2.1. Rheological Properties of the Inks
Steady-state and oscillatory measurements were conducted, as depicted in
Figure 1A for the shear sweep and in
Figure 1B for the frequency sweep, respectively. All samples exhibited shear-dependent viscosity, which varied with collagen/chitosan ratio (
Figure 1A). It was observed that samples with a higher collagen content (0CHI) had higher viscosity, a trend also reported by other authors [
14]. Shear-thinning behavior, characterized by a decrease in viscosity with increasing shear rate, was observed for the three samples. The observed shear-thinning behavior (
Figure 1A) originates from a complex molecular reorganization within the hybrid network. At low shear rates, the ink maintains high viscosity due to the entanglement of collagen triple helices and chitosan chains, stabilized by a dense network of hydrogen bonds. As the shear rate increases, mechanical stress breaks these physical interactions and forces the biopolymer chains to align in the direction of flow. This behavior is highly desirable for printable solutions, as they are intended to flow easily when subjected to syringe-driven forces [
14].
Several rheological models were evaluated to fit the experimental data. The Carreau–Yasuda model was selected as it provided the most accurate fit (R
2 = 0.99–1.00) and effectively described the Newtonian plateau at low shear rates and the subsequent transition to shear-thinning behavior. As can be seen in
Figure 1A and confirmed in
Table 1, infinite-viscosity values (
) were significantly different as a function of the chitosan content used. The higher the chitosan content, the lower the viscosity values at low shear rates. This effect was not noticeable at high shear-rate values. The relaxation time constant (
λc) was also affected by the chitosan content used, indicating that viscosity started decreasing as a function of the shear rate at slightly higher values.
The rheological parameters derived from the Carreau–Yasuda model provide a clear relationship with the extrusion performance. At high shear rates (), low viscosity values ensure that the ink flows easily through the nozzle, facilitating a continuous extrusion process. Conversely, at low shear rates (), high viscosity values provide significant resistance to flow, which is crucial for the material to stop flowing once deposited on the platform. To better understand whether the deposited filament will remain stable and support additional layers without collapsing, it is necessary to analyze the frequency sweeps, which characterize the mechanical integrity of the polymeric system at rest.
Oscillatory measurements (
Figure 1B) demonstrated that all the studied samples exhibited solid-like behavior, with the storage modulus (G′) higher than the loss modulus (G″) [
15]. The observed solid-like behavior is highly beneficial for the deposition process on the printing platform, ensuring structural stability and allowing the printed layers to support the weight of subsequent layers of material without deformation. The moduli values also depended on the chitosan content, as shown in the shear sweeps, with 40CHI having the smallest difference between G′ and G″ and, thus, the lowest self-supporting capacity, indicating the importance of selecting the collagen/chitosan ratio [
16]. These rheological differences among the three samples demonstrate interactions between the two polymers, resulting in changes in their shear and frequency curves, probably due to the penetration of chitosan among collagen fibers, leading to a decompaction of the fibers and altering their flow properties [
17]. Additionally, it has been proposed that new interactions may form between both biopolymers through hydrogen bonds between hydroxyl and amino groups of chitosan and the polar side chains of the amino acid residues in collagen [
18].
2.2. Physicochemical Properties of the Scaffolds
The structure of the samples was determined using X-ray diffraction, as can be observed in
Figure 2A. The peak around 7.4° represents the distance between the chains in the triple helix of collagen, while a peak around 22° is related to the unordered parts of collagen [
19]. The peak around 30° could be related to collagen fibrillar order [
20]. Overall, it can be concluded that the structure of the scaffolds is amorphous, with some regions showing more ordered structures.
Regarding thermal properties, DSC curves (
Figure 2B) showed two endothermic peaks. The first peak around 100 °C is related to the water release, and the second one around 200–220 °C is attributed to the denaturation of collagen [
21]. While this process may overlap with the onset of thermal decomposition, it is well-documented that the major thermal degradation of the collagen backbone occurs at higher temperatures, typically around 300 °C [
22,
23]. This second transition exhibits a visible broadening and a shift towards lower temperatures in the chitosan-containing formulations compared to the pure collagen control (0CHI). This broadening could reflect a decrease in the cooperativity of the thermal process, indicating that the penetration of chitosan chains into the collagen bundles creates a more disordered molecular arrangement. Furthermore, the shift in the denaturation onset further suggests that the interactions between both biopolymers interfere with the native stabilizing forces of the fibers, effectively reducing the thermal stability of the collagen arrangement [
24]. In order to assess the interactions between collagen and chitosan, FTIR spectra are presented in
Figure 2C. The broad band from 3600 cm
−1 to 3000 cm
−1 is attributed to N-H and O-H vibrations. The amide I band appears at 1629 cm
−1, 1631 cm
−1, and 1633 cm
−1 for 0CHI, 20CHI, and 40CHI, respectively, suggesting the interactions between collagen and chitosan by hydrogen bonding [
25]. The amide III band also shifts from 1239 cm
−1 for 0CHI and 20CHI to 1241 cm
−1 for 40CHI. These shifts suggest that the amino (–NH
2) and hydroxyl (–OH) groups of chitosan interact with the carboxyl (–COOH) and amide groups of collagen chains. These physical interactions effectively modulate the molecular environment, reinforcing the hybrid matrix and promoting the rheological and mechanical stability observed in the 20CHI and 40CHI formulations.
The construction of a precisely defined object through 3D printing requires high control over the filament diameter. This control is conditioned not only by the exit diameter of the needle but also by the viscoelastic properties of the hydrogels [
14]. For the 0CHI formulation (
Figure 3A), excessive gelation was observed, resulting in a misaligned and irregular filament. On the contrary, the filament formed by 20CHI ink (
Figure 3B) was regular in all the sections and showed a smooth appearance, indicating the ability of this ink for 3D printing. Finally, as expected by the previously shown rheological results, 40CHI exhibited insufficient gelation capacity (
Figure 3C), as can be observed by the drop formed at the bottom of the extruded filament [
26]. Considering the filament with the best shape fidelity, 20CHI ink was selected for 3D printing (
Figure 3D) to obtain a 1 mm height scaffold (
Figure 3E). The inner structure of this scaffold was investigated by scanning electron microscopy (SEM), revealing a porous structure (
Figure 3F). Importantly, the collagen fibril structure was observed (
Figure 3G), indicating that the chitosan addition does not compromise the structure of collagen and preserves the triple helix. These results are consistent with the abovementioned rheological results, which showed higher viscosity for samples with higher collagen content, and also with FTIR results, which suggested new interactions between collagen and chitosan, resulting in an easier flow of the material through the nozzle. Furthermore, the printed material retains its shape, preserving the triple helix structure and forming a porous scaffold as required for tissue engineering [
27].
In order to assess the behavior of the scaffolds in contact with water, swelling tests were performed, and the results are shown in
Figure 4A. 0CHI samples reached a swelling value of 420%, while chitosan-containing samples showed values of 1615 and 1550% for 20CHI and 40CHI, respectively. The difference in the swelling profile is due to the different nature of collagen and chitosan molecules. Collagen is a fibrous protein with a triple helix configuration, and chitosan penetrates between protein chains, loosening the network and increasing the water uptake capacity. It is worth noting that the increase in chitosan content did not increase the swelling capacity of the scaffolds. The stabilization of the swelling capacity in the 40CHI formulation, despite higher chitosan content, can be related to the opposite effects caused by the network loosening and the physical crosslinking when increasing chitosan content. Although the incorporation of chitosan disrupts the tight collagen packing, as evidenced by the DSC and XRD results, the higher content of chitosan in 40CHI increases the number of available functional groups for intermolecular hydrogen bonding. This creates a more densely interconnected hybrid network that, while less stiff than 20CHI due to the lower collagen content, provides enough physical resistance to limit further water uptake. This is consistent with the rheological findings, where 40CHI inks showed the lowest zero-shear viscosity, indicating a different degree of molecular entanglement that ultimately governs the scaffold’s macroscopic behavior. Regarding hydrolytic degradation, the values are shown in
Table 2. As can be seen, degradation values ranged around 25% after reaching swelling equilibrium for all the samples, with no statistical differences among them.
In addition to chemical biomimicry, scaffolds must exhibit a mechanical behavior similar to that of the target tissue in order to ensure proper cell differentiation. Therefore, compression tests with 10% deformation were performed, and stress–strain curves are shown in
Figure 4B. A 10% compressive strain was selected to ensure a stable mechanical response within the linear viscoelastic region of the scaffolds, accounting for the initial compliance of the hydrogels. This value, although slightly exceeding the physiological range from 2.4% to 8.5% reported by Eckstein and colleagues for patellar cartilage, is representative of the upper limit of physiological deformations and allows for a robust calculation of the compressive modulus [
28]. In this work, cohesiveness is defined as the ability of the scaffold to recover its original height and structural integrity after repeated loading. This parameter was calculated as the ratio of the second compressive stress divided by the first one, and, therefore, values close to one indicate a good recovery ability. As can be seen in
Figure 4B, all the samples exhibit linear deformation behavior until 2% strain, but the stress values go up sharply in chitosan-containing samples, while collagen samples remain linear. The calculated compressive moduli are shown in
Table 2, where the 20CHI samples showed the highest values (12.8 kPa). Although this modulus falls within the physiological range described for native cartilage (10–20 kPa) [
29]. This alignment is observed under a specific macroscopic strain of 10 %. It should be noted that, although this deformation allows for a reliable calculation of stiffness within the linear viscoelastic region, the mechanical behavior of native tissue is ultimately determined by its complex anisotropic architecture under dynamic loading, which differs from the static evaluation performed on the scaffolds. Regarding cohesiveness values, it can be observed that chitosan-containing samples demonstrated superior recovery compared to pure collagen after two compression-decompression cycles. The decrease in the compressive modulus for 40CHI is attributed to the steric hindrance caused by the excess of chitosan chains, which disrupts the continuity of the collagen fibrillar network and interferes with the efficient distribution of mechanical stress across the matrix.
Swelling and mechanical results indicated that interactions between chitosan and collagen occurred. It is noteworthy that the total biopolymer concentration remained constant for all samples (3%). The 2.6-fold increase in the compressive modulus for the 20CHI formulation compared to the control (0CHI) demonstrates that the mechanical performance is governed by synergistic intermolecular interactions rather than simple polymer concentration. This reinforcement results from the formation of a hybrid network stabilized by hydrogen bonding between chitosan and collagen, which effectively enhances the stiffness and cohesiveness of the scaffold despite the lower collagen content. Considering the obtained results, the 20CHI formulation, in comparison to 0CHI, was selected to perform advanced characterization by SAXS, WAXS, and SANS, as well as cytocompatibility and neocartilage formation tests.
2.3. Advanced Characterization by WAXS, SAXS, and SANS
With a transmitted beam, WAXS analysis revealed the same characteristic triple helical structure of collagen in both 0CHI and 20CHI samples, featuring distinct peaks at q = 2.2 Å
−1 (
Figure 5A). This suggests the molecular integrity of collagen, supporting the observations from XRD, which characterize the surface of the scaffolds. The broad peak at around q = 3.0 Å
−1 was also observed, which represents the amorphous collagen peptide chains.
SAXS analysis (
Figure 5B) showed that the control dry collagen scaffold (0CHI) has smooth interfaces according to Porod’s law, with the scattering intensity featuring a q
−4 dependence. A similar power law dependence was observed for 20CHI. The sharp peaks between q = 0.10–0.50 Å
−1 shown in both 0CHI and 20CHI samples indicate a lamellar structure. It is noteworthy that both scattering profiles lacked the set of sharp peaks that originated from the quarter-staggered periodic packing in native collagen fibers. However, a broad peak at q = 0.50–0.60 Å
−1 (
Figure 5C) was observed as a characteristic feature for laterally packed collagen molecules (intermolecular lateral packing, ILP in short), matching a known 1.1–1.2 nm packing distance in dry collagen fibers [
20] and the 7.4° peak in XRD results. These observations suggest that collagen was dispersed during processing, then allowed to pack laterally, although randomly positioned axially.
Also, the integrated 1D SAXS profile of the 0CHI sample showed a sharp turn at q = 0.54 Å−1, suggesting that this broad feature was significantly oriented at the spots measured, whereas in the 20CHI sample, this is less prominent. It could be related to the better dispersion of collagen assemblies through the interaction with chitosan that moderates the gelation. Additionally, an indicative broad peak was found only in the 20CHI sample at around 0.20 Å−1. This may be associated with an intermolecular packing structure of collagen/chitosan in the scaffold, with a d-spacing of 3.1 nm.
The structural features were further studied using humidity-controlled SANS to highlight changes when 0CHI and 20CHI absorb moisture (D
2O in this case). SANS data of the samples at three q-ranges were plotted separately (
Figure 6).
At high q, the peak from laterally packed collagen molecules (ILP peak) and the residual peaks were again observed (
Figure 6A,D), matching the SAXS results. At mid q, data were composed of a power law dependence (
Figure 6B,E), which continued towards low q before the intensities were affected by multiple scattering (
Figure 6C,F). Within the q-range sufficiently separated from the affected part at low q, 0CHI and 20CHI showed power law dependences of q
−3.52 and q
−3.67, respectively, suggesting rough interfaces between structural domains across multiple scales. Note that the exponents were generally smaller than those from the SAXS results, due to the different contrast space of SAXS and SANS. SANS is advantageous for resolving the interfaces between polypeptide, polysaccharide, and solvents, as these two biopolymer components have poor contrast under X-ray, as shown in
Figure 2A.
Upon changing the RH levels from 2% to over 90% (equilibrium of RH reached within 40 min), D
2O absorption occurred rapidly in the first 1–2 h, showing an increase in the interface scattering intensity (mid q and low q, the power law component) and the diminished ILP peak and decreased background (high q, constant). If the ILP had remained ordered, D
2O would have increased the contrast between the triple helical molecules and revealed a stronger peak. Therefore, our observation suggests that the lateral packing of collagen molecules was less ordered upon swelling. The change in background is associated with the hydrogen–deuterium exchange (HDX) on labile sites, which reduces the total incoherent scattering of the sample. The process is much slower in 0CHI control (5 h) compared to 20CHI (1.5 h). This can be an indicator of water accessibility through the scaffold matrix associated with multiple factors, including pore size and connectivity, as well as surface hydrophilicity, confirming the swelling results obtained, where swelling increases significantly with the incorporation of chitosan (
Figure 4A).
At mid q and low q, the significant and steady increase in the intensity of the power law component upon exposure to RH = 90% suggests an enhanced contrast associated with the uptake of D2O into voids in the matrices. D2O in 0CHI slowly dispersed through the matrix over the tested period (16 h), and, in contrast, for 20CHI, intensity increased rapidly for the initial 1 h, followed by negligible differences for the remaining 15 h.
Comparing the humid end products, the power law exponent increased from q−3.52 and q−3.67 to q−3.63 and q−3.75 at the hydrated state. The interfaces are slightly smoother when swollen, probably due to the straightened interdomain areas with voids holding up water. It is also noted that, during the tested period, no gel network nor quarter-staggered native collagen was observed. The lack of gel network features suggests that the scaffolds contain mostly bundled integrated collagen molecules rather than unfolded (denatured) gelatin-like chains, indicating that the procedure used in the preparation of the gels does not break down the triple helix of collagen, maintaining its fibrillar structure, and, consequently, the scaffolds maintain their structure in culture media at 37 °C.
2.4. Cytocompatibility Assessment and Biochemical Evaluation of Neocartilage Formation
Cytocompatibility is one of the most important features when developing new treatment strategies in tissue engineering. In this study, the scaffold was tested in accordance with the ISO 10993-1 standard for “Biological evaluation of medical devices” [
30]. In this case, experiments were performed with 3T3-J2 murine fibroblasts as a cell model. The standard stipulates that cell viability cannot be less than 70%. As can be seen in
Figure 7, cell viability is higher than 70% for the extract and for direct contact cytotoxicity studies, indicating the cytocompatibility of the scaffolds.
Subsequently, to assess whether these scaffolds could support the growth of two cell types, adipose mesenchymal stem cells (aMSCs) and chondrocytes, the proliferation of both cell types was assessed over 7, 14, 21, and 28 days. As can be seen in
Figure 8A, both chondrocytes and aMSCs proliferated in culture continuously, with subtle differences over time. For example, chondrocytes showed greater proliferation from day 21 in culture, while aMSCs slowed down and continued to increase in number by day 28. These quantitative results obtained are in agreement with fluorescence microscope images (
Figure 8B), confirming high cell viability throughout the extended culture. As illustrated in
Figure 8B, aMSCs exhibited slower growth and remained in more isolated clusters at day 28, while the chondrocytes demonstrated a tendency to cover the entire scaffold. Nevertheless, these observations indicate that the scaffolds allow both survival and proliferation of the two types of cells.
In addition, this study aimed to assess the ability of the scaffolds to support extracellular matrix deposition by aMSCs and chondrocytes. Quantification of total sGAG demonstrated increased extracellular matrix (ECM) deposition by days 21 and 28 for both cellular types (
Figure 8C). Chondrocytes produced a slightly higher content of sGAG over time. These results indicate that the developed scaffolds effectively support ECM deposition by both aMSCs and chondrocytes. The observed increase in sGAG content at days 21 and 28 suggests active and sustained ECM synthesis, a key indicator of the functional scaffold performance in cartilage tissue engineering. Notably, chondrocytes produced slightly higher levels of sGAG across all time points, consistent with their native chondrogenic phenotype and intrinsic capacity to secrete cartilage-specific ECM components [
31]. In contrast, aMSCs exhibited a gradual increase in sGAG production, highlighting the scaffold’s potential to support chondrogenic differentiation in progenitor cells. The comparable ECM deposition by both cell types at later stages suggests that the scaffold microenvironment provides favorable biochemical and biophysical cues for matrix synthesis and cellular function. Although specific chondrogenic markers were not quantified, the sustained sGAG production over 28 days is indicative of the functional activity of the cells and the active secretion of a cartilaginous extracellular matrix. Although steady matrix deposition highlights the potential of the 20CHI scaffold for cartilage regeneration applications, the absence of specific chondrogenic markers and in vivo validation remains a limitation that must be addressed in future studies to definitively confirm its regenerative efficacy.