Lie
Chen
a,
Xi
Yao
b,
Zhandong
Gu
a,
Kaikai
Zheng
c,
Chuangqi
Zhao
a,
Wenwei
Lei
a,
Qinfeng
Rong
a,
Ling
Lin
g,
Jiaobing
Wang
d,
Lei
Jiang
ae and
Mingjie
Liu
*af
aKey Laboratory of Bio-Inspired Smart Interfacial Science and Technology of Ministry of Education, School of Chemistry and Environment, Beihang University, Beijing, 100191, P. R. China. E-mail: liumj@buaa.edu.cn
bSchool of Engineering and Applied Sciences, Kavli Institute for Nanobio Science and Technology, Harvard University, Cambridge, 02138 MA, USA
cState Key Laboratory of Polymer Physics and Chemistry, Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100190, P. R. China
dSchool of Chemical and Chemistry Engineering, Sun Yat-sen University, Guangzhou, 510275, P. R. China
eKey Laboratory of Bio-Inspired Materials and Interfacial Science, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, P. R. China
fInternational Research Institute for Multidisciplinary Science, Beihang University, Beijing, 100191, P. R. China
gEngineering Research Center of Marine Biological Resource Comprehensive Utilization, SOA, The Third Institute of Oceanography of the State Oceanic Administration, Xiamen 361005, China
First published on 16th November 2016
The diffusion and transport of substances between a hydrogel and its environment have received tremendous research interest, due to the wide range of applications of hydrogel materials in fields related to drug carriers and drug delivery vehicles. To date, much research has been done to tailor the diffusion and transport of substances through hydrogels, where most efforts were focused on tuning the 3D network properties of the hydrogel including loop size, hydrophobicity of building blocks and the stimuli-responsive properties of backbones. These conventional strategies, however, usually suffer from complicated fabrication procedures and result in a homogeneous increase in hydrophobicity of the hydrogel network, leading to low efficiency control over the diffusion of substances through the hydrogel. Herein, a facile strategy that can functionalize the surfaces of hydrogels, while keeping the interior network unchanged, was reported, and is realized by quaternization reaction confined to the hydrogel/oil interface. Owing to the introduction of the photo-responsive molecule IBSP as a modifier, the surface wettability of the resulting hydrogel can be controlled by light both in air and underwater environments. Consequently, the diffusion rate of a substance through this modified hydrogel can be regulated by light, which brings convenience to the controlled release of hydrogels and other hydrogel-related fields.
To date, a large variety of stimuli-responsive hydrogel systems that can respond to external stimuli, such as light illumination,6 temperature,7 pH,8 ionic strength,9 electricity,10 magnetic fields,11 and certain chemicals, were developed for the controlled release of cargoes embedded in hydrogels.12 Light and temperature are contact free and environmentally friendly stimuli, which make them the most commonly used to trigger substance release from hydrogels. Conventionally, the most straightforward method to obtain a stimuli-responsive hydrogel is the chemical modification of a hydrogel with stimuli-responsive moieties in its building blocks or use of a stimuli-responsive polymer to construct its network.13 To realize the controlled release of small molecules or macromolecules such as proteins and other biomacromolecules based on this hydrogel, stimuli-responsive swelling/deswelling and sol–gel transition processes of the hydrogel were generally adopted.14 However, these strategies that are used to prepare stimuli-responsive hydrogels usually require complex procedures, and the sol–gel transition process of the hydrogel would inevitably lead to the burst release of cargoes incorporated in the hydrogel. Consequently, it remains a challenge to develop a more reasonable strategy that can overcome these shortcomings.
Herein, we report a facile strategy to functionalize the surface of hydrogels with photo-responsive wettability and photo-controlled release properties. A spiropyran derivative was covalently tethered on the hydrogel surface forming a superficial layer with a thickness of about 1.2 μm through confined quaternization reaction at the hydrogel/oil interface. The resulting hydrogel exhibits superhydrophobicity and photo-responsive properties on its surface, while the superhydrophilicity of the hydrogel inner networks was well preserved. Due to the photo-responsive ring opening and ring closing mechanisms of modifiers, the underwater oil wettability and underwater oil adhesion force upon this modified hydrogel can be reversibly switched using light illumination. Finally, this superhydrophobic photo-responsive superficial layer on the modified hydrogel has a significant influence on preventing the immediate diffusion of substances from the hydrogel to the aqueous environment, and the diffusion rate of substances from this modified hydrogel can be controlled using light. The simple method to prepare stimuli-responsive hydrogels reported in this work promotes immediate applications of hydrogels in areas related to substance diffusion, as well as potentially having applications in drug carriers or drug controlled release systems.
The photo-responsive molecule IBSP that is used in this work is basically of the same nature as spiropyran, which is a widely utilized photo-responsive molecule, due to the vast difference in physico-chemical properties of spiropyran (SP) and merocyanine (MC) isomers.22 The charge separation in MC that is formed upon ultraviolet (UV) irradiation gives rise to a large electric dipole moment compared with the SP isomer. As shown in Fig. 2a, the SP and MC isomers can be reversibly switched through illumination with UV and visible (Vis) light, respectively.
As shown in Fig. 2b, the surface of the hydrogel became superhydrophobic after modification,23 and when further illuminated with UV (365 nm, 120 mW cm−2, 10 s) irradiation the hydrophobicity of the hydrogel surface was reduced, which is due to the photo-induced isomerization of the non-polar SP form to the polar MC form. This process can be reversed by visible light (470 nm, 30 mW cm−2, 5 min) illumination.24 As shown in Fig. 2c, the water contact angle on the surface of the modified hydrogel was decreased by 10 degrees (from 152.1° to 142.1°) in twenty minutes. This indicated that the superhydrophobicity of the modified layer on the hydrogel is quite stable in air.
The success of interfacial modification of the hydrogel was confirmed using UV-Vis spectroscopy. Fig. 2d shows UV-Vis spectra of IBSP (dissolved in dichloromethane) before (black) and after (red) UV irradiation, and it was found that the SP isomer is optically transparent in the visible region whereas the MC isomer absorbs strongly at 500–650 nm. Fig. 2e shows UV-Vis spectra of the hydrogel (ca. 1 mm in thickness) coated with IBSP, and after UV irradiation it develops a broad peak at 500–600 nm, which is almost the same position as compared with Fig. 2d. This suggested that the IBSP was successfully coated on the hydrogel. In addition, the success of modification can also be identified by the color change of the modified hydrogel before (faint yellow) and after (pink) UV irradiation (Fig. 2b).
As mentioned above, the oil used in this work was not perfectly immiscible with water, which would give rise to the modifiers dissolved in oil being able to penetrate into the hydrogel and graft onto the polymer network, forming a hydrophobic layer with limited thickness on the hydrogel surface. The thickness of this hydrophobic layer was characterized using laser scanning confocal microscopy (LSCM). Owing to the fluorescence properties of IBSP (Fig. S1†), the fluorescence of IBSP molecules can be observed using LSCM when IBSP is illuminated by proper excitation light (488 nm). As shown in Fig. 3a, the thickness of the modified layer increased upon increasing the modification time. Furthermore, with an extension of the modification time, the thickness of the modified layer reached a plateau (1.2 μm) in about 7 hours (Fig. 3b).
Since the modification of the hydrogel was successful (the success of the modification was also confirmed using FTIR spectroscopy as shown in Fig. S2†), we supposed that the superhydrophobicity of the hydrogel was attributed to its surface composition and surface roughness. On one hand the surface energy was reduced due to the hydrogel surface being covered by hydrophobic components after modification.25 On the other hand, after modification hierarchical micro-/nanoscale surface roughness on the IBSP-modified hydrogel was generated. Fig. 3c and d show the 3D morphology of the hydrogel before and after modification, respectively. Before modification, only micro-scale grooves were observed, which are introduced by cutting. After modification, micro-/nanoscale surface roughness was generated and contributed to the formation of superhydrophobicity on the surface of the modified hydrogel.26 As for the formation of micro-/nanoscale surface roughness on the IBSP-modified hydrogel, it was supposed that the organic modified layer was swollen with oil after the modification. Once the hydrogel was exposed to an air environment, this layer would shrink and form nano-scale roughness due to oil evaporation.27 Further, upon illuminating the IBSP-modified hydrogel with UV light there was no obvious difference observed in the surface morphology, as shown in Fig. 3e compared with Fig. 3d. This may be due to the change in surface morphology on a molecular scale, which cannot be observed using 3D optical microscopy.
Generally, due to the dehydration of hydrogels in air, hydrogels have been designed and prepared for use in aqueous environments, such as in microfluidic devices,28 water/oil separation,29 contact lenses,30 drug release systems and marine antifouling coatings.31 Taking this into consideration, a few tests were carried out in underwater environments to estimate the stability of the modified layers on hydrogel surfaces. As shown in Fig. 4a, the underwater oil (1,2-dichloroethane, 2 μL) contact angle on the IBSP-modified hydrogel became larger upon UV irradiation, which indicates an increase of oleophobicity of the IBSP-modified hydrogel. The wettability change in this liquid/liquid/solid system is attributed to the existence of IBSP on the hydrogel surface. Upon UV irradiation, the non-polar SP isomer on the hydrogel surface changed to a strong polarity MC form, which can be easily wetted by water as illustrated in Fig. 4a. Accordingly, once the IBSP-modified hydrogel was illuminated by UV light in an underwater environment, the surface of the hydrogel was rapidly wetted by water, which prevented the surface from being further wetted by oil, and thus gave rise to a large underwater oil contact angle (OCA) on the hydrogel. Owing to the reversible photo-responsive properties of IBSP, this process can be reversed by visible light illumination. Fig. 4b shows the reversible switching of the underwater OCA on the IBSP-modified hydrogel upon UV (150.6 ± 4.3°) and Vis (131.3 ± 3.1°) light irradiation, respectively. Moreover, the underwater oil (1,2-dichloroethane, 5 μL) adhesion force upon the IBSP-modified hydrogel can also be reversibly switched, along with the change in wettability.32 In the experiment, the adhesive force was defined as the force required to take the oil drop away from the substrate. An oil droplet was brought into contact with the surface of the hydrogel then allowed to leave in an underwater environment, and the adhesion force between the oil and the surface was recorded using a high-sensitivity micromechanical balance system.32 Force changes were recorded using a balance system when the hydrogel surfaces were controlled to come into contact with and leave an oil drop. An optical microscope lens and a charge-coupled device (CCD) camera system were also used to record images during the measurements. As shown in Fig. 4c, upon Vis light illumination, the underwater oil adhesion force upon the IBSP-modified hydrogel was about 40 mN, while after UV irradiation this force decreased by about 30 mN. The corresponding force–distance curves of the underwater oil adhesion force measurement before and after UV irradiation are shown in Fig. 4d and e, respectively. As a supplement, a series of snapshots corresponding to the four stages of the dynamic underwater oil adhesion force measurements are shown in Fig. S3,† which also represents the change of underwater oil adhesion force before and after UV irradiation. It is noted that each photo-responsive reversible switch process (Fig. 4b and 3c) can be carried out at least four times, suggesting that the superficial modified layer on the hydrogel is quite stable in an underwater environment and might be further used to manipulate the substances’ diffusion through the surface of the hydrogel.
To show that this modified layer of the hydrogel can indeed act as a “smart” barrier during the substances’ diffusion between the hydrogel and aqueous environment, we designed a small molecule release system. The mechanism is illustrated in Fig. 5a. After modification, the surface of the resulting hydrogel was covered with a photo-responsive superhydrophobic IBSP layer, which was able to prevent the surface from being wetted by water and suppressed the cargoes inside the bulk hydrogel to be released into the aqueous environment at a certain time. Once the modified hydrogel was illuminated by UV light, the surface of the modified hydrogel became much more easily wetted by water due to isomerization of the non-polar SP form to the polar MC form. Consequently, the diffusion rate of substances through the surface of the hydrogel was accelerated.
Fig. 5 Photo-responsive controlled release of fluorescein. (a) Schematic of the photo-responsive release system. (b) In situ UV/Vis absorption at 490 nm (the characteristic peak of fluorescein disodium (Fig. S4†)) as a function of time, monitoring the fluorescein released to the water environment from the hydrogel. (c) The average diffusion rate of fluorescein was deduced from (b) during the first hundred seconds. |
At first, fluorescein was embedded into the hydrogel network, and the rate of fluorescein being released from the hydrogel to aqueous solution was monitored using UV-Vis spectroscopy. The diffusion amount of fluorescein from the hydrogel as a function of time is shown in Fig. 5b, and the pristine hydrogel did not exhibit suppression of the fluorescein release, which is due to the size of the fluorescein molecule being much smaller than the loop size of the hydrogel network, resulting in free diffusion of fluorescein from the hydrogel. In contrast, the diffusion of fluorescein from IBSP-modified hydrogels was significantly blocked. When further illuminated by UV light (365 nm, 120 mW cm−2, 20 s) the diffusion rate of fluorescein from the IBSP-modified hydrogel was accelerated. Fig. 5c shows the average diffusion rate of fluorescein released from the hydrogel, deduced from Fig. 5b (first 100 s). The average diffusion rate of fluorescein from the IBSP-modified hydrogel to water is ∼0.088% s−1, while after UV irradiation, the average diffusion rate is ∼0.853% s−1, which is about 10 times faster. These results show the excellent photo-responsive controlled release properties of the IBSP-modified hydrogel, which indicates that the IBSP-modified layer on the hydrogel can indeed act as a “smart” barrier during substances’ diffusion across the surface of the hydrogel. As for the long period release of this system, the IBSP-modified hydrogel also exhibited good photo-responsive controlled release properties (Fig. S5 and S6†). The time that is taken to release 60% of the total amount of fluorescein for the IBSP-modified hydrogel has been delayed by more than one hour compared with the pristine hydrogel, and this time for the IBSP-modified hydrogel can be further accelerated using UV irradiation at the initial stage of the release process.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6sc04634g |
This journal is © The Royal Society of Chemistry 2017 |