process.
The fact that high optical transmittance from dilute (0.1 wt%) chitin suspension (Fig. 3) were achieved at visible light wavelength ranging from 400 to 800 nm also confirmed the presence of small particles.23 Moreover, the transmittance gradually became higher with increasing of ultrasonic time, which further confirmed that smaller chitin particles were obtained after ultrasonic treatment for longer time, and this was consistent with TEM results. Additionally, these results also suggested that larger fractions were present since the transmission was not yet above 90%, and this can also be confirmed by TEM in Fig. 1.
Fig. 4b presented the interfacial tension between water and soybean oil as a function of regenerated chitin. It can be seen that the interfacial tension of all system decreased with increasing of time and the presence of chitin particles lowered the interfacial tension values between water and soybean oil significantly. Moreover, the interfacial tension values obtained at equilibrium state were lower for regenerated chitin ultrasonically treated for longer time, indicating that emulsifying ability of smaller particles will be superior. This can be explained that smaller particles are easier to be adsorbed to the oil–water interface with a much faster speed and the theoretical maximum adsorbed amount of particles for a close-packed monolayer in the oil–water interface will be larger if the particles are smaller,24 thus lowering the interfacial tension to a greater extent.
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Fig. 5 Typical optical micrographs and size distribution of emulsion stabilized with ultrasonically treated regenerated chitin (0.5 wt%). |
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Fig. 6 Micrographs and volume of the O/W emulsion stabilized with ultrasonically treated regenerated chitin (0.5 wt%) after storage for 30 days. |
pH has a strong effect on the surface charge and stability of colloidal particles, which will significantly affect the stability of emulsion. The influence of pH on the stability of emulsion was shown in Fig. 7, and it can be seen that the emulsion was stable in a wide range of pH from 3 to 9, indicating excellent pH stability. This further indicated that emulsion stabilized by insoluble polysaccharide can withstand extreme environment stress compared with that of other polymer particles such as protein.8 The emulsion volume is smaller and the emulsion size is larger in both the acidic and alkaline condition, while the emulsion was the most stable in neutral condition, with the smallest emulsion size and largest emulsion volume. The pK of chitin is reported to be around 6.3,3 so as the pH reached lower values, e.g. pH 3.0, or higher values e.g. pH 9.0, the chitin will be positively or negatively charged. The electrostatic repulsive forces at these pH levels and a low chitin concentration (0.5 wt%) would prevent the formation of a strong network. In contrast, when the pH of the dispersion is around 6.3, the repulsive electrostatic forces are minimized and the dispersed chitin could then easily aggregate and form a gel. This will further stabilize the emulsion towards creaming, which will result in better stability of the emulsion.
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Fig. 7 Volume and average size of the O/W emulsion prepared with RC20 (0.5 wt%) after storage for 30 days. |
The rheological properties of the Pickering emulsion were shown in Fig. 8. Pronounced shear-thinning behavior of the emulsion can be observed at shear rates higher than 0.1 s−1. In all cases, shear viscosity of emulsion was high at low shear rate, and then progressively decreased with increasing of shear rate. This phenomenon is a typical flow behavior of oil-in-water emulsion,26 which corresponds to the deflocculation of droplets upon shearing. But there was not obvious viscosity difference among emulsions stabilized by regenerated chitin treated for different time. Frequency sweep was conducted with a constant strain of 0.1%, which was within the linear viscoelastic region of emulsions. It was found that G′ was considerably higher than G′′ at any test frequency, indicating a predominantly elastic gel-like behavior.27 Furthermore, G′ and G′′ gradually increased with frequency, suggesting the gel-like network might be maintained through non-covalent physical cross-links in nature.28 Also there was not significant modulus difference between emulsions stabilized by regenerated chitin after different treatment. Similar observation was also reported in gel-like O/W emulsion stabilized by phytosterol colloidal particles26 and hydrophobic starch particles.25
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Fig. 8 (a) Shear-rate dependence of viscosity and (b) dynamic frequency sweep of O/W emulsions stabilized by ultrasonically treated regenerated chitin (0.5 wt%). |
This journal is © The Royal Society of Chemistry 2015 |