Changjiang
Fan
ab,
Chao
Zhang
c,
Liqiong
Liao
*a,
Sheng
Li
a,
Weiping
Gan
a,
Jinping
Zhou
a,
Dong-An
Wang
*b and
Lijian
Liu
a
aKey Laboratory of Biomedical Polymers of Ministry of Education & College of Chemistry and Molecular Sciences, Wuhan University, Wuhan, Hubei 430072, P. R. China. E-mail: liqiongliao@whu.edu.cn
bSchool of Chemical and Biomedical Engineering, Nanyang Technological University, 70 Nanyang Drive, Blk N1.3-B2-13, Singapore 637457, Singapore. E-mail: DAWang@ntu.edu.sg; Fax: +65 6791 1761; Tel: +65 6316 8890
cSchool of Engineering, Sun Yat-Sen University, Guangzhou, Guangdong 510006, P. R. China
First published on 9th July 2015
Abundant research efforts have been devoted to meet the demands for high-strength hydrogels in biomedical applications. Double-network (DN) hydrogels and homogeneous hydrogels are two typical samples. In this study, a novel ultra-strong and resilient double macromolecular network (DMMN) hydrogel system has been developed via a two-step sequential cross-linking process using hyaluronan (HA) and high molecular weight poly(ethylene glycol) (PEG) for the first and second network, respectively. A lower concentration of the HA precursor solution and a higher concentration of the PEG precursor solution as well as a higher molecular weight of the PEG precursor are beneficial to produce high-strength DMMN gels. Dynamic light scattering measurements demonstrate that DMMN gels possess the more evenly distributed polymer networks; the distinctive double and relatively evenly distributed networks of the DMMN gel make it combine the current DN and homogeneous network strategies for preparing robust hydrogels. The optimized DMMN gel is capable of sustaining up to 50 MPa of compressive stress. Besides, DMMN gels exhibit excellent cytocompatibility. This study expands the DN principle in designing and fabricating high-strength hydrogels with biocompatible macromolecules that show a promising prospect for biomedical applications.
Based on the fracture mechanisms of DN gels, energy absorption and dissipation of the ductile second network plays a critical role in the drastic enhancement of the mechanical strength of DN gels. According to our previous study,21,22 the hydrogel fabricated with poly(ethylene glycol) 20000 diacrylate (PEG20K-DA, Mn = 20
000 g mol−1) could store and dissipate much more fracture energy in the compression process compared with the hydrogel synthesized from lower molecular weight poly(ethylene glycol) 4000 diacrylate (PEG4K-DA, Mn = 4000 g mol−1). In this study, double macromolecular network (DMMN) gels have been designed and fabricated, based on the DN principle, using a two-step photocrosslinking with methacrylated hyaluronan (HA–MA) for the first network and PEG20K-DA or PEG4K-DA for the second network. The influence of the molecular weight and initial solution concentration of poly(ethylene glycol) diacrylate (PEG-DA) as well as the initial concentration of the HA–MA solution on the mechanical strength of DMMN has been evaluated in detail. The homogeneities of DMMN hydrogels are examined with a dynamic light scattering technique.
A hyaluronan–methacrylate conjugate (HA–MA) is synthesized by referring to the previous study after slight modification.23 Briefly, HA (1.0 g, 2.4 mmol) is dissolved in 250 mL of the phosphate-buffered saline (PBS, pH 7.4) solution, followed by the addition of 80 mL of DMF under vigorous stirring. GMA (0.1 mol) and triethylamine (0.05 mol) are added into the HA solution. The reaction mixture is stirred for five days at room temperature, and concentrated with rotary evaporation. The concentrated solution is dialyzed for three days in DI water, and then freeze-dried.
For the preparation of DMMN hydrogels, the HA gels, synthesized from 2%, 2.8%, or 3.5% (g mL−1) of the HA–MA solution, are immediately immersed into PEG20K-DA solutions (10%, 15%, or 20%, g mL−1) containing 0.05% (g mL−1) of Irgacure 2959. After 72 hours of immersion, the fully swelled HA gels are subject to crosslinking under UV light for 5 minutes after wiping off the surface solution to obtain DMMN gels. A series of DMMN gels are prepared with HA–MA and PEG20K-DA as parent precursors, and referred to as the DMMN-x–y gel (x and y stand for the initial percentage concentration of HA–MA and PEG20K-DA precursors, respectively). Besides, the DMMN-2-4K gel is fabricated from 2% (g mL−1) of the HA–MA solution and 20% (g mL−1) of the PEG4K-DA precursor solution.
Concentration (%) = Wd0/(Ws0 − Wd0) × 100% |
Mass ratio = (WDMMN − WHA)/WHA |
Water content (%) = (Ws − Wd)/Ws × 100% |
DMMN gels are fabricated by a two-step photocrosslinking. As shown in Fig. 1A, HA gels are synthesized from UV-light induced gelation of HA–MA solutions (Fig. 1A-a), and then immersed in PEG-DA solutions (Fig. 1A-b). HA gels swell gradually (Fig. 1B), at the same time, PEG-DA precursors and photoinitiators diffuse into HA gels (Fig. 1A-c). The fully swelled HA gels are taken out and exposed to UV light for the second crosslinking to obtain DMMN gels (Fig. 1A-d).
The diffusion process of the second precursor into the first network is crucial to determine the polymer content and mass ratio of the second and the first networks that have a great influence on the mechanical properties of the resultant DN gels.10 In particular, the macromolecular PEG-DA is different from the small monomer that is usually used to fabricate DN gels.6 For example, flexible PEG-DA precursors mainly exist in the form of chain aggregates in (semi-)concentrated solution and have a lower diffusion rate than the small monomer.28,35 Therefore, the diffusion of PEG20K-DA into the HA2.0 gel is typically monitored as a function of immersion time. As shown in Fig. 2, the polymer concentration in the HA2.0 gel rapidly increases from about 2% to 24% (w/w) within the first hour of immersion, which can be attributed to the de-swelling of HA2.0 gels due to the osmotic pressure caused by a great difference in polymer concentrations between the inside and outside of the HA2.0 gel. The similar phenomenon is also reported by Khademhosseini et al.29 After five hours of immersion, the polymer concentration in the HA2.0 gel reaches up to 31.5 ± 1.0% (w/w), whereas, the increase in the rate (slope of the curve) from the first to the 5th hour becomes smaller than that within the first hour. The polymer concentration in the HA2.0 gel decreases from the 5th to the 24th hour, which indicates that the re-swelling of the HA2.0 gel occurs. After 72 hours of incubation, the polymer concentration in the HA2.0 gel stabilizes at 22 ± 0.5% (w/w), which suggests that the concentration of the PEG20K-DA precursor reaches equilibrium between the inside and outside of the HA2.0 gel. This result demonstrates that three day immersion is enough for the diffusion of the PEG20K-DA precursor into HA gels.
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Fig. 2 Polymer concentration in the HA2.0 gel as a function of immersion time in 20% (g mL−1) PEG20K-DA solution. |
A series of hydrogels, including PEG gels, HA gels, and DMMN gels, are fabricated, and the compression tests are performed to study their mechanical properties with varied concentrations or molecular weights of precursors (Table 1). Interestingly, the PEG10 gel is stronger than the PEG20 gel; the fracture stress and fracture energy of the PEG10 gel are significantly higher than those of the PEG20 gel. This result does not accord with the classical Lake–Thomas theory that is followed by HA gels whose fracture stress and fracture energy are increased from the HA2.0 to HA2.8 and HA3.5 gel.30 Actually, we have observed a similar phenomenon in our previous study,21 and the unusual result should be attributed to the PEG network structures that are derived from the precursor solutions. Dynamic light scattering (DLS) measurements are performed to investigate the chain structures in PEG20K-DA solutions. As shown in Fig. 3A, in a dilute PEG20K-DA solution (0.5%, g mL−1), major PEG20K-DA precursors exist as a single chain, and their hydrodynamic radii (4.2 ± 0.6 nm) are close to the theoretical value (3.3 nm).31 In a (semi-)concentrated solution, more flexible PEG20K-DA chains entangle with each other to form chain aggregates. The hydrodynamic radius of PEG20K-DA chain aggregates increases from 58 ± 20 nm to 380 ± 97 nm with the increase of the concentration of the PEG20K-DA solution from 0.5% to 10% (g mL−1). When the concentration of the PEG20K-DA solution is 20% (g mL−1), the PEG20K-DA single chain disappears, and the hydrodynamic radius of chain aggregates reaches up to 1018 ± 124 nm. The increase in the size of chain aggregates from 10% to 20% (g mL−1) of PEG20K-DA solutions leads to a significant increase in spatial inhomogeneities that is directly demonstrated by a 5-fold increase in ensemble average scattering intensity (〈I〉E) (Fig. 3B).11,32 The spatial chain inhomogeneities can be frozen during the cross-linking process.34,35 Therefore, the networks of the PEG20 gel are more inhomogeneous than those of the PEG10 gel, typically including more network defects between chain aggregates and unevenly distributed cross-linking points as well as more inhomogeneous polyacrylate kinetic chains. The more inhomogeneities of PEG20 gels than PEG10 gels can cause severe stress concentration under stress,11 resulting in lower fracture strain, fracture stress, and fracture energy (Table 1).
Samples | Fracture stress (MPa) | Fracture strain (%) | Fracture energy (kJ m−3) | Mass ratio | Water content (%) |
---|---|---|---|---|---|
PEG10 | 5.78 ± 0.85 | 97.4 ± 1.2 | 275 ± 48 | — | 97.4 ± 0.2 |
PEG20 | 1.14 ± 0.37 | 86.3 ± 1.5 | 101 ± 30 | — | 95.7 ± 0.1 |
HA2.0 | 0.02 ± 0.01 | 45.6 ± 6.6 | 1.6 ± 0.4 | — | 99.9 ± 0.0 |
HA2.8 | 0.07 ± 0.02 | 38.5 ± 1.4 | 5.1 ± 1.1 | — | 99.7 ± 0.1 |
HA3.5 | 0.11 ± 0.01 | 39.9 ± 0.9 | 8.2 ± 0.4 | — | 99.5 ± 0.1 |
DMMN-2-10 | 17.7 ± 3.9 | 95.8 ± 1.2 | 678 ± 128 | 28.6 ± 3.7 | 97.4 ± 0.2 |
DMMN-2-15 | 30.5 ± 6.3 | 95.6 ± 2.4 | 1277 ± 110 | 40.7 ± 1.4 | 96.6 ± 0.1 |
DMMN-2-20 | 50.1 ± 4.4 | 94.6 ± 2.9 | 2374 ± 372 | 46.5 ± 2.0 | 95.9 ± 0.1 |
DMMN-2.8-20 | 8.22 ± 3.7 | 88.4 ± 1.6 | 475 ± 119 | 26.3 ± 4.0 | 94.3 ± 0.7 |
DMMN-3.5-20 | 1.03 ± 0.16 | 76.2 ± 1.5 | 215 ± 42 | 14.5 ± 0.7 | 92.2 ± 0.2 |
DMMN-2-4K | 2.73 ± 0.77 | 66.6 ± 0.9 | 323 ± 62 | 183.9 ± 11.9 | 88.7 ± 0.6 |
However, the fracture stress and fracture energy of the DMMN gels, fabricated with 2% (g mL−1) of the HA–MA solution for the first network, gradually increase with the increase of PEG20K-DA concentration from 10% to 15% and 20% (g mL−1); at the same time, their fracture strains are comparable (Table 1). In other words, the second PEG20K networks in the DMMN-2-20 gel are capable of absorbing and storing more fracture energy than those in DMMN-2-15 and DMMN-2-10 gels under stress. Surprisingly, this result does not agree with aforementioned PEG10 and PEG20 gels.
The elastic modulus of the HA2.0 gel is too small to be accurately measured; the elastic modulus of the DMMN-2-20 gel (41.3 ± 3.2 kPa) is not significantly different from that of the PEG20 gel (39.9 ± 9.5 kPa). The comparable elastic modulus indicates that the PEG20K networks both in the DMMN-2-20 gel and the PEG20 gel sustain the stress, but the fracture strain of the DMMN-2-20 gel (94.6 ± 2.9%) is significantly larger than that of the PEG20 gel (86.3 ± 1.5%). The homogeneity of the HA2.0 gel (the first network for DMMN-2-20 gel synthesis), DMMN-2-20 gel, and PEG20 gel is studied using DLS tests. As shown in Fig. 4b, compared with the PEG20 gel, the HA2.0 gel shows much lower average scattering intensity (〈I〉E), and as expected, 〈I〉E of the DMMN-2-20 gel is significantly lower than that of the PEG20 gel. These data demonstrate that the DMMN-2-20 gel, including PEG20K networks and HA networks, is composed of more evenly distributed polymer chains. The fracture patterns of the PEG20 gel and DMMN-2-20 gel are carefully observed and compared (Fig. 4a). The fracture of the PEG20 gel occurs in the middle and produces big pieces of fragments. This fracture pattern can be attributed to the evident stress concentration caused by network inhomogeneities,32,33 just like the above-mentioned unevenly distributed cross-linking points and inhomogeneous polyacrylate kinetic chains, as well as network defects. However, the entire DMMN-2-20 gel breaks into tiny pieces, suggesting that the load is evenly applied on the gel networks. These phenomena again demonstrate the homogeneity of the DMMN-2-20 gel. Therefore, the more evenly distributed PEG20K networks in the DMMN-2-20 gel, containing more PEG20K chains, can absorb and store more energy than those in the DMMN-2-15 gel and DMMN-2-10 gel, when they suffer the same compression deformation (namely strain).21 Compared with the inhomogeneous PEG20 gel, the more evenly distributed PEG20K networks in the DMMN-2-20 gel may have resulted from the disaggregation of PEG20K-DA precursors from chain aggregates in the diffusion process into the HA2.0 gel.35–37Fig. 5 illustrates the proposed formation mechanisms of the PEG gel and DMMN gel. The flexible PEG20K-DA precursors take random coil conformation and entangle with each other to form chain aggregates, which are frozen during the cross-linking process and results in an inhomogeneous PEG gel (Route 1).40,41 In Route 2, the HA2.0 gel serves as a template for the diffusion of PEG20K-DA precursors. PEG20K-DA chains dissociate them from the large chain aggregates in solution and diffuse into the HA2.0 gel, and then DMMN gels with more evenly distributed polymer networks are formed after second cross-linking.35–37
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Fig. 5 Schematic fabrication process of the PEG gel (Route 1) and DMMN gel (Route 2). SIPN stands for semi-interpenetrating networks. |
The obtained DMMN gels showed excellent mechanical properties, especially for the DMMN-2-20 gel. As shown in Fig. 6a–c, the DMMN-2-20 gel possesses excellent anti-compression ability in spite of its high water content (95.9 ± 0.1%, Table 1). It achieves an outstanding compressive fracture stress of 50.1 ± 4.4 MPa, which is about 2500 times and 44 times higher than that of the HA2.0 gel (0.02 ± 0.01 MPa) and PEG20 gel (1.14 ± 0.37 MPa), respectively. The fracture energy of the DMMN-2-20 gel (2374 ± 372 kJ m−3) is also obviously much higher than those of the HA2.0 gel (1.6 ± 0.4 kJ m−3) and PEG20 gel (101 ± 30 kJ m−3). The superior mechanical strength and large recoverable deformation are vividly demonstrated by loading a person's body weight (approx. 74 kg, i.e., 163 pounds) on the DMMN-2-20 gel (diameter 12.5 mm, height 10.8 mm) (Video, ESI†). The gel can fully recover from the compressed state upon removal of load and retain its intactness and resilience, exhibiting rubber-like behaviors. The cyclic loading experiments are carried out to explore energy dissipation of DMMN gels. As shown in Fig. 6d, the DMMN-2-20 gel dissipates energy effectively, as demonstrated by the large hysteresis loop in the first loading–unloading curve. The pronounced hysteresis is also observed in the first loading–unloading cycle of the PEG20 gel (Fig. 6e), suggesting that the second PEG network in DMMN gels can effectively dissipate energy under stress. This result indicates that the PEG network as the second network is significantly different from the widely used polyacrylamide (PAAm) network that shows negligible hysteresis in the loading–unloading cycle.6,20 Immediately second loading–unloading cycles of the PEG20 gel and DMMN-2-20 gel are conducted. The hysteresis loops for both gels become much smaller at the second loading–unloading cycles. These results demonstrate that the energy dissipation of DMMN gels under stress might mainly be attributed to the rearrangement of PEG20K chains of the second network, such as coil-stretch conformation transition.21,38
To further characterize the DMMN gel system, the influence of the molecular weight of the PEG-DA precursor and the concentration of the HA–MA solution on the mechanical properties of DMMN gels are evaluated, respectively (Table 1). The DMMN-2-4K gel is fabricated with the same 2% (g mL−1) HA–MA solution as the first network and 20% (g mL−1) PEG4K-DA solution as the second network. However, the fracture stress of the DMMN-2-4K gel (2.73 ± 0.77 MPa) are significantly lower than that of the DMMN-2-20 gel. Weng et al. report a series of HA/DAAm DN gels, using 2% (g mL−1) HA gel as the first network and the small monomer N,N-dimethylacrylamide (DAAm) as the second network, of which the maximum fracture stress is 5.2 MPa.39 Compared with the DMMN-2-4K gel and HA/DAAm DN gel, we can conclude that the high molecular weight of the PEG-DA precursor plays an important role in generating high-strength double-network gels. The PEG20K networks in the DMMN-2-20 gel have lower crosslink density than PEG4K networks in the DMMN-2-4K gel due to the higher molecular weight;21 the lower crosslink density is beneficial to the extension of PEG20K chains under stress.21 Besides, the chain length of PEG20K networks in the DMMN-2-20 gel is higher than that of PEG4K networks in the DMMN-2-4K gel. Therefore, the DMMN-2-20 gel can achieve a higher strain and absorb more fracture energy than the DMMN-2-4K gel. When keeping the concentration of PEG20K-DA constant at 20% (g mL−1), the increased concentration of the HA–MA solution from 2% to 2.8% and 3.5% (g mL−1) makes the fracture stress of the DMMN gels drop greatly from 50.1 ± 4.4 to 8.22 ± 3.7 and 1.03 ± 0.16 MPa. The above results suggest that higher molecular weight of PEG-DA precursors (for the second network) and lower initial concentration of the HA–MA precursor solution (for the first network) are beneficial for producing high-strength DMMN gels.
The mass ratio of the second network to the first network is regarded as the crucial structure parameter for preparing robust DN gels.10 As shown in Fig. 7, similar to previously reported DN gels,6 the fracture stress of the DMMN gels increases with the increase of the mass ratio of the second to the first network, except for those of DMMN-2-10 and DMMN-2.8-20 gels. They exhibit a similar mass ratio of PEG to HA network (Table 1 and Fig. 7), however, the fracture stress and strain of the DMMN-2–10 gel (17.7 ± 3.9 MPa and 95.8 ± 1.2%) is significantly higher than those of the DMMN-2.8-20 gel (8.22 ± 3.7 MPa and 88.4 ± 1.6%). Furthermore, though the mass ratio of DMMN-2-4K is up to 183.9 ± 11.9, its fracture stress and fracture strain is only 2.73 ± 0.77 and 66.6 ± 0.9%, respectively. This result further demonstrates that the relative lower concentration of the HA–MA precursor solution as well as the higher molecular weight of the PEG-DA precursor is crucial for preparing high-strength DMMN gels. Cytotoxicity of DN gels is another major concern for biomedical applications,10 and the DMMN gels exhibit excellent cytocompatibility due to the widely recognized materials (namely PEG and HA) as well as the well established photo-crosslinking method (ESI,† Fig. S2).
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Fig. 7 Mass ratios of the PEG20K network to HA network in DMMN gels. The statistical significance is indicated with **(p ≤ 0.01). |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5tb00867k |
This journal is © The Royal Society of Chemistry 2015 |