3.1 QPI particle size and zeta-potential as affected by US treatment and pH
Preliminary experiments showed that QPI without treatment cannot form stable emulsions due to large protein aggregate size (> 3 µm) and inferior surface properties [14, 16]. Therefore, the US treatment was employed to reduce the particle size of QPI suspension prior to preparation of emulsions [26]. As shown in Fig. 1A, sonication at 19.9 W for 25 min significantly reduced the z-average particle size of QPI suspension from ~ 3500 nm to ~ 300 nm. The particle size significantly decreased with US treatment time up to 5 min and then it nearly reached a plateau at 25 min. Therefore, the 25 min US treated QPI sample was selected for further studies. A significant reduction in particle size induced by US treatment has been widely reported in other plant protein suspensions. Zhang, Zuo [28] found that the particle size of QPI suspension was significantly decreased to ~ 132 nm at a sonication density of 10 kJ/mL. O'Sullivan, Murray [29] found that US treatment (power density 34 W·cm− 2) for 2 min could substantially decreased the particle size of pea protein isolate suspensions from ~ 5000 nm to ~ 200 nm. Various extents of decrease in particle sizes have been reported in previous studies, which could be related to the sample characteristics and sonication conditions. The size reduction of protein particles could be due to the breakdown of non-covalent bonds in protein large aggregates induced by extensive shear forces, micro-jetting, and turbulence generated by ultrasonic cavitations [26, 30].
The emulsification performance of food proteins is also strongly determined by the pH and surface charges as protein diffusion to the oil-water interface could be affected by these factors [21]. The effect of pH on zeta-potential (surface charges) and particle sizes of US treated QPI suspensions are shown in Fig. 1B and 1C, respectively. The absolute zeta potential values of QPI suspensions tend to approach to zero at the pH around 5 and significantly increased at pH 3 (~ 28 mV) and pH 7 and pH 9 (~ -33 mV). This finding is consistent with previous studies that the isoelectric point of QPI is around pH 4.5-5 [31, 32].
The sonicated QPI suspension at pH 5 shows the largest particle size (~ 1650 nm) followed by at pH 3 (~ 500 nm), indicating the aggregation of sonicated QPI at acidic pH. While at pH 7 and pH 9, the particle size of sonicated QPI remained ~ 300 nm. This observation agrees well with previous studies that proteins typically exhibit the largest particle size at or close to their isoelectric point due to weakened electrostatic repulsions between adjacent protein molecules [15, 26]. The low charge on the surface of protein molecules also promote protein aggregation through other non-covalent interactions including hydrophobic interactions, van der Waals and hydrogen bonding interactions [33]. The high absolute zeta-potential values of the QPI at pHs far away from the isoelectric point could be due to protein unfolding and exposure of highly charged amino acids [34].
3.2 Effect of pH and oil content on microstructural characteristics of QPI stabilised emulsions
The microstructural characteristics of QPI stabilised emulsions containing 20%, 40%, and 60% oil at various pHs were evaluated by CLSM and confocal micrographs are shown in Fig. 2 where the protein phase are shown in green and oil droplets appear in red. For all the samples, proteins indeed stabilised oil-water interfaces and large aggregate network of both oil droplets and protein particles can be observed. This indicates the robustness of utilizing ultrasonication to prepare O/W emulsions stabilised by sonicated QPI particles. The formation of aggregate network structure has been observed in previous studies of protein stabilised emulsions prepared by high intensity emulsification techniques such as ultrasonication and high pressure microfluidisation. Zhang, Luo [8] showed that the aggregated emulsion stabilised with milk protein concentration (MPC 70) can be formed by ultrasonication when the oil content ≥ 35%. In another study of formation of emulsions by ultrasonication, Li, Martin [2] demonstrated that stable aggregated emulsion gels can be formed by using various food and non-food particles such as bovine micellar casein and graphene oxide. Liu, Zhang [35] prepared gel-like emulsions stabilised by whey protein isolate (WPI) using microfluidisation at the oil content varied from 30–60%. The formation of aggregated emulsions could be due to interdroplets bridging and QPI void-filling effects, which can be observed in Fig. 2. It can be also found that the microstructure of emulsions is significantly affected by the pH of QPI suspension and the oil content. Protein interfacial layers seem thicker and the protein aggregates in the continue phase are larger at pH 3 and 5 than at pH 7 and 9. At pH 5 in particular, QPI tend to form large protein aggregates at the oil-water interface as well as in the continuous phase due to low solubilities close to the isoelectric point. At the same oil content, emulsions stabilised by the QPI at pH 5 showed the largest oil droplet size compared to other pHs, suggesting an inferior emulsification performance of QPI at or close to the isoelectric point. Similar observations had been found in previous studies of emulsions formed by commercial potato, rice and pea proteins at pH 3.5, 5, and 7 using a conventional rotor-stator type mixer (Ultraturrax) [36]. The severe aggregation of proteins close to the isoelectric point could prevent the exposure of buried hydrophobic groups, enhance protein-protein interactions, and make a slower diffusion of proteins to oil-water interfaces, impeding protein absorption and rearrangement at the interfaces [37, 38].
At all the pHs of QPI suspensions, oil droplet size showed a significant increase with an increase in the oil content. This could be due to the fact that at fixed QPI concentration (3 wt%), the QPI particles available for the stabilisation of oil-water interfaces decreased, resulting in the formation of large oil droplets. The similar observations have been made in emulsions stabilised by sorghum kafirin particles at the oil content varying from 30–70% [39] and emulsions stabilised by commercial potato, rice and pea proteins at the oil content varying from 10–40% [36]. In addition, as the oil content increased, oil droplets tend to become more closely packed. For QPI stabilised emulsions at pH 7 and 9 containing 60% oil, some oil droplets were even compressed and exhibited polyhedron-type shapes. This has been commonly observed in high internal phase emulsions (oil volume fraction ≥ 74%) stabilised by QPI particles [16] and soy proteins [40], for examples. However, it is worth noting that most of high internal phase emulsions were prepared using low intensity emulsification method such as ultraturrax. It has been suggested that the interdroplets bridging and colloidal particle void filling under extensive turbulence by ultrasonication could induce distortion and rearrangement of oil droplets thus leading to the compress packing of oil droplets with polyhedron-type shapes [2, 8]. This is confirmed by the TEM observation of QPI stabilised emulsions as shown in Fig. 3. TEM images showed that more extensive oil droplets aggregation at 60% oil than 20% oil. Furthermore, QPI particles formed a cluster-like network at the oil-water interface as well as in the continuous phase. The large protein aggregates (particularly at pH 5) were found on both oil-water interfaces and in the continuous phase. The distance between oil droplets seems to be smaller at pH 7 than at pH 3 and pH 5, indicating more closely and compressed packing of oil droplets that are in line with CSLM observations.
3.3 Effects of pH and oil content on oil droplet sizes of QPI stabilised emulsions
In order to further characterise emulsion structures and validate CLSM findings, droplet sizes were determined by static light scattering (SLS) and results are shown in Fig. 4. At the same oil content, oil droplets stabilised by QPI at pH 5 were the largest followed by at pH 3 and pH 7, while the oil droplets had the smallest size at pH 9. For example, for emulsions containing 20% oil, the oil droplet size was ~ 10 µm, ~ 5 µm, ~ 3.5 µm and ~ 2.5 µm for oil droplets stabilised by QPI at pH 5, pH 3, pH 7, and pH 9, respectively. At the same pH, the oil droplet size showed a substantial increase as the oil content increased. For example, for droplets stabilised by QPI at pH 7, the size of oil droplets increased from ~ 3.5 µm at 20% oil content to ~ 23 µm at 60% oil content. Overall, the oil droplet size determined by SLS agreed well with CLSM observations. The smaller oil droplet size found at pH 7 and pH 9 could be due to their high surface charges (absolute zeta-potential values), enhanced electrostatic repulsions and solubilities, leading to high molecular structural flexibility and emulsification capability [36]. In addition, the oil droplet size (D [4, 3]) of all emulsion samples was not considerably changed after storage for 21 days at 20°C (results not shown), indicating good stabilities of these emulsions.
3.4 Effects of pH and oil content on rheological properties of QPI stabilised emulsions
The highly aggregated nature of oil droplets and network formation may result in formation of gel-like emulsion or emulsion gels. Small deformation oscillatory rheology was used to study viscoelastic properties of all emulsion samples. The storage modulus (G´) and loss modulus (G″) as a function of frequency for emulsion samples are shown in Fig. 5 (left hand-side). As shown in frequency sweep results, all the samples displayed that the G´ was higher than G″ in the whole frequency range. Further, both G´ and G″ were only slightly dependent on frequency, indicating a typical solid-like gel behaviour for all samples [13, 41]. This was confirmed by a tube-inversion test (inset images in Fig. 5) that most of emulsion samples showed gel-like and self-supporting behaviour that can adhere to the bottom of the glass tubes after inversion. However, some samples such as oil droplets stabilised by QPI at pH 5 containing 20% and 40% oil, they flowed after tube inversion which could be due to weak gel strength. The flowability of emulsions is related to the movement of oil droplets against one another [2]. Therefore, the gel-like behaviour of the aggregated emulsion could be attributed to the network formation of oil droplet and protein particles, leading to the constrains of oil droplets movement in the network, which was revealed by CLSM and TEM observations (Fig. 2 and Fig. 3). To compare the gel strength among all the samples, the G´ at 1 Hz are plotted in Fig. 6A. At pH 5, pH 7 and pH 9, G´(1Hz) showed an increasing trend with an increase in oil content. For example, the G´(1Hz) of oil droplets stabilised at pH 5 substantially increased from ~ 90 Pa at 20% oil content to ~ 1150 Pa at 60% oil content. The greater gel strength found at a high oil content could be attributed to the tighter packing of oil droplets as observed in CLSM and TEM micrographs. This behaviour agrees well with previous rheological studies of kafirin particles stabilised emulsions with oil content varied from 30–70% [39].
However, the G´(1Hz) of emulsions at pH 3 firstly increased from ~ 350 Pa at 20% oil content to ~ 1600 Pa at 40% oil content and then decreased to ~ 1300 Pa at 60% oil content. As the phase inversion (O/W to W/O) was not observed, the decrease in G´(1Hz) at 60% oil at pH 3 could be due to inhomogeneities of samples and/or differences in protein aggregation at the oil-water interface and in the continuous phase. It has been suggested that the rheology of emulsion is not only related to the oil droplet size and interfacial layer structures but also depends on the excess protein particles remaining in the continuous phase [16, 42]. This is indeed reflected in the complex rheological properties of emulsions as affected by pH. At low oil contents (20% and 40% oil), oil droplets stabilised by QPI at pH 5 exhibited the lowest G´(1Hz) value compared to other pHs. This behaviour may have been caused by being close to the isoelectric point of the protein (pI ~ 4.5), which generates the formation of protein aggregates, thus inducing the loose packing of oil droplets with the largest oil droplet size at pH 5. This could be responsible for the lowest gel strength at low oil contents (20% and 40% oil contents). However, oil droplets tend to become tighter packings at all pHs when the oil content is 60%. Under this circumstance, the rheological property of emulsion seems to be dominated by the interactions and packing of oil droplets. Therefore, all the emulsion exhibited strong gel strength (i.e. G´(1Hz) > 1000 Pa) at 60% oil.
Large deformation rheological properties of all emulsion samples were studied by strain sweep measurements. G´ and G″ as a function of strain amplitude are demonstrated in Fig. 5 (right hand-side). For all the samples, both G´ and G″ were independent of strain amplitude at small strains, indicating a linear viscoelastic behaviour. This also indicated that 0.5% strain amplitude used for frequency sweeps measurements, was within the linear viscoelastic region (LVR). When the strain was increased, G´ decreased for all emulsion samples, suggesting a structural broken down and shear thinning behaviour. In terms of G″, most samples exhibited a monotonous decrease as the strain was increased. However, for the emulsion stabilised by QPI at pH 9 containing 20% oil, the G″ was first increased and then decreased with the increase in strain amplitude. The overshoot of G″ could be related to dissipation of deformation energy due to rearrangement of oil droplets before the final break down of emulsion structures [16, 43]. The similar behaviour was reported in large deformation rheological studies of concentrated emulsions stabilised by canola protein isolates [44] and multiwalled carbon nanotubes [43]. When the strain amplitude was further increased, the decrease of G″ was faster than G´, leading to a crossover of G´ and G″. The stress at which G´ = G″ occurred was defined as the breaking stress. Beyond this point, the G″ is greater than G´, suggesting the disintegration of gel network and samples became fluid-like [45]. To compare large deformation rheological properties among all emulsion samples, the breaking stress are plotted and shown in Fig. 6B. Overall, the breaking stress showed similar trends with pH and oil contents as G´(1Hz), indicating the large deformation rheology results agreed well with small deformation rheology findings.