Yu Chenc,
Weipeng Lu*ac,
Yanchuan Guo*abc,
Yi Zhuc,
Haojun Luc and
Yuxiao Wuc
aKey Laboratory of Photochemical Conversion and Optoelectronic Material, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing 100190, China
bUniversity of Chinese Academy of Sciences, Beijing 100049, China
cHangzhou Research Institute of Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Hangzhou 310018, China. E-mail: luweipeng@mail.ipc.ac.cn; Tel: +86-571-87853765
First published on 29th June 2018
As a degradable natural biomaterial, gelatin has good biocompatibility and nontoxicity, but gelatin is easily soluble in water which has limited its application. In order to solve this tough defect, superhydrophobic gelatin films (GSF) were prepared by first grafting silica nanoparticles onto gelatin films and then modifying silica nanoparticles with a fluorosilane coupling agent (FAS). Fourier transform infrared spectroscopy (FTIR), scanning electron microscopy (SEM), a particle size analyzer, a contact angle instrument (CA), X-ray photoelectron spectroscopy (XPS), a universal materials tester and an Incucyte™ Zoom system were used to characterize the morphology, molecular interactions, superhydrophobic performance, and cytotoxicity. Results show that GSF300 modified by silica nanoparticles with a particle size of 303 nm has the largest contact angle (158.6°). At the same time, the contact angle is still more than 150° after 48 hours of infiltration in water. These results indicate that GSF300 has strong long-term water resistance. In addition, GSF300 has good mechanical strength, durability and nontoxicity. Therefore, such a durable, robust and superhydrophobic film has good potential applications in various functional biomedical aspects.
Due to the easy water absorption in wet environment, gelatin needs to have strong water resistance and superhydrophobicity. In order to solve this intractable problem, researchers have made a lot of attempts, such as blending, grafting. For example, S. Afshar et al. developed a hydrophobic biodegradable nanocomposite gelatin films by blending starch and graphene oxide, and the static contact angle was 112.04° ± 4.85, which was 40° greater than pure gelatin film.7 C. Shi et al. prepared a new gelatin film modified by starch-based ester Starch-EDTAD-NHS (SEN), and the contact angle was found to increase from 77.8° to 126.7° with increasing concentration of SEN.8 Besides, gelatin/zein nanofiber films by hybrid electrospinning were reported by Deng et al., and when the weight ratio was 1:1, the contact angle reached the 118°, resulting in a good solvent resistance against water.9 From the above description, we can find that these methods can improve the hydrophobicity of gelatin to some extent. However, no reports have yet provided superhydrophobic gelatin films. In addition, it is important to note that gelatin, as a protein macromolecule, has many hydrophilic groups on the surface, such as amino and hydroxyl. So, simple blending or grafting can hardly guarantee the hydrophobic properties for a long time.
Inspired with nature surface, such as lotus leaves, water strider legs, and cicada wings,10,11 superhydrophobic surfaces are characterized by a static water contact angle (WCA) above 150° and a sliding angle (SA) less than 10°, by definition.12,13 Due to the unique water-repellent property, superhydrophobic materials have gained tremendous interest, which has widespread applications in self-cleaning,14,15 anti-icing,16 metal anti-corrosion,17 separation of oil and water,18 especially in biomedical fields such as anti-sticking of protein, cells, and/or bacteria,19–21 and drug release.22,23 Therefore, the study of superhydrophobic gelatin materials is of great application value.
Herein, in order to realize the superhydrophobicity of gelatin films, suitable amount of formaldehyde and glycerol were firstly added to the film as crosslinkers and plasticizers respectively to improve its mechanical properties. Then we prepared silica nanoparticles with different particle sizes by Stöber24 sol–gel process. Next, the obtained silica nanoparticles were deposited on the modified gelatin film to improve the surface roughness, further functionalized with fluoroalkylsilane (FAS) in an ethanolic solution to obtain superhydrophobic gelatin film. As far as we know, this was the first time to prepare superhydrophobic gelatin film material. More importantly, the super hydrophobic gelatin films have good mechanical strength, durability and nontoxicity, which greatly expands the biological application of superhydrophobic material. The results are summarized and discussed in the following sections.
Sample | NH3·H2O/TEOS (volume ratio), with constant volume ratio of C2H5OH/TEOS = 33 | Diameter/nm |
---|---|---|
S1 | 1.3 | 127 |
S2 | 1.5 | 225 |
S3 | 2.0 | 303 |
S4 | 2.7 | 447 |
During the preparation of gelatin films, most hydrophilic groups such as amino group and carboxyl group move inward and form hydrogen bonds with internal hydrophilic groups, and at this point, the surface of the films are some hydrophobic groups, such as aliphatic chain and aryl groups.25 It is worth noting that the carbonyl group is generally on the hydrophobic side due to trans structure of the peptide bond. When silica nanoparticles are deposited on the surface of the film, it's very likely that a large number of hydroxyl groups on the silica nanoparticles can form abundant hydrogen bonds with the carbonyl group on the surface of the gelatin with hydroxyl groups acting as H donors and carbonyl groups acting as H acceptors. Next, due to the hydrolysis of the Si–OC2H5 of FAS in acid condition, the obtained hydrolyzed fluorosilane can condense with hydroxyl groups of silica nanoparticles. Finally, the superhydrophobic gelatin-based films (GSF) are formed by above process.
Fig. 1 FESEM top-view images of various films. (a) GS100, (b) GS200, (c) GS300, (d) GS400, (e) GSF100, (f) GSF200, (g) GSF300, and (h) GSF400. |
FTIR spectras of pure gelatin film, GE, GS300 and GSF300 are showed in Fig. 2a–d respectively. In Fig. 2a, the spectrum of pure gelatin depicts characteristic peaks at 1629 cm−1, 1531 cm−1 and 1237 cm−1, which corresponds to amide I, amide II and amide III respectively. The amide I band is dominantly attributed to the CO stretching vibrations. The amide II and III bands are due to the N–H bending vibrations and C–N stretching vibrations respectively.26 As shown in Fig. 2b, the peak situates around 1037 cm−1 might be related to glycerol.27,28 Besides, the characteristic peak positions at 1630 cm−1, 1533 cm−1 and 1238 cm−1 are shifted slightly higher compared with the pure gelatin, which may be caused by the occurrence of the Schiff base reactions between the –NH2 of the gelatin and Formaldehyde.29,30 The spectrum in Fig. 2c shows three significant peaks of silica nanoparticles. The strongest peak is at 1068 cm−1, which is due to the asymmetric stretching vibration of Si–O–Si bonds in the silica nanoparticles. Another peak appearing at 792 cm−1 is associated with the bending mode of Si–O–Si bonds. In addition, a weak absorption peak appears at 950 cm−1, which is caused by the presence of Si–OH bonds. In the Fig. 2d, two tiny peaks at 1201 cm−1 and 1144 cm−1 superimposed on the left shoulder of the Si–O–Si peak at 1038 cm−1 are due to the stretching vibration of C–F bonds and C–Si–O bond that arises the link between FAS molecules and the silica nanoparticles.31
In addition, XPS was selected to further explore the atomic composition of the film surface. As shown in Fig. 3a and b, the pure gelatin film and the GE have the same three peaks at 288 eV, 400 eV and 532 eV, which can be confirmed to belong to C1 s, N1 s and O1 s respectively. And this is consistent with their compositions. In the Fig. 3c, the significant decrease of the C1 s peak at 288 eV and almost disappearance of the N1 s peak at 400 eV are both caused by the silica nanoparticles coated on the GS300. Furthermore, the characteristic peaks of Si2 p at 103 eV and Si2 s at 154 eV are also detected. Next, the Fig. 3d shows that the C1 s peak at 285 eV, 291 eV and 293 eV are undoubted ascribed to CH2, CF2 and CF3 functional groups, respectively. In addition, the peaks at 688 eV, 834 eV and 862 eV are also observed on the surface of GSF300, which can be determined to be caused by CF2, CF3 of FAS. So XPS characterization confirms that the silica nanoparticles and FAS molecules are successfully bonded to the gelatin film, which is consistent with the result of FTIR spectra.
Fig. 3 XPS spectra of the surface of the films. (a) Pure gelatin film, (b) GE, (c) GS300, (d) GSF300. |
As an extremely hydrophilic substance, gelatin has abundant hydrophilic groups. But as shown in Fig. 4a, the instantaneous WCA is 102.4° ± 1.2, showing a certain hydrophobicity. As we mentioned above, during the preparation of gelatin films, most hydrophilic groups move inward and form hydrogen bonds with internal hydrophilic groups, and the surface of the films is some hydrophobic groups. Therefore, the instantaneous WCA of the gelatin film is greater than 90° and exhibits a certain hydrophobicity. But pure gelatin film has strong water absorbability and can absorb water after a few seconds. The WCA of GE is 113° ± 0.9, which is 10° larger than the pure gelatin film. This is due to the crosslinking effect of the formaldehyde and the amino group of the gelatin molecule, thus the hydrophobicity of the film is improved. Meanwhile, the Fig. 4a also shows that the WCAs of the films GS100, GS200, GS300 and GS400 are 18.4° ± 1.3, 15.4° ± 1.0, 14.3° ± 1.1 and 17.6° ± 1.0, respectively. This is attributed to the presence of a large number of hydroxyl groups on the surface of the silica nanoparticles, so the water droplets can be completely spread over the films.32 The WCAs of the films GSF100, GSF200, GSF300 and GSF400 are found to be 152.3° ± 0.1, 156.6° ± 1.8, 158.6° ± 1.2 and 151.9° ± 1.0, respectively. It can be seen that all the GSF exhibit high water repellency. As shown in Fig. 4b, the superhydrophobicity of GSF was further characterized in regards to the hysteresis of water contact angle which was measured by SA. The SAs of the films GSF100, GSF200, GSF300 and GSF400 are 10.8° ± 0.5, 6.3° ± 0.8, 5.6° ± 0.5 and 9.0° ± 0.9, respectively. The above results show that the WCA of GSF is more than 150° and the SA is less than 10°, which accords with the definition of superhydrophobicity. In addition, Fig. 4b indicates that the WCAs increase from 152.3° ± 0.1 to 158.6° ± 1.2 by increasing the size of the silica nanoparticles modified with FAS from 127 to 303 nm. However, as the size increases further to 447 nm, the water contact angle decreases to 151.9°. We find that the obtained results are similar with the observations by Brassard et al.31 In Brassard et al. studies, the sizes of nanoparticles (40–300 nm) are related to roughness. As the particle size increases, the surface roughness increases, which leads to the increase of contact angle. Then we also tested the relationship between the amount of silica nanoparticles loaded and the WCA. From Fig. 4c, we can see that the WCA increases with the increase of the amount of silicon nanoparticles, when the mass ratio of silica nanoparticles to GE reaches 0.3, the WCA is more than 150°, which shows superhydrophobic property. This can be explained that there is a correlation between the roughness and the silica nanoparticles as well as the WCA and roughness, that is, with the increase of the loading amount of silica nanoparticles, the roughness of the film increases continuously, which leads to the increase of WCA. When the silica nanoparticles/GE ratio of GSF is about 0.3, the roughness of the film reaches the peak value, so, when the mass ratio of silicon nanoparticles to GE is greater than 0.3, the roughness of the film will not continue to increase, resulting in no significant change in WCA. Therefore, 0.3 is the best silica nanoparticles/GE ratio for preparing superhydrophobic GSF. Next, we took the GSF300 as an example to test the water resistance by immersing film into water. From Fig. 4d, it can be seen that after 7 day of immersing, the contact angle of the GSF300 decreases from 158.6° ± 1.2 to 143.7° ± 1.1, and still remains excellent water resistance.
Table 2 exhibits tensile strength, and elongation at break of the pure gelatin, GE, GS300 and GSF300. The tensile strength of GE increases by 8% compared to the pure gelatin film. This behavior can be assigned to the crosslinking effect between the aldehyde group and the amino group of the gelatin molecule.33 What's more, due to the formation of a dense and stable coating on the surface of the gelatin film by silicon nanoparticles, the tensile strength of GS300 and GSF300 increases by 98% and 51%, respectively. Meanwhile, the elongation at break of GE, GS300 and GSF300 increased by 153%, 90% and 122%, respectively compared to the pure gelatin film. This finding can be explained by the possibility that glycerol molecules can form hydrogen bonds with gelatin molecules, which can destroy the hydrogen bonds between and within the molecular chains of gelatin, weaken the interaction within the gelatin molecules, enhance the elasticity and increase the elongation at break.34,35 Based on above datas, it demonstates that the GSF300 has good mechanical properties. Furthermore, it is worth noting that after 7 days of immersion in water, the GSF300 remains in its original shape, but some swelling occurs. The tensile strength, and elongation at break is 18.24 ± 8.35 and 40.18 ± 7.44, respectively. Besides, to prove that the GSF has a mechanical durable superhydrophobic surface, abrasion and peeling tests of GSF300 were carried out. Fig. 5a shows the plot of the WCA of superhydrophobic paper as a function of abration times, and it indicates that the WCA decreases to 150° after 5 abration times. Mechanical stability of the GSF300 was also evaluated via tape peeling. As shown in Fig. 5b, repeated peeling with the new tape results in gradual decrease of the contact angle, and after peeling for 5 times, the film is still superhydrophobic. From the above tests, it demonstrates that the obtained GSF300 has good mechanical stability.
Thickness/mm | Tensile strength/MPa | Elongation/% | |
---|---|---|---|
Pure gelatin film | 0.22 ± 0.01 | 55.60 ± 0.09 | 1.99 ± 0.09 |
GE | 0.20 ± 0.02 | 60.38 ± 4.94 | 5.04 ± 0.45 |
GS300 | 0.19 ± 0.04 | 110.01 ± 7.02 | 3.78 ± 0.67 |
GSF300 | 0.19 ± 0.01 | 83.96 ± 12.0 | 4.42 ± 0.09 |
As potential implantable materials, we hope that the obtained superhydrophobic gelatin films need to have good biocompatibility and nontoxicity. Therefore, the proliferation of GSF300 and pure gelatin film were studied by real-time monitoring of human fibroblast cell lines (hFOB 1.19) using an Incucyte™ Zoom microscope. As shown in Fig. 6, time-lapse imaging of the blank control shows a standard growth curve up to 39% cell confluence level by day 7, while the pure gelatin film reaches 69% cell confluence level by day 7. It indicates that the pure gelatin film efficiently promotes the cell proliferation. Meanwhile, the growth curve of GSF300 was a little higher than the blank control, which represents that the GSF300 has certain promoting effect on cell proliferation. The cytotoxicity was expressed by the relative growth rate (RGR, %) as follow in Table 3. It is found that all the relative growth rates are more than 100%, corresponding to the cytotoxicity level of 0 per the standard (Table S1, ESI†). In addition, as shown in Fig. 7, the human fibroblasts cells cultured in extraction media from the pure gelatin film and GSF300 are marked by a green phase object mask via the software of Incucyte™ Zoom, which display healthy spindle-like or star-like shape, and the amount of cells rised with the extension of culture time, suggesting that GSF300 imposes no suppression on the growth of cells.
Fig. 6 Real-time cell confluence study in human fibroblast cell lines (hFOB 1.19). The cell population was monitored for 168 h using an Incucyte™ Zoom system in an incubator (5% CO2 and 37 °C). |
1 day | 3 day | 5 day | 7 day | ||
---|---|---|---|---|---|
GSF300 | GRG (%) | 122 | 133 | 116 | 104 |
Cytotoxicity level | 0 | 0 | 0 | 0 | |
Pure gelatin film | GRG (%) | 156 | 164 | 181 | 174 |
Cytotoxicity level | 0 | 0 | 0 | 0 |
Fig. 7 Cell morphology of GSF300 and pure gelatin film at point of 1, 3, 5, 7 day. Scale bar: 200 μm. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra04066d |
This journal is © The Royal Society of Chemistry 2018 |