Elizângela Hafemann Fragalab,
Lorenzo Metillib,
Frédéric Pignonb and
Sami Halila
*a
aUniv. Grenoble Alpes, CNRS, CERMAV, 38000 Grenoble, France. E-mail: sami.halila@cermav.cnrs.fr
bUniv. Grenoble Alpes, CNRS, Grenoble INP (Institute of Engineering Univ. Grenoble Alpes), LRP, 38000 Grenoble, France
First published on 29th January 2025
Supramolecular oleogels, in which low-molecular weight oleogelators self-assemble into various nanostructures through non-covalent interactions, have witnessed increasing research activity in various fields of science, including food, cosmetics or remediation of marine oil spills. Herein, we report a simple scalable and environmentally friendly carbohydrate-based oleogelator, namely, the sodium salt of N,N′-dimethyl β-C glucosyl barbiturate (GlcBMe) that self-assembles through sonication to induce the gelation of polar organic solvent and later of non-polar vegetable oils by cationic exchange with quaternary ammonium surfactants. Water-soluble GlcBMe was capable of forming self-assembled fibrillar network bridging insoluble particles in the oil by sonication in the presence of a small amount of water. The rheological properties are reinforced by in situ particle bridging with quaternary ammonium surfactants as evidenced by multi-scale structural analyses. IR analysis indicated that –OH (from carbohydrates) and –CO (from barbituric ring) were involved in hydrogen bonding promoting the formation of a fibrous network. The oleogel presented a non-Newtonian system showing a shear-thinning behavior and thixotropic properties. Advantageously, these oleogels showed excellent control and slow release of the loaded-vitamin E in a pH-dependent manner.
Therefore, reducing the molecular weight to obtain LMOGs that could jellify fatty phases in a cold process is of great interest. The range of structures known to be LMOGs is plentiful and multifarious – from n-alkanes, waxes, lecithin, 12-hydroxystearic acid to more complex synthetic ones (sorbitan stearate (Span® 60), 1,3:
2,4-di-O-benzylidene-D-sorbitol (DBS), glyceryl fatty acid esters). They have already been useful for several industrial applications such as in food products to replace non-healthy trans/saturated fats, in cosmetics to prevent oil leakage or to stabilize emulsions, in dermo-pharmacy/cosmetic for enhanced transdermal penetration, and in plastic and paint industries as thickeners. However, most of these LMOGs need a heating–dissolution process for oleogelation. As previously mentioned, such a process is a disadvantage for many industrial applications. In addition, there is a general tendency to promote the replacement of petro-sourced materials by renewable resources in order to avoid or reduce the impact that process technologies and industrial products have on the environment.
As part of our program aimed at designing and synthesizing carbohydrate derivatives with controlled self-assembly abilities, we recently demonstrated that amphiphilic sodium salts of β-C-glycosyl barbiturates could induce supramolecular hydrogelation by screening the negative charge on the barbituric ring after a heating/cooling cycle.4,5 Here, we report a simple, efficient, and an unprecedented one-step synthesis of an eco-friendly carbohydrate-based oleogelator, namely, N,N′-dimethyl β-C-glucosyl barbiturate (GlcBMe) that allows the formation of supramolecular oleogels induced by a short sonication time (cold process). Sodium salts of β-C-glycosyl barbiturates are easily accessible in water through a “green” Knoevenagel condensation between protecting-group-free carbohydrates and barbituric acid derivatives.6,7 Structure–oleogelation property relationships were performed with a series of β-C-glycosyl barbiturate derivatives that highlighted the delicate balance between the nature of the N-substituents on the barbituric ring and the orientation of the hydroxyl groups on the carbohydrate. Finally, detailed mechanical properties and flow behavior were fully characterized to establish, in particular, the thixotropic nature of the oleogels. Moreover, vitamin E, as an antioxidant used for topical applications, was entrapped during the oleogelation and the differential in vitro release profile was performed.
Oleogel | Surfactant | Oil |
---|---|---|
a GlcBMe – means oleogelator (sodium 5-(β-D-glucopyranosyl)-1,3-dimethylbarbiturate) and GlcBMe + Ar + H2O–mix means mixture of GlcBMe, argan and H2O without sonication; C = CTAB; T = TBAB, A = argan, Ro = rosehip, Al = almond and Co = coconut. | ||
aGlcBMe + Ar + H2O–mix | — | Argan |
GlcBMe–Ar | — | Argan |
GlcBMe–C–Ar | CTAB | Argan |
GlcBMe–C–Ro | CTAB | Rosehip |
GlcBMe–C–Al | CTAB | Almond |
GlcBMe–C–Co | CTAB | Coconut |
GlcBMe–T–Ar | TBAB | Argan |
GlcBMe–T–Ro | TBAB | Rosehip |
GlcBMe–T–Al | TBAB | Almond |
GlcBMe–T–Co | TBAB | Coconut |
![]() | (1) |
The discovery of our GlcBMe organogelator prompted us to investigate the structure/gelation property relationships by modifying selectively the nature of the carbohydrate or the N-substituent on the barbituric ring. The other potential LMOGs were synthesized in a similar manner by treatment of the corresponding carbohydrate (monosaccharide – glucose, mannose, galactose; disaccharide – cellobiose, maltose) with N,N′-disubstituted barbituric acid derivatives (N-methyl or N-cyclohexyl) in water at neutral pH and at 80 °C for 4 h (Scheme 1). The products were identified by 1D and 2D NMR, IR spectroscopy, and mass spectrometry (Fig. S2–S20†). The gelation tests showed no gelation properties for the series of synthesized β-C-glycosyl barbiturate derivatives and clearly evidenced the complexity of predicting LMOGs. Indeed, our results highlighted the fragile hydrophobic/hydrophilic balance needed to exhibit controlled aggregation without precipitation or complete solubility and the importance of the orientation of the carbohydrate hydroxyl groups for the non-covalent H-bond driving forces of gelation (Fig. S21†).
Gelation tests with less polar organic fluids such as edible oils were unsuccessful because of the high insolubility of our hydrophilic LMOG. Since our LMOG is a sodium salt of β-C-glucosyl barbiturate, we thought that by exchanging the sodium salt by an organic quaternary ammonium could compatibilized our LMOG to apolar solvents or oils. For such purpose, we used cetyltrimethylammonium bromide (CTAB) and tetrabutylammonium bromide (TBAB) which are also known as cationic surfactants. By this way, the gelation tests using sonication were successfully achieved with a wide range of vegetable oils such as argan, rosehip, almond, or coconut (Scheme 2). The MGC was still found to 2 wt% for all tested oils and the need of 0.4 wt% of water was still required. For the argan oil, the gelation occurred even without the need for organic quaternary ammonium (Scheme 2a), and no valuable explanations were found since the fatty acid composition of argan oil is roughly similar to those of almond oil.12
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Scheme 2 Mechanism of formation of (a) GlcBMe-based oleogel in argan oil and (b) GlcBMe-based oleogels with cationic surfactants and different oils. |
To deeper understand the role of each component before and after sonication, the microstructure of a mix of GlcBMe, water, and argan oil was visualized by confocal laser scanning (CLSM) and scanning electron microscopy (SEM). For improving the contrast between oil and water phases, a water-soluble fluorescein salt fluorophore was added. Before sonication, Fig. 1(a) (fluorescein stained) evidenced water droplets distributed non-homogeneously over the argan oily surface and SEM image revealed rod shape of as-prepared GlcBMe with a length of 0.55 ± 0.15 μm (Fig. 1(c)). While the sonication resulted in a more homogeneous dispersion of water and in mainly disaggregated GlcBMe areas (Fig. 1(b)). This suggests that sonication contributes to dissociate GlcBMe aggregates and to help in water penetration. This process allowed initiation of GlcBMe self-assembly towards a fibrillar network mixed with bridged GlcBMe microparticles as evidenced by SEM images (Fig. 1(d)) and as schematically illustrated in Scheme 2.
The same observations were pointed out for oleogels containing quaternary ammonium surfactants (CTAB or TBAB). Indeed, confocal images of a sonication-induced oleogel consisting in argan oil, CTAB, and GlcBMe oleogelator showed well-dispersed fibrillar structures encompassing granular CTAB crystals (Fig. S22†) and GlcBMe microparticles. The cationic surfactant particles in the “composite” or “hybrid” oleogel should act as additional physical cross-linking points in the network, presumably supported by ionic interactions between positively charged surfactants and the negatively charged surface of self-assembled GlcBMe fibers. This assumption was supported by the fact that non-ionic surfactants did not lead to oleogels.
XRD was used to evaluate the molecular assembly of GlcBMe and CTAB crystals in the GlcBMe–C–Ar oleogel, and the diffractograms are shown in Fig. S23.† The information about the order and the lateral packing of the molecular layers are provided by long spacing and short spacing peaks, respectively. Diffraction peaks in the XRD patterns of native GlcBMe and CTAB or the oleogel structured by GlcBMe and CTAB confirmed the presence of crystals, and their different spacing values indicated that the crystals had various structures, which were consistent with the results observed in SEM images. When oleogel is formed from the mixing of GlcBMe and CTAB in argan oil, we observed a broad diffraction signal around 20° 2θ, arising from the liquid crystal structuring of triacylglycerides of liquid argan (Ar) oil.13 And the higher diffraction peak in the long spacing region associated with the raw GlcBMe disappeared (48.5 Å), which indicated that a new self-assembly structure with fewer molecular layers was formed by GlcBMe. Noteworthy, several characteristic peaks for GlcBMe and CTAB were kept with slight shifts in d-spacing, suggesting that the subcell packing of GlcBMe and CTAB crystals were both modified in oleogel. It is reasonable to assume that in GlcBMe–C–Ar oleogel system, GlcBMe self-assembly and intimate mixture of crystal structures of GlcBMe and CTAB are the cause of oil gelation.
To further understand which molecular interaction occurred in the mixed crystals of GlcBMe, FTIR measurements were carried out. FTIR spectra of the oleogel samples (GlcBMe–Ar, GlcBMe–C–Ar, GlcBMe–T–Ar) as well as the raw materials (GlcBMe oleogelator, argan oil, CTAB, TBAB) and the mixture without sonication (GlcBMe–Ar–H2O–mix) are shown in Fig. 2 for comparison. First observation, the oleogels did not reveal a new peak formation or peak disappearance revealing that simply physical interactions arose between the components. Next, the FTIR spectra of oleogels exhibited a shallow broad peak in the range of 3700–3100 cm−1 assigned to intermolecular H-bonding network of OH groups of glucose and amide bonds of barbituric ring that is not present for argan oil and surfactants (CTAB and TBAB). The oleogels, argan oil, CTAB and TBAB showed an absorption band around 2920 cm−1 and 2850 cm−1, attributed to symmetrical and asymmetrical stretching of aliphatic C–H in CH2 and CH3 groups. The strong peak at 1750 cm−1 is characteristic of CO stretching vibrations of the ester carbonyl functional group of the triglycerides of argan oil as usually observed with vegetable or edible oils.14 Around 1680 cm−1 and 1580 cm−1, it was possible to distinguish characteristic bands of C
O of amide constituting GlcBMe.15 The argan oil-based oleogels shifted the position of the FTIR main peaks, with the most sensible ones about 1680 cm−1 and 1580 cm−1 (Fig. 2(b)), suggesting multiple molecular interactions between gelator–gelator, gelator–surfactants and gelator/surfactant–oil phase, including mainly intermolecular OH and C
O H-bondings and some van der Waals interactions.16 Thus, a possible mechanism of intermolecular interaction pattern was proposed in Fig. 2(c). Since GlcBMe oleogelator is not soluble in fatty phases, self-assembled fibers and resulting gelation can be mainly attributed to hydrogen bonding, while with surfactants, van der Waals interactions and particle bridging play a contributive role, even though they are much weaker than hydrogen bonding.
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Fig. 2 (a) IR spectra (4000–450 cm−1) and (b) (2000–1400 cm−1) of GlcBMe, argan oil, GlcBMe–Ar–H2O–mix, GlcBMe–Ar, CTAB, GlcBMe–C–Ar, TBAB and GlcBMe–T–Ar (c) illustration of self-assembly mechanism. |
Fig. 3 and S24,† along with Tables 2 and S1,† provide insights into the melting behavior of oleogels as characterized by DSC. Initially, GlcBMe and GlcBMe–Ar–H2O–mix exhibited glass transition at approximately 76 °C and 63 °C, respectively, indicating changing from a hydrogen-bound system.17 Notably, GlcBMe displayed a primary endothermic peak around 106.8 °C. Upon the addition of a small quantity of water without sonication (GlcBMe–Ar–H2O–mix), the peak shifted slightly to 109.8 °C, suggesting a change in the melting process due to partial water-solubilization of GlcBMe, that disrupting the organization of GlcBMe crystals in the oil system. Following sonication and formation of GlcBMe–Ar oleogel, a single endothermic peak at 114.6 °C was observed, indicative of the formation of a more robust structure, likely associated to a self-assembly into a fibrillar network. The lower melting temperature (60–96 °C), observed after the addition of CTAB or TBAB particles to GlcBMe, may indicate the melting of intimate mixed crystals (GlcBMe and CTAB or TBAB), as shown in Fig. S24.† However, despite the expectation that the insertion of CTAB or TBAB particles would promote additional physical cross-liking points, valuable explanations for this behavior were not found, indicating that they had complex interaction mode. Additionally, the different studied oils led to a slight variation in endothermic peak position. This suggests that composition, polarity, and viscosity of the oil likely disturb the specific organization of mixed crystal and consequently influence the melting behavior.
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Fig. 3 DSC graph for GlcBMe, GlcBMe–Ar, GlcBMe–Ar + H2O–mix, GlcBMe–Ar, CTAB, GlcBMe–C–Ar, TBAB, GlcBMe–T–Ar. *Analysis of GlcBMe, CTAB, and TBAB was made in oil. |
Rheological studies were then carried out to have more information on the mechanical strength and the flow behavior of oleogels. Oleogels prepared by self-assembly and after addition or surfactant particles were examined in rheological studies at 25 °C. Fig. 4(a) shows the amplitude sweep for oleogel GlcBMe–Ar and with the addition of surfactant particles in argan oil, GlcBMe–C–Ar and GlcBMe–T–Ar, respectively. All samples showed the amplitude sweep which exhibited dominant solid behavior with G′ > G′′, with higher values for GlcBMe–C–Ar and GlcBMe–T–Ar samples. For GlcBMe–Ar the G′ and G′′ start to decrease until reaching a critical strain of 6.5% (where G′ = G′′). Above the critical strain, G′ became smaller than G′′, indicating the breaking of the structure and the initiation of the flow of the sample in accordance with the typical behavior of a yield stress jellified suspension. A frequency sweep was done to obtain more information, as shown in Fig. 4(b). The testing showed a predominance of elastic solid-like behavior (G′ > G′′), with an apparent elastic response across the full frequency range (detail data for other studied oils shown in Fig. S25a†).18 The storage modulus (G′) values corresponding to the plateau at low strain rate in the linear domain of Fig. 4(a) can effectively describe the mechanical strength of gels, and the corresponding values are reported in Fig. 4(c). Even GlcBMe–Ar exhibited higher G′, the addition of surfactant particles, increasing the mechanical properties of oleogel with a significantly statistic difference (P < 0.05). The value with almost 1.0 × 10−5 Pa was rarely reported before with other LMWG (Table S2†),19,20 resulting in higher overall resistance to deformation. The G′ of the oleogels indicated their great potential to be used in applications requiring a semi-solid behavior. In Fig. S26a† we can note that the G′ values of the oleogels were influenced by oil nature. In addition, the tanδ(G′′/G′) value was summarized in Fig. 4(d) and S26b.† It was found that the tan
δ value of oleogel with surfactant particles was lower than GlcBMe–Ar, indicating the higher elasticity of oleogel after the insertion of surfactant particles. In terms of flow behavior, all samples displayed shear-thinning behavior since their viscosity declined gradually with the increasing shear rate (Fig. S27†). At the lowest shear rates, started the progressive disruption of the fiber network. With increasing shear rate, a complete breakdown of the fiber network displayed an orientation consistent with parallel flowing as evidenced by CLSM microscopy images in Fig. S28.†21 This relatively higher viscosity at a low shear rate will bring better long-term stability of the oleogels during storage which is important for industrial applications.22
Further, the thixotropic nature was examined by step-strain measurement, to investigate to gain insights into the structural recovery. A two-step breakdown/buildup procedure was applied during the breakdown step and increase of strain from 0.03% to high magnitude strain (100%) was applied to destroy the oleogel, and then, in the buildup step a low magnitude strain (0.03%) was exerted to evaluate the rate and extent of recovery of bulk properties. To investigate the recovery of oleogel after breaking and reforming, the G′ of recovering was shown in Fig. 5(a), (b) and S29–S30.† Interestingly, all oleogel reached 100% recovery, which is indicative of the impressive self-healing properties of the oleogel. Oleogel-based rosehip and surfactant particles was found to be able to rapidly recover the properties within 120 s, which demonstrated the reversible and robust nature of oleogel. More interestingly the recovery time seen in these oleogels is significantly influenced by the type of oil as well. The highest recovery G′ was demonstrated by oleogels prepared with argan and coconut. The differences in recovery time in terms of different oils may be explained by changes in the polarity and level of unsaturation of the oil. The triacylglycerol (TAG) composition is an important factor. Argan oil for example, mainly presented unsaturated groups like oleo-dilinolein (OLL), dioleolinolein (OOL), palmito-oleio-linolein (POL), palmitodiolein (POO), and triolein (OOO), including oleic and linoleic,23 suggesting that the unsaturated groups probably hinder the organization time of the fibers. It is clear that the oil type comprises diverse proportions of saturated and unsaturated fatty acids such as oleic acid (C18:
1), linoleic acid (C18
:
2), palmitic acid (C16
:
0), and stearic acid (C18
:
0) (Table S3†). According to Kim et al.,24 there is a correlation of the composition between the composition of oil in terms of the amount of C18
:
1 (oleic acid) and C18
:
2 (linoleic acid) fatty acids. Okuro et al.25 highlighted the relationship between solvent polarity on mechanical strength, which is explained by the polar components of the oil phase's ability to interact with the oleogelator by creating hydrogen bonds.
Oil binding capacity (OBC) is an important property of oleogels, which is attributed to the amount of the oil that remains entrapped within the structure relying on the interactions between liquid oil and the gelator molecules. The oil binding capacity might be influenced by factors such as size, shape, and distribution of components in the network.26,27 Oleogels-based different oils and surfactant particles were evaluated. Fig. 6(a) shows oleogels based on different oil and surfactant particles at a given oleogelator concentration. Oleogels-based rosehip showed a higher % OBC of around 60%. The higher percentage of OBC for oleogels-based rosehip showed a similarity to mechanical strength (G′). The percentage of OBC in oleogel samples on coconut was the lowest, around 20%. Considering different surfactant particles just for argan and almond oil showed some slight differences. However, the different type of oil seems to have more effect in % OBC, which probably in this system more branches and aggregates leading stronger 3D network which entraps liquid oil in the system.
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Fig. 6 (a) Oil binding capacity vs. different oil types at same gelator concentration (b) vitamin E release at pH 7.4 and 5.5 from oleogel GlcBMe–C. |
The in vitro release behavior of the vitamin E (VE – a-tocopherol) model entrapped in the gel network was examined by the method of dialysis. VE is a natural antioxidant acting in cutaneous protective pathways against aging, atopic dermatitis, or melanoma, for instance.28 It also widely used in food industry as a shelf-life enhancer of fatty products or to improve oxidative stability in heated oils. The release profile was carried out at two different physiological pH (7.4 and 5.5 (pH similar to the skin)) and similar behaviors were observed but with a higher release of VE at pH 7.4 (37% at 30 h) than at pH 5.5 (28% at 30 h) (Fig. 6(b)). A careful examination of the diffusion of VE through the lipid matrix of oleogels showed that during the first 2 h, a slight burst release of VE increased linearly for up to 15 h, after which the vitamin concentration remained constant. The higher release of VE at pH 7.4 compared to pH 5.5 is probably due to the higher solubility of VE at high pH, which increases the tendency of the drug molecule to leave toward the aqueous medium.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ra08087d |
This journal is © The Royal Society of Chemistry 2025 |