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Article

The Thermodynamic and Gelation Properties of Ovalbumin and Lysozyme

College of Food Science, Northeast Agricultural University, Harbin 150030, China
*
Author to whom correspondence should be addressed.
Gels 2025, 11(6), 470; https://doi.org/10.3390/gels11060470
Submission received: 22 May 2025 / Revised: 16 June 2025 / Accepted: 17 June 2025 / Published: 19 June 2025
(This article belongs to the Special Issue Application of Composite Gel in Food Processing and Engineering)

Abstract

Ovalbumin (OVA) and lysozyme (LYZ) are the predominant globular proteins in egg white and play a crucial role in influencing thermal stability and colloidal behavior. In this study, the thermal and conformational stability of OVA and LYZ under various physicochemical conditions including pH (5–9), protein concentrations (5, 10, and 20%), heating rates (2.5, 5, and 10 °C/min), sugars (sucrose and glucose), and salts (NaCl, KCl, and CaCl2) was systematically investigated using differential scanning calorimetry (DSC), aiming to elucidate their behavior within colloidal and gel-forming systems. The denaturation temperatures (Td) of OVA and LYZ in water (5% w/v, 5 °C/min) were 80.22 °C and 77.46 °C, respectively. The Td of LYZ and OVA decreased with protein concentration, heating rate, and CaCl2. OVA thermal stability was improved with increasing pH, but the stability of LYZ was decreased. Sugars enhanced the thermal stability of OVA and LYZ. In contrast, NaCl and KCl increased OVA stability but reduced LYZ stability. LYZ exhibited nearly 100% reversibility during the second heating cycle in water. Sugars maintained reversibility at approximately 90% for LYZ. However, the presence of salts diminished the reversibility. In contrast, OVA was completely denatured in water and sugar and salt solutions.

1. Introduction

Hen egg white protein (EWP) is a highly excellent source of foods, which is widely used as a key ingredient in numerous food production processes, especially for its functional properties such as emulsification, foaming, and gelation [1,2,3]. In the industrial production of liquid egg whites, the heat pasteurization process is necessary. It serves to sterilize EWP by eliminating pathogenic bacteria and reducing spoilage bacteria (Salmonella and Escherichia coli) through high-temperature treatment. This is important for ensuring food safety and protecting human health [4,5,6]. However, egg white exhibits limited thermal stability, as it loses fluidity and forms aggregates around 60 °C. And protein aggregation is a common occurrence in egg white production due to its susceptibility to thermal sensitivity [7]. Aggregation is easily induced by external stresses including pH, mechanical vibrations, alkali treatment, pulsed electric fields, and particularly heat treatment [8,9,10,11]. Protein aggregation disrupts the physicochemical properties and functional characteristics of egg whites in food production [12]. During pasteurization egg white protein approaches denaturation, aggregation, and precipitation, which affect the quality of the egg product [7]. Therefore, it is crucial to regulate the thermal stability of egg whites during pasteurization and heat processing [13]. Improving the thermal stability of egg proteins can increase the temperature of heat pasteurization and provide significant benefits for egg manufacturing [14]. Extensive research has focused on the aggregation of egg white proteins, such as the crosslinking of disulfide bonds, and non-covalent hydrophobic and electrostatic interactions [15]. The dominant factors influencing protein aggregation and gel properties are the disulfide bonds and free sulfhydryl groups [12,15,16].
Sample environment including solution pH, ionic strength, and co-solvents, which could promote protein unfolding, enhance hydrophobic interactions, reduce ionic bonds, and disrupt disulfide bonds [17,18]. Egg white is a complex mixture of protein systems with extensive studies focusing on aggregation and gel formation [19]. Comprehensive research has been directed toward understanding the overall properties of the egg white system affected by factors such as salt, sugar, and pH. Consequently, elucidating the thermal properties of key egg white proteins is essential for improving egg product processing and quality control [19,20,21,22].
OVA is the major protein comprising approximately 54% of egg whites. It is a globular phosphoglycoprotein with a molecular mass of 42.8 kDa consisting of 386 amino acid residues containing one disulfide bond and four sulfhydryl groups [23]. OVA is the most important protein in the heat gel formation of egg white aggregation for sulfhydryl groups [24,25]. Lysozyme (LYZ) is approximately 3.4% of egg whites and consists of 129 amino acids with a molecular mass of 14.6 kDa. The tertiary structure is stabilized by four disulfide bonds and no sulfhydryl groups [26]. LYZ has a higher isoelectric point (pI = 10.7) compared to other white proteins, and LYZ is the only alkaline protein in egg white. At natural pH LYZ can bind with other egg white proteins, such as ovomucin, ovalbumin, and ovotransferrin [27]. Meanwhile the antibacterial activity of LYZ has widespread use as a preservative agent in the food industry [28].
OVA and LYZ are the primary factors to affect egg white aggregation and gel formation. Previous studies have demonstrated that OVA and LYZ spontaneously associate with other egg white proteins at extremely low ionic strength even at room temperature [28,29]. In recent years, research has increasingly focused on enhancing the thermal stability and reducing the aggregation of egg white through factors such as pH, salts, and novel technologies [30,31,32,33], and DSC has been used to study the thermal stability of whole egg white system [34,35]. Using specific salts and controlled pH conditions has successfully improved the thermal stability and aggregation behavior of egg white proteins, providing valuable insights for industrial applications. However, there is limited information on the use of differential scanning calorimetry (DSC) to explore the individual protein thermal properties of OVA and LYZ. This study aims to investigate the thermal properties of OVA and LYZ under various conditions, including pH, and the presence of sucrose, glucose, NaCl, KCl, and CaCl2 to improve liquid egg white production and explore the potential applications of OVA and LYZ in the food industry.

2. Results and Discussion

2.1. The Thermal Properties of OVA and LYZ

Figure 1 shows the DSC thermograms of OVA, LYZ, and the mixture sample in water. The thermograms of LYZ indicated a single peak and the Td at 77.46 °C. The denaturation peak onset was at 71.28 °C and ended at 83.03 °C with a peak width of 11.75 °C. During the second heating cycle, LYZ exhibited nearly 100% reversibility. The Td remained at 77.46 °C and a consistent enthalpy change (ΔH = 7.3 J/g). LYZ exhibited reversibility due to its four disulfide bonds and the absence of free sulfhydryl groups. Upon heating and cooling, the native disulfide linkages are able to reform without generating new bonds or inducing permanent conformational changes, thereby preserving the native tertiary structure [12]. These findings are consistent with previous studies on the thermal behavior of structurally constrained food proteins [36].
The OVA thermograms showed that there was a signal peak at 80.22 °C with denaturation onset at 73.95 °C and endset at 84.23 °C. The peak had a width of 10.28 °C and the enthalpy was 3.5 J/g. Following this, the sample was cooled and reheated for a second heating cycle, but the thermograms indicated no peak, and these results indicate that OVA has no thermal reversibility upon heating. OVA contains four free sulfhydryl groups and one disulfide bond in its structure [37]; when OVA was denatured the structure unfolded and free sulfhydryls formed new disulfide bonds. New disulfide bonds can induce structural changes in OVA, resulting in aggregation and irreversible denaturation [11,38]. This irreversible behavior highlights the propensity of OVA to form thermally induced aggregates and gel networks through disulfide-mediated crosslinking.
Previous research has shown that the structure of egg white proteins can be altered at relatively low temperatures, leading to protein unfolding and the exposure of hydrophobic regions and thiol groups [39]. These structural changes result mainly from the disruption of intramolecular disulfide bonds, exposure of free sulfhydryl groups, and enhancement of hydrophobic interactions, all contributing to irreversible denaturation and aggregation [1]. In the mixed protein system, the thermal stability decreased in the mixed sample. This destabilization may be attributed to the initial unfolding of LYZ, which exposes reactive sites that can interact with unfolded regions of OVA, thereby accelerating OVA’s thermal denaturation [36]. As the protein structure unfolds the exposure of inner hydrophobic and thiol groups increases. These exposed hydrophobic regions and thiol-disulfide interactions drive the unfolding and aggregation of the protein structure [40,41]. Molecular interactions promote protein–protein crosslinking, leading to aggregation and the formation of heat-induced gel-like structures.

2.2. Effect of the Heating Rate

The temperature of denaturation (Td), onset, endset, and reversibility degree (Rd) of OVA and LYZ at different heating rates (2.5, 5.0, and 10.0 °C/min) are presented in Table 1. The heating rate significantly affected the Td of OVA (p < 0.05). The Td of OVA significantly increased with the heating rate (p < 0.05), ranging from 78.06 °C to 81.59 °C. However, the enthalpy change (ΔH 3.5–3.7 J/g) remained relatively constant across different heating rates. The reversibility of OVA after the second heating cycle was 0%, indicating irreversible denaturation.
The LYZ thermal stability decreased with the heating rate; LYZ exhibited the highest Td (77.79 °C) at 10.0 °C/min and the lowest Td (77.12 °C) at a heating rate of 2.5 °C/min. The ΔH of LYZ was slightly altered and ranged from 7.0 to 7.3 J/g. In the second heating cycle the reversibility of LYZ was nearly 100% at all three heating rates. The enthalpy and reversibility of LYZ are less affected by the heating rate. From a kinetic perspective, slower heating rates allow more time for molecular rearrangement, potentially enhancing protein unfolding and dissociation, which may slightly influence the apparent Td values [42,43].
These results indicated that the OVA and LYZ denaturation and thermal aggregation were influenced by heating time. Protein denaturation and aggregation are time-dependent processes that involve protein–protein associations [44]. When protein is heated for extended periods, the protein secondary structure becomes more susceptible to change at lower temperatures [45]. These results eventually lead to a decrease in protein denaturation temperature and aggregation [46]. The heating rate has less effect on the protein denaturation process, so the ΔH and protein reversibility were less affected. In contrast, OVA showed a significant increase in Td (p < 0.05) due to there being four free sulfhydryl groups in the OVA structure. Free sulfhydryl groups may form new disulfide bonds upon heating, inducing structural changes that result in an elevated Td with an increasing heating rate.

2.3. Effect of Protein Concentration on the Thermal Properties

The thermal properties of OVA and LYZ in different protein concentrations are shown in Table 2. The thermal stability of OVA was decreased in higher protein concentrations. The Td of OVA in the protein concentration 200 mg/mL, 10 mg/mL, and 5 mg/mL was 79.93 °C, 80.05 °C, and 80.22 °C. The enthalpy had a less significant effect on protein concentration and the enthalpy at 50 mg/mL and 200 mg/mL was 2.2 J/g and 1.3 J/g, respectively. The Td of LYZ was 74.53 °C, 76.54 °C, and 77.42 °C at protein concentrations of 20%, 10%, and 5%. These values all significantly (p < 0.05) increase with decreasing protein concentration. The results indicated that protein concentration could influence the thermal stability of OVA and LYZ [47].
The protein concentration can affect OVA and LYZ heat-induced aggregation. Higher protein concentration samples during heat treatment can aggregate and denature easily [46]. This is because the protein concentration can affect protein reaction with the concentration increasing the reaction of protein, and the results show that protein has less thermal stability with protein concentration increasing [43].

2.4. Effect of pH on the Thermal Properties

As shown in Figure 2, the thermal properties of OVA and LYZ were significantly affected by pH (5.0–9.0). The Td and ΔH increased significantly with pH increasing (p < 0.05), with Td ranging from 80.26 °C to 83.73 °C and ΔH from 2.6 to 4.3 J/g. However, OVA showed no thermal reversibility with pH. This enhanced thermal stability at higher pH may be due to increased electrostatic repulsion and structural rigidity as the pH moves away from OVA’s isoelectric point (pI ≈ 4.5), reducing the tendency for aggregation and unfolding. In contrast, LYZ exhibited decreasing thermal stability with increasing pH. Its Td decreased from 77.89 °C at pH 5.0 to 71.62 °C at pH 9.0, and ΔH ranged from 6.6 to 11.1 J/g. Reversibility also dropped dramatically from 100% at pH 5.0 to 1.2% at pH 9.0. This suggests that LYZ undergoes irreversible conformational changes at alkaline pH, likely due to disrupted hydrogen bonding and altered charge distribution, consistent with previous findings [48,49].
pH is an important factor effect protein thermal properties. When the solution pH is close to pI, the net charge of the protein is at a minimum and the protein cooperativity is at a maximum [45]. Therefore, OVA and LYZ have the lowest Td and enthalpy at the pH close to pI. Concurrently, the reversibility rate of LYZ diminishes progressively with the pH. pH affects LYZ net charge, secondary structure, and reversibility rate, and these results are in agreement with previous research that forms irreversible aggregation heated around 80 °C in higher pH [50]. LYZ is a basic protein (pI 10.7), so LYZ tends to associate electrostatically with other acidic proteins [28,51,52].

2.5. Effect of Sugars on the Thermal Properties

Figure 3 shows the Td and ΔH of OVA and LYZ in glucose and sucrose solutions at concentrations ranging from 0.05 to 0.5 M. Compared to the control (water), LYZ and OVA exhibited significantly higher Td and ΔH values in the presence of sugars. The Td of LYZ increased to 79.61 °C in glucose and 80.08 °C in sucrose. At 0.5 M concentration, ΔH increased by 27.45% and 11.39% in the glucose and sucrose solutions, respectively, indicating enhanced thermal stability. Sugars may also form hydrogen bonds with the protein surface, thereby enhancing structural integrity during heating. LYZ exhibited high thermal reversibility in both sugar solutions, with values ranging from 89 to 92% in glucose and 90–93% in sucrose, regardless of sugar concentration.
These results showed that sucrose had a significant increase in the thermal stability of OVA and LYZ than glucose, and the results were concentration-dependent. The values are all significantly (p < 0.05) higher than the control sample which was absent of sugar. The stabilizing effect of sucrose and glucose for LYZ was higher than OVA [53,54]. The presence of sugars can influence the entropy release associated with the protein–sugar state, as increased hydrogen bonding contributes to greater structural stability. The observed decrease in ΔH is due to the preferential exclusion mechanism of sugar. In this mechanism the protein has less protein conformational stability and decreases the protein flexibility and molecular interactions during protein denaturation, resulting in the protein having higher Td and lower ΔH in sugar solution [55,56].
Sugars can improve the thermal stability of LYZ and OVA. At the same concentration, the effect of disaccharides on protein thermal stability was greater than monosaccharides. Sugars can affect the entropy release of the protein–sugar state by enhancing hydrogen bonding, which stabilizes the structure. The observed reduction in ΔH may result from the preferential exclusion mechanism, where sugars are excluded from the protein surface. This exclusion limits conformational flexibility and weakens intramolecular interactions during denaturation, leading to a higher Td and lower ΔH in sugar solutions. Sugar molecules were preferentially or weakly excluded from the protein surface and preserved the native protein hydration shell [57]. The cohesive force increased as sugar concentration increased, which increased the energy required for cavity formation for the associated structures in the solvent [58,59].

2.6. Effect of Salts on the Thermal Properties

2.6.1. Effect of Salts on Thermal Properties of OVA

Ions can influence the net charge, hydration shell, and electrostatic interactions of proteins, thereby affecting their structure and thermal stability [60]. As shown in Figure 4, the thermal behavior of OVA was evaluated in the presence of different concentrations (0.25–1.0 M) of NaCl, KCl, and CaCl2. In comparison to the sample absent of salt, the thermal stability of OVA had a significant improvement in NaCl and KCl solution (1.0 M) with the Td being 84.09 °C and 83.96 °C. However, in the CaCl2 solution, the stability of OVA had a significant decrease and Td was reduced to 76.70 °C. When the samples were reheated, there was no reversibility in the second cycle. In comparison to the absent CaCl2, the ΔH of OVA decreased by 42% in 1.0 M CaCl2.
NaCl and KCl have a stabilizing effect on the thermal stability of OVA which was concentration-depended. The enthalpy of OVA was decreased by about 29.5% and 24.3% in 1.0 M NaCl and KCl solution. NaCl and KCl can change electrostatic interactions between protein molecules by altering surface charge. Additionally, salts may enhance hydrophobic interactions among proteins, thereby influencing their structural stability [61].
The thermal stability of OVA increased with rising concentrations of NaCl and KCl, as Na+ and K+ ions can alter the net surface charge of the protein and change intermolecular interactions. Less stable regions within the protein fold may act as nucleation sites for further unfolding under thermal stress [62]. In contrast, CaCl2 can form calcium bridges with the protein, leading to structural alterations. As a result, CaCl2 exerts a stronger destabilizing effect on protein conformation and thermal stability [63]. Cations with high charge density tightly bind water molecules in a structured hydration shell that limits their ability to form strong hydrogen bonds with the surrounding water. Under these conditions, anion-specific effects become more pronounced, as anions compete for the limited hydrogen-bonding sites available on the remaining unbound water molecules at the hydration shell interface [64].
When OVA was reheated in the NaCl and KCl solutions, the reversibility of OVA was 0%. The salt solution could increase the thermal stability and affect the denaturation mechanism. During the protein denaturing process the free thiol interchanges with disulfide, forming new disulfide bonds [65]. Salt can stabilize egg white thermal properties and combining it with sugar can have a synergistic effect on keeping the denatured protein in solution [14,54].

2.6.2. Effect of Salts on Thermal Properties of LYZ

Figure 5 shows the DSC results of LYZ heated in NaCl, KCl, and CaCl2 solutions at different salt concentrations. The Td of LYZ significantly decreased as the salts concentration. In comparison with the salt-free sample (77.46 °C), the Td of LYZ decreased to 73.92 °C (1.0 M NaCl), 74.23 °C (1.0 M KCl), and 68.89 °C (1.0 M CaCl2) when the salt solution concentration reached 1.0 M. In salt solution, the enthalpy of LYZ decreases with salt concentration, the decreasing trend and value are relatively consistent. The enthalpy of LYZ ranged from 6.2 to 6.4 J/g in 1.0 M solution of three salts. There was a significant effect on the thermodynamic negative stability and the enthalpy decreased with salt concentration.
These results indicate that KCl, NaCl, and CaCl2 have a significant impact on the thermal stability of LYZ in salt solutions, and the thermal destabilization is observed with the order Ca2+ > K+ > Na+. The result is in agreement with previous research [66]. And the order of the effect on LYZ is opposite to the traditional Hofmeister series [67,68].
Salts can affect the thermal stability, Td, ΔH, and reversibility degree of OVA and LYZ, as cations can alter protein electrostatic interactions by changing the net charge on the protein surface. In high-concentration salt solutions, the net surface charge is reduced, resulting in weakened electrostatic interactions between macromolecules and the suppression of coacervation. In high salt solutions, cations can influence surface charge density serving as nucleation centers for further protein unfolding due to their inherent instability within the folded structure [69]. In the second heating cycle, the reversibility of LYZ was decreased with salt concentration, and the reversibility of LYZ was decreased with salt concentration. The reversibility of LYZ in three salt solutions (0.25 M) was about 90%. When the salts concentration increased to 1.0 M, the reversibility was decreased to 19.41% in NaCl (1.0 M), 35.85% in KCl (1.0 M), and 75.39% in CaCl2 (1.0 M).
All salts exhibited a similar trend in reducing the reversibility of LYZ; however, CaCl2 resulted in a higher degree of LYZ reversibility compared to NaCl and KCl. The observed trend followed the order Ca2+ > K+ > Na+, consistent with the Hofmeister series. Salts have a similar effect on reducing LYZ reversibility, but CaCl2 showed higher values of LYZ reversibility than NaCl and KCl. And the following trend appeared as Ca2+ > K+ > Na+ which follows the Hofmeister series, and cation can affect the charge on the protein surface charge and affect the protein–protein encounters and denature to decrease the reversibility of LYZ. In the solution, the presence of cation can increase the energy barrier for association and effectively screen charge interactions in the unfolded state, and this results in a reduction in the thermal reversibility of OVA and LYZ [70].

2.7. Structural Characteristics of OVA and LYZ

The secondary structural changes in OVA and LYZ are shown in Figure 6. OVA exhibited two negative peaks at approximately 208 and 222 nm and a positive peak at 190 nm, indicating the presence of α-helical structures. Additionally, a positive band around 195 nm and a negative band at 218 nm were also observed, which are indicative of β-sheet structures [71]. When OVA was denatured the value of peaks was decreased, which means that the OVA had lost the protein secondary structure. Figure 6A,B indicate that OVA at different concentrations affects protein structural changes upon heating, as evidenced by the decreased absorption peaks at 190, 208, and 222 nm in the circular dichroism (CD) spectra. The results showed protein denaturation and conformational change after heating. With increasing protein concentration the α-helical content decreased and the random structure showed an increasing trend. In contrast, the secondary structure of LYZ remained relatively stable, with protein concentration having minimal impact on the protein secondary structure after heating [72,73].
The CD spectra of salt solutions (NaCl, KCl, and CaCl2) and water were similar; however, in the sugar solution (sucrose and glucose), the curve was more similar to that of the unheated sample, suggesting that sugar can protect the OVA structure better. In sugar solution the protein exhibited more α-helical and less random structure. The LYZ CD spectra showed two negative peaks at approximately 208 and 220 nm, and on the side had positive peaks at around 190 and 240 nm [74]. The similarity of these curves suggests that LYZ possesses excellent thermal stability and reversibility. In sugar solution the peak value was increased at the α-helical and β-sheet structures indicating that LYZ has enhanced thermal stability in the sugar solution. In contrast salts (NaCl, KCl, and CaCl2) decreased the content of α-helical and increased the random structure and this result shows that the salts cannot stabilize the secondary structure [75]. This result is consistent with the DSC results, which showed that sugars help stabilize α-helical and β-sheet structures, thereby enhancing protein thermal stability.

3. Conclusions

This study systematically elucidates the effects of pH, salts, sugars, heating rate, and protein concentration on the thermal properties of OVA and LYZ. The results demonstrate that pH modulates the thermal stability of OVA and LYZ differently. Increased protein concentration and slower heating rates were associated with reduced thermal stability, suggesting enhanced molecular interactions and aggregation under these conditions. Sugars (monosaccharides and disaccharides) significantly improved the thermal stability of proteins in a concentration-dependent factor, providing insights into their protective roles in heat processing. Regarding ionic effects, Na+ and K+ ions markedly increased OVA thermal stability, whereas Ca2+ decreased it due to calcium-induced structural alterations and possible bridging effects. LYZ exhibited reduced Td in all the salt solutions, with a clear concentration-dependent decline in reversibility ranging from 20% to 90%. OVA displayed complete and irreversible denaturation across all the tested conditions, regardless of pH, salts, and sugars. These results show extensive secondary structural loss, sulfhydryl-disulfide exchange, and hydrophobic interactions, supporting the notion that OVA has a strong propensity for heat-induced aggregation and network formation, positioning it as a promising gel-forming protein. LYZ retained a higher degree of structural integrity and reversibility following thermal treatment, indicating limited capacity to participate in heat-induced gelation. These results of OVA and LYZ offer valuable theoretical support for the rational design and optimization of protein-based gel systems in food and colloidal applications.

4. Materials and Methods

4.1. Materials

Ovalbumin (product A5503 approximately 98% purity as per manufacturer) and lysozyme (product L6876 approximately 90% purity as per manufacturer) of hen white protein obtained from Sigma-Aldrich Co. (St. Louis, MO, USA) were used. Sugars, NaCl, KCl, and CaCl2 were from Titan Technology Co., Ltd. (Tianjin, China). All the reagents were of analytical grade.

4.2. Sample Preparation

Solutions containing OVA and LYZ were prepared by dissolving the proteins in H2O to achieve a concentration of 50 mg/mL. Preliminary experiments demonstrated that a concentration of 50 mg/mL for each protein was necessary to achieve satisfactory DSC sensitivity. The samples underwent gentle agitation and aliquots (10 μL) of the solutions were subsequently transferred into DSC pans for analysis.

4.2.1. Effect of pH

The OVA and LYZ were prepared in 0.1 mol/L phosphate buffers ranging from pH 5 to pH 9 and the protein concentration was 50 mg/mL, pH was adjustment with NaOH (1 mol/L) and HCl (1 mol/L) was determined according to the method of Alli [36]. The phosphate buffers were prepared with Na2HPO4 and NaH2PO4 as reagents.

4.2.2. Effect of Salts

To investigate the effect of Na+, K+, and Ca2+ on the thermal properties of OVA and LYZ, OVA and LYZ were dissolved in solutions of NaCl, KCl, and CaCl2 with pH ranging from 7.0 to 7.1 and different concentrations (0.25, 0.50, 0.75, and 1.0 M), the final protein concentration was 50 mg/mL.

4.2.3. Effect of Sugars

To investigate the effect of sugars on the thermal properties of OVA and LYZ, OVA and LYZ were dissolved in sucrose and glucose solutions with concentrations 0.05, 0.1, 0.25, and 0.5 M, the final protein concentration was 50 mg/mL.

4.2.4. Effect of Heating Rate

To investigate the effect of heating rate on the thermal properties OVA and LYZ were dissolved separately in water (pH 7.0) at a concentration of 50 mg/mL. The samples were heated at different heating rates (2.5, 5.0, and 10.0 °C/min), respectively.

4.2.5. Effect of Protein Concentration

The method to investigate the effect of different protein concentrations was determined according to the method of Alli [36]: OVA and LYZ were dissolved in water at concentrations of 50 mg/mL, 100 mg/mL, and 200 mg/mL, respectively. And then samples were heated at a heating rate of 5.0 °C/min.

4.2.6. Differential Scanning Calorimetry (DSC)

All samples were heat-treated and analyzed by DSC (STARe SYSTEM, METTLER TOLEDO, Greifensee, Switzerland). Each sample was heated from 25 to 100 °C at a heating rate of 5 °C/min. The peak temperature of protein denaturation (Td) and heat of transition of enthalpy (ΔH) (area underneath peak) were calculated from each thermal graph. After heating, the samples were cooled to 25 °C in DSC and reheated the second cycle under the same conditions. The reversibility rate of OVA and LYZ was determined from the ratio of the first and second endothermal peaks [76]. All DSC sample experiments were performed in triplicate.

4.2.7. Circular Dichroism Spectrum

Circular dichroism (CD) spectra were taken using a chirascan (V100) spectropolarimeter (Applied Photophysics Ltd., Surrey, UK). The circular dichroism spectra of the OVA and LYZ samples (50 mg/mL) in water and different salt (NaCl, KCl, and CaCl2) and sugar (glucose and sucrose) solutions were collected at the 0.1 mol/L concentration. The samples were recorded at 25 °C in the range from 190 to 250 nm with a spectral resolution of 0.1 nm, and the protein concentration was 0.2 mg/mL. The scan speed was 100 nm/s and the response time was 0.125 s with the bandwidth of 1 nm. Quartz cells with an optical path of 0.1 cm were used. Typically, 16 scans were accumulated and subsequently averaged. A total of three spectra were accumulated and averaged.

4.2.8. Statistical Analysis

All the experiments were performed in triplicate. The data were analyzed using a One-Way Analysis of Variance (ANOVA) test, and the means were compared using Fisher’s least significant difference test (p < 0.05).

Author Contributions

Methodology, S.F. and M.Q.; Software, L.W. and S.L.; Formal analysis, R.L.; Data curation, Y.L.; Writing—original draft, L.W. and R.L.; Writing—review & editing, Y.C.; Visualization, J.Z. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. DSC thermograms of OVA, LYZ, and mixture: A. LYZ first cycle (5% w/v), B. LYZ second cycle (5% w/v), C. OVA first cycle (5% w/v), D. OVA second cycle (5% w/v), E. OVA+LYZ first cycle (10% w/v), and F. OVA+LYZ second cycle (10% w/v).
Figure 1. DSC thermograms of OVA, LYZ, and mixture: A. LYZ first cycle (5% w/v), B. LYZ second cycle (5% w/v), C. OVA first cycle (5% w/v), D. OVA second cycle (5% w/v), E. OVA+LYZ first cycle (10% w/v), and F. OVA+LYZ second cycle (10% w/v).
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Figure 2. The effect of pH on the thermal properties of OVA and LYZ: (A). The effect of pH on OVA. (B). The effect of pH on LZY.
Figure 2. The effect of pH on the thermal properties of OVA and LYZ: (A). The effect of pH on OVA. (B). The effect of pH on LZY.
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Figure 3. The effect of sugar concentration on the thermal properties of OVA and LYZ: (A). The effect of glucose concentration on OVA. (B). The effect of sucrose concentration on OVA. (C). The effect of glucose concentration on LYZ. (D). The effect of sucrose concentration on LYZ.
Figure 3. The effect of sugar concentration on the thermal properties of OVA and LYZ: (A). The effect of glucose concentration on OVA. (B). The effect of sucrose concentration on OVA. (C). The effect of glucose concentration on LYZ. (D). The effect of sucrose concentration on LYZ.
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Figure 4. The effect of (A) NaCl, (B) KCl, and (C) CaCl2 concentration on the thermal properties of OVA.
Figure 4. The effect of (A) NaCl, (B) KCl, and (C) CaCl2 concentration on the thermal properties of OVA.
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Figure 5. The effect of (A) NaCl, (B) KCl, and (C) CaCl2 concentration on the thermal properties of LYZ.
Figure 5. The effect of (A) NaCl, (B) KCl, and (C) CaCl2 concentration on the thermal properties of LYZ.
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Figure 6. The influence of the salts, sugars, and protein concentration on the secondary structure from CD analysis: (A) The effect of concentration on OVA, (B) the effect of concentration on OVA, (C) the effect of salt and sugars on OVA, and (D) the effect of salt and sugars on LYZ.
Figure 6. The influence of the salts, sugars, and protein concentration on the secondary structure from CD analysis: (A) The effect of concentration on OVA, (B) the effect of concentration on OVA, (C) the effect of salt and sugars on OVA, and (D) the effect of salt and sugars on LYZ.
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Table 1. The effect of heating rate on the thermal properties of OVA and LYZ.
Table 1. The effect of heating rate on the thermal properties of OVA and LYZ.
Rate
(°C/min)
OVA LYZ
Onset (°C)Td (°C)Endset (°C)ΔH (J/g)Rd (%)Onset (°C)Td (°C)Endset (°C)ΔH (J/g)Rd (%)
2.575.06 ± 0.15 a78.06 ± 0.19 a81.39 ± 0.21 a3.5 ± 0.2 a066.65 ± 0.13 a76.18 ± 0.12 a79.60 ± 0.16 a7.0 ± 0.1 a100
575.68 ± 0.17 b80.22 ± 0.11 b84.38 ± 0.15 b3.5 ± 0.1 b071.50 ± 0.18 b77.46 ± 0.05 b82.45 ± 0.04 b7.3 ± 0.1 b100
1077.13 ± 0.18 c81.59 ± 0.19 c85.51 ± 0.17 c3.7 ± 0.1 b071.55 ± 0.11 b77.68 ± 0.12 c83.40 ± 0.13 c7.4 ± 0.1 b100
Different small letters in the same column indicate that values are significantly different (p < 0.05).
Table 2. The effect of protein concentration on the thermal properties of OVA and LYZ.
Table 2. The effect of protein concentration on the thermal properties of OVA and LYZ.
Protein
mg/mL
OVA LYZ
Onset (°C)Td (°C)Endset (°C)ΔH (J/g)Rd (%)Onset (°C)Td (°C)Endset (°C)ΔH (J/g)Rd (%)
5075.68 ± 0.17 a80.22 ± 0.11 a84.38 ± 0.15 a3.5 ± 0.1 a071.50 ± 0.18 a77.46 ± 0.05 a82.45 ± 0.04 a7.3 ± 0.1 a100
10074.06 ± 0.12 b80.05 ± 0.03 b83.73 ± 0.13 b3.2 ± 0.1 b070.55 ± 0.22 b76.51 ± 0.07 b81.97 ± 0.11 b7.2 ± 0.1 a100
20073.63 ± 0.11 c79.93 ± 0.06 b83.57 ± 0.03 c3.0 ± 0.1 c068.93 ± 0.16 c74.53 ± 0.03 c79.90 ± 0.13 c7.1 ± 0.1 a100
Different small letters in the same column indicate that values are significantly different (p < 0.05).
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Wang, L.; Li, R.; Lv, S.; Liu, Y.; Fang, S.; Zang, J.; Qing, M.; Chi, Y. The Thermodynamic and Gelation Properties of Ovalbumin and Lysozyme. Gels 2025, 11, 470. https://doi.org/10.3390/gels11060470

AMA Style

Wang L, Li R, Lv S, Liu Y, Fang S, Zang J, Qing M, Chi Y. The Thermodynamic and Gelation Properties of Ovalbumin and Lysozyme. Gels. 2025; 11(6):470. https://doi.org/10.3390/gels11060470

Chicago/Turabian Style

Wang, Lifeng, Rongcheng Li, Siyi Lv, Yulin Liu, Shuaifu Fang, Jingnan Zang, Mingmin Qing, and Yujie Chi. 2025. "The Thermodynamic and Gelation Properties of Ovalbumin and Lysozyme" Gels 11, no. 6: 470. https://doi.org/10.3390/gels11060470

APA Style

Wang, L., Li, R., Lv, S., Liu, Y., Fang, S., Zang, J., Qing, M., & Chi, Y. (2025). The Thermodynamic and Gelation Properties of Ovalbumin and Lysozyme. Gels, 11(6), 470. https://doi.org/10.3390/gels11060470

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