# Tunable Structures and Properties of Electrospun Regenerated Silk Fibroin Mats Annealed in Water Vapor at Different Times and Temperatures

Authors: Xiangyu Huang; Suna Fan; Alhadi Ibrahim Mohammed Altayp; Yaopeng Zhang; Huili Shao; Xuechao Hu; Minkai Xie; Yuemin Xu
Journal: Journal of Nanomaterials
 (2014)

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## Abstract

Regenerated silk fibroin (SF) mats were fabricated using electrospinning technique, followed by mild water vapor annealing to effectively tune the structures and improve the mechanical properties of the mats at different annealing times and temperatures. The breaking strength and the breaking energy of the mats treated with water vapor at 65°C for 12 h reached 6.0 MPa and 171.7 J/kg, respectively. The conformational transition of the SF mats was significantly influenced by the treating temperature, while the influence of time was comparatively limited. The influence is consistent with the time-temperature equivalent principle and would be helpful for the preparation of water-vapor-annealed silk-based biomaterials for various applications.


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## Body

## 1. Introduction

Silk fibroin (SF), the main component of natural silks fromBombyx mori silkworms, has contributed to the outstanding mechanical properties, excellent biocompatibility, and controllable biodegradability of silks [1]. Recently, many SF-based materials have been developed in different forms for biomedical applications, such as scaffolds, hydrogels, porous sponges, tubes, microspheres, and fibers [2–10]. In these forms of SF, electrospun SF mats exhibit similar morphological structure to the native extracellular matrix (ECM), which may greatly promote the cell attachment and proliferation on this material [11, 12].Before the electrospun SF mats are applied in tissue engineering, they always require certain types of posttreatment to enhance their mechanical properties and stability in water. Most of the reported posttreatment methods are based on the chemical agents, especially the aqueous alcoholic solutions [13, 14]. However, the organic solvents may cause potential negative effects on human bodies. The soaking process may also lead to the loss of embedded drugs, thereby limiting the applications of SF mats in drug-delivery fields [15]. Recently, a posttreatment method using water vapor annealing to induce the conformational transition in SF has been investigated due to its mild processing conditions and elimination of organic solvents. Min et al. [16] proved the mild characteristic of water vapor treatment through investigating cell behavior on water-vapor-treated SF nanofibers. Jeong et al. [17] confirmed that water vapor could successfully stabilize the SF matrices as alcohol vapor. However, the results of water vapor treatment may significantly depend on the treating time and the temperature. Therefore, in order to control the structures and properties of SF via water vapor annealing, it is necessary to investigate the detailed influence of temperature and time on SF. Hu et al. reported a method of temperature-controlled water vapor annealing to control the structures and properties of SF films [18]. However, the detailed influences of annealing time and temperature on SF mats are rarely reported. Moreover, the average diameter of the electrospun fibers is much smaller than the thickness of films, so that the influences of posttreatment process on the mats may be significantly different from those on the films.In this study, we provide an effective and easy-conducting approach to fabricate electrospun regenerated SF mats with tunable structures through water vapor annealing at different times and temperatures. Improved mechanical properties are desired to be achieved for further biomedical applications.


## 2. Experimental

### 2.1. Materials

B. moricocoons produced in Zhejiang Province, China, were used as raw material to extract SF. Analytical-grade sodium carbonate (Na2CO3) and lithium bromide (LiBr) were obtained from Sinopharm Chemical Reagent Co., Ltd. (Shanghai, China) and Zhongli Industrial Co., Ltd. (Shanghai, China), respectively. Cellulose semipermeable membranes with a molecular weight cutoff of 14000±2000 D were purchased from Yuanju Co., Ltd. (Shanghai, China).


### 2.2. Preparation of Silk Fibroin and Electrospun Mats

TheB. mori cocoons were boiled twice in 0.5 wt% Na2CO3 solution to remove sericin. Degummed silks were then dissolved in 9.0 M LiBr aqueous solution at 40°C for 2 h and further dialyzed in deionized water at 10°C for 3 days according to the established procedures [19]. Ultimately, a purified 33 wt% SF solution was obtained through concentrating at 10°C.The SF mats were fabricated by electrospinning using the purified 33 wt% SF solution and were randomly collected on a grounded collector with a spinneret-to-collector distance of 10 cm. During electrospinning, a high voltage of 20 kV was applied and a flow rate of spinning dope was maintained at 1.2 mL/h. The details of this process can be found in our previous literature [20].


### 2.3. Water Vapor Annealing on SF Mats

A constant temperature and humidity chamber (HCP 108, Memmert GmbH + Co. KG, Germany) was used in the posttreatment process. Relative humidity (RH) in the chamber was fixed at90±1%. In the temperature-controlled series, samples were treated with water vapor for 3 h at different temperatures: 45, 55, 65, and 75°C. In the time-controlled series, samples were treated with water vapor at 65°C for different times: 0.5, 1, 3, 6, 9, 12, 15, 18, and 24 h. After posttreatment, samples were dried in a sealed container with desiccant for 48 h before further characterization.


### 2.4. Characterization

The morphology of the SF mats was examined by scanning electron microscopy (SEM; JSM-5600LV, JEOL, Japan). Diameters of the electrospun fibers were measured directly from their SEM images using Image Tool software based on at least 100 fibers.The secondary structure of the electrospun fibers was characterized by a Raman spectrometer (LabRAM-1 B, Dilor, France) at a 1 cm−1 resolution. All samples were irradiated by a He-Ne laser with a wavelength of 632.8 nm. Spectra were recorded in the range of 900–1800 cm−1.Wide angle X-ray diffraction (WAXD) patterns were obtained at the BL15U1 beamline in Shanghai Synchrotron Radiation Facility (SSRF) at a wavelength of 0.07746 nm. The sample-to-detector distance was calibrated using lanthanum hexaboride (LaB6) as a standard to 187 mm. Each specimen was exposed for 30 s and the corresponding background was recorded simultaneously. Data analysis was carried out by FIT2D software. Then a method reported previously was applied to calculate the crystallinity of the SF mats according to the diffractograms [21].An Instron 5969 material testing instrument (Instron Co., USA) was applied to investigate the mechanical properties of the mats at25±5°C and 50±5% RH. Thickness of the samples was tested by a CH-1-S thickness gauge (Shanghai Liuling Instruments Co., China). All samples were cut into 5 mm × 40 mm pieces for tensile test, which was conducted with an extension rate of 1 mm/min and a gauge length of 20 mm. At least 10 specimens were tested for each mat sample.


## 2.1. Materials

B. moricocoons produced in Zhejiang Province, China, were used as raw material to extract SF. Analytical-grade sodium carbonate (Na2CO3) and lithium bromide (LiBr) were obtained from Sinopharm Chemical Reagent Co., Ltd. (Shanghai, China) and Zhongli Industrial Co., Ltd. (Shanghai, China), respectively. Cellulose semipermeable membranes with a molecular weight cutoff of 14000±2000 D were purchased from Yuanju Co., Ltd. (Shanghai, China).


## 2.2. Preparation of Silk Fibroin and Electrospun Mats

TheB. mori cocoons were boiled twice in 0.5 wt% Na2CO3 solution to remove sericin. Degummed silks were then dissolved in 9.0 M LiBr aqueous solution at 40°C for 2 h and further dialyzed in deionized water at 10°C for 3 days according to the established procedures [19]. Ultimately, a purified 33 wt% SF solution was obtained through concentrating at 10°C.The SF mats were fabricated by electrospinning using the purified 33 wt% SF solution and were randomly collected on a grounded collector with a spinneret-to-collector distance of 10 cm. During electrospinning, a high voltage of 20 kV was applied and a flow rate of spinning dope was maintained at 1.2 mL/h. The details of this process can be found in our previous literature [20].


## 2.3. Water Vapor Annealing on SF Mats

A constant temperature and humidity chamber (HCP 108, Memmert GmbH + Co. KG, Germany) was used in the posttreatment process. Relative humidity (RH) in the chamber was fixed at90±1%. In the temperature-controlled series, samples were treated with water vapor for 3 h at different temperatures: 45, 55, 65, and 75°C. In the time-controlled series, samples were treated with water vapor at 65°C for different times: 0.5, 1, 3, 6, 9, 12, 15, 18, and 24 h. After posttreatment, samples were dried in a sealed container with desiccant for 48 h before further characterization.


## 2.4. Characterization

The morphology of the SF mats was examined by scanning electron microscopy (SEM; JSM-5600LV, JEOL, Japan). Diameters of the electrospun fibers were measured directly from their SEM images using Image Tool software based on at least 100 fibers.The secondary structure of the electrospun fibers was characterized by a Raman spectrometer (LabRAM-1 B, Dilor, France) at a 1 cm−1 resolution. All samples were irradiated by a He-Ne laser with a wavelength of 632.8 nm. Spectra were recorded in the range of 900–1800 cm−1.Wide angle X-ray diffraction (WAXD) patterns were obtained at the BL15U1 beamline in Shanghai Synchrotron Radiation Facility (SSRF) at a wavelength of 0.07746 nm. The sample-to-detector distance was calibrated using lanthanum hexaboride (LaB6) as a standard to 187 mm. Each specimen was exposed for 30 s and the corresponding background was recorded simultaneously. Data analysis was carried out by FIT2D software. Then a method reported previously was applied to calculate the crystallinity of the SF mats according to the diffractograms [21].An Instron 5969 material testing instrument (Instron Co., USA) was applied to investigate the mechanical properties of the mats at25±5°C and 50±5% RH. Thickness of the samples was tested by a CH-1-S thickness gauge (Shanghai Liuling Instruments Co., China). All samples were cut into 5 mm × 40 mm pieces for tensile test, which was conducted with an extension rate of 1 mm/min and a gauge length of 20 mm. At least 10 specimens were tested for each mat sample.


## 3. Results and Discussion

### 3.1. Morphology and Nanostructure of SF Mats

Figure1 shows typical morphologies and diameter distribution histograms of the electrospun SF mats which were obtained by water vapor annealing at different conditions. As-spun mat was also shown in the figure for comparison. All water-vapor-annealed samples and the as-spun sample present smooth surface morphologies. When compared with the alcohol-treated or postdrawn SF mats with rough surface [20, 22], the water-vapor-annealed samples with smooth surface show obvious advantages. This suggests that the water vapor annealing is quite a mild posttreating method which would not cause severe damages to the fiber surface. And the diameter distribution histograms show that the diameters of fibers increase with the temperature. This is probably attributed to the significant swelling of SF fibers in water vapor during annealing.SEM images and diameter distribution histograms of water-vapor-annealed electrospun SF mats under different conditions: (a) as-spun; (b) 55°C-3 h; (c) 65°C-3 h; and (d) 65°C-9 h.
(a)
(b)
(c)
(d)


### 3.2. Secondary Structures of SF Mats

The secondary structure transition of the SF fibers occurs in the water vapor annealing process. Figure2 shows the Raman spectra of the SF mats posttreated at different times and temperatures. The assignments of the major bands in the spectra were based on literatures [23, 24]. Spectra of the as-spun fibers exhibit obvious bands relate to α-helix (1103 cm−1), random coil (1251, 946 cm−1), and β-turn (1675 cm−1), which are somehow obscure in the posttreated samples. In addition, intense bands at 1666 cm−1, 1230 cm−1, and 1085 cm−1 which correspond to β-sheet conformation are observed in the spectra of the posttreated fibers. The varied intensities of the characteristic peaks suggest that the time and temperature definitely affect the structural transition of SF mats in different degrees.Raman spectra of electrospun SF fibers: (a) samples treated with water vapor at 65°C for different times: (A) as-spun, (B) 0.5 h, (C) 3 h, (D) 9 h, and (E) 24 h; (b) samples treated with water vapor for 3 h at different temperatures: (A) 45°C, (B) 55°C, (C) 65°C, and (D) 75°C.
(a)
(b)To further investigate the relationships between secondary structure of the SF mats and annealing condition, we conducted the quantitative analysis in amide I region of Raman spectra. As shown in Figure3, with prolonged time or raised temperature, the β-sheet content significantly increases accompanied with decreased contents ofα-helix (time > 0.5 h), random coil, and β-turn conformation. This suggests that SF mats with desired secondary structures can be achieved through controlling a single variable of either time or temperature during water vapor annealing. The SF mats annealed at 75°C for 3 h (37.1%) show an even higher β-sheet content than the mats treated at 65°C for 24 h (34.3%). This indicates that the increase of temperature may be more effective than time in inducing the conformation transition of SF. Apart from high temperature, water molecule is another indispensable factor in the formation of β-sheets. As proved by Hu et al. [25], the water-silk structure possesses a lower glass transition temperature than that of the pure dry silk. Therefore, during the water vapor annealing process, the high content of free water molecules may weaken the original intermolecular bonding force within SF and decrease the required energy for movements of amino acids [26]. Moreover, the high ambient temperature could provide more energy for the molecular movements. As a result, the high-temperature water vapor annealing successfully induces the conformational transition of SF. Mo et al. [27] also found that the formation of β-sheets in SF relates to the dissociation of hydrogen bonds between water and peptides and reformation of stronger hydrogen bonds between peptides themselves. Accordingly, we may be able to control the microstructure of SF materials accurately in a high-humidity environment by simply adjusting the ambient temperature.Quantitative analysis of the secondary structure components of electrospun SF fibers treated with water vapor at different conditions: (a) annealed at 65°C for different times; (b) annealed for 3 h at different temperatures.
(a)
(b)


### 3.3. Crystalline Structure of SF Mats

It has been reported that silk fibroin from theB. mori contains two forms of crystalline modifications, silk I and silk II,as well as the amorphous structure. Moreover, silk II is commonly considered to be constituted of β-sheets [28]. To further investigate the effects of water vapor annealing temperature and time on SF fibers, WAXD diffractograms (Figure 4) were obtained to analyze the crystalline structure of SF according to Asakura’s assignments [29]. Regardless of the temperature, all samples posttreated for different times (Figure 4(a)) exhibit apparent diffraction peaks atD-spacing of 0.226, 0.36, 0.43 nm which correspond to the reflection of silk II structure [30, 31]. Meanwhile, the characteristic reflection of amorphous structure atD-spacing of 0.407 nm is observed in the as-spun fibers, while it is absent in water-vapor-annealed fibers. It indicates that the crystallization rate of SF during water vapor annealing at 65°C is quite rapid. This relationship can be seen more obviously from Figure 5(a). During water vapor annealing at 65°C, the crystallinity of SF mats improves promptly from 35.5% to 47.3% within 1 h. However, when the annealing time prolongs from 1 to 24 h, the crystallinity keeps improving gradually and further reaches 52.2%. It can be concluded that time is an important factor to control the crystallization of SF mats during water vapor annealing and the rise of annealing time leads to a higher crystallinity. Nevertheless, the influence of time is rather limited, especially under a high ambient temperature.WAXD diffractograms of electrospun RSF fibers: (a) samples treated with water vapor at 65°C for different times: (A) as-spun, (B) 0.5 h, (C) 1 h, (D) 3 h, (E) 6 h, (F) 9 h, (G) 12 h, (H) 15 h, (I) 18 h, and (J) 24 h; (b) samples treated with water vapor for 3 h at different temperatures: (A) 45°C, (B) 55°C, (C) 65°C, and (D) 75°C.
(a)
(b)Crystallinities of electrospun RSF mats treated with water vapor: (a) at 65°C for different times; (b) for 3 h at different temperatures.
(a)
(b)Figure4(b) shows the influence of temperature on SF mats during water vapor annealing. When the annealing time was fixed at 3 h, the characteristic reflection of silk I structure atD-spacing of 0.72 nm [32, 33] can be observed on the diffractograms at 45 and 55°C. At higher temperatures of 65 and 75°C, clear changes of the diffractograms occur. Not only silk I reflection at 0.72 nm disappears, but also silk II reflections become more intense with the increasing annealing temperature. It can be found from Figure 5(b) that the crystallinity of SF mats increases almost linearly from 45.1% to 51.5% with raising temperature from 45 to 75°C. The above results suggest that the temperature in water vapor annealing process could significantly influence the crystallization behavior of SF mats.


### 3.4. Mechanical Properties of SF Mats

The mechanical properties of the SF mats treated with water vapor at different temperatures and times are shown in Figure6. It can be seen from Figure 6(a) that the breaking strength of the SF mats is greatly improved after annealing in water vapor at 65°C and gradually increases with prolonged treating time. When temperature rises, a more significant increasing trend of breaking strength can be found in Figure 6(b). The two curves of breaking strength in Figure 6 present great consistency with the corresponding crystallinity changes shown in Figure 5. This indicates that the potential SF materials with tunable properties and structures can be achieved by controlling the annealing time and temperature. Although the water-vapor- annealed SF mats do not have mechanical properties comparable to those of the posttreated mats via uniaxial drawing in ethanol solution [20], the moderate characteristic of water vapor annealing is still quite attractive. The mild conditions would be favorable for drug loading and preparation of SF materials with enhanced and uniform mechanical properties [34]. When the mats are annealed at 65°C for 15 h, the breaking stress is improved to 6.0 MPa, which is about 4 times of the as-spun mats (1.8 MPa) [20]. The mats with similar properties could also be achieved within 3 h while raising the temperature to 75°C. This well exhibits the time-temperature equivalence, which may be attributed to the more energy that SF molecules absorbed for conformational transition in a longer annealing period or at a higher annealing temperature. From another aspect, the motion of SF molecules is time dependent. The longer time could result in a more complete structure transition, namely, an increased content of the stable β-sheet structure in SF.Breaking strength and breaking energy of electrospun RSF mats treated with water vapor: (a) at 65°C for different times; (b) for 3 h at different temperatures.
(a)
(b)However, the breaking energy of the mats changes irregularly with annealing condition. It increases with annealing time or temperature first but decreases at an annealing time longer than 15 h in Figure6(a) or at a temperature higher than 65°C in Figure 6(b). This may be attributed to the microstructure changes in SF fibers. With increasing treating time or temperature, the transformation from silk I to silk II is performed more completely. As the primary antiparallel β-sheet structure in silk II structure is more stable than the characterized β-turn type in silk I [35], the SF mats present a higher breaking elongation with increasing β-sheet content. When the crystallinity of SF mats is higher than 50%, the samples with low breaking strain become much brittle and the breaking energy decreases. This phenomenon is similar to the results of SF films [18].


## 3.1. Morphology and Nanostructure of SF Mats

Figure1 shows typical morphologies and diameter distribution histograms of the electrospun SF mats which were obtained by water vapor annealing at different conditions. As-spun mat was also shown in the figure for comparison. All water-vapor-annealed samples and the as-spun sample present smooth surface morphologies. When compared with the alcohol-treated or postdrawn SF mats with rough surface [20, 22], the water-vapor-annealed samples with smooth surface show obvious advantages. This suggests that the water vapor annealing is quite a mild posttreating method which would not cause severe damages to the fiber surface. And the diameter distribution histograms show that the diameters of fibers increase with the temperature. This is probably attributed to the significant swelling of SF fibers in water vapor during annealing.SEM images and diameter distribution histograms of water-vapor-annealed electrospun SF mats under different conditions: (a) as-spun; (b) 55°C-3 h; (c) 65°C-3 h; and (d) 65°C-9 h.
(a)
(b)
(c)
(d)


## 3.2. Secondary Structures of SF Mats

The secondary structure transition of the SF fibers occurs in the water vapor annealing process. Figure2 shows the Raman spectra of the SF mats posttreated at different times and temperatures. The assignments of the major bands in the spectra were based on literatures [23, 24]. Spectra of the as-spun fibers exhibit obvious bands relate to α-helix (1103 cm−1), random coil (1251, 946 cm−1), and β-turn (1675 cm−1), which are somehow obscure in the posttreated samples. In addition, intense bands at 1666 cm−1, 1230 cm−1, and 1085 cm−1 which correspond to β-sheet conformation are observed in the spectra of the posttreated fibers. The varied intensities of the characteristic peaks suggest that the time and temperature definitely affect the structural transition of SF mats in different degrees.Raman spectra of electrospun SF fibers: (a) samples treated with water vapor at 65°C for different times: (A) as-spun, (B) 0.5 h, (C) 3 h, (D) 9 h, and (E) 24 h; (b) samples treated with water vapor for 3 h at different temperatures: (A) 45°C, (B) 55°C, (C) 65°C, and (D) 75°C.
(a)
(b)To further investigate the relationships between secondary structure of the SF mats and annealing condition, we conducted the quantitative analysis in amide I region of Raman spectra. As shown in Figure3, with prolonged time or raised temperature, the β-sheet content significantly increases accompanied with decreased contents ofα-helix (time > 0.5 h), random coil, and β-turn conformation. This suggests that SF mats with desired secondary structures can be achieved through controlling a single variable of either time or temperature during water vapor annealing. The SF mats annealed at 75°C for 3 h (37.1%) show an even higher β-sheet content than the mats treated at 65°C for 24 h (34.3%). This indicates that the increase of temperature may be more effective than time in inducing the conformation transition of SF. Apart from high temperature, water molecule is another indispensable factor in the formation of β-sheets. As proved by Hu et al. [25], the water-silk structure possesses a lower glass transition temperature than that of the pure dry silk. Therefore, during the water vapor annealing process, the high content of free water molecules may weaken the original intermolecular bonding force within SF and decrease the required energy for movements of amino acids [26]. Moreover, the high ambient temperature could provide more energy for the molecular movements. As a result, the high-temperature water vapor annealing successfully induces the conformational transition of SF. Mo et al. [27] also found that the formation of β-sheets in SF relates to the dissociation of hydrogen bonds between water and peptides and reformation of stronger hydrogen bonds between peptides themselves. Accordingly, we may be able to control the microstructure of SF materials accurately in a high-humidity environment by simply adjusting the ambient temperature.Quantitative analysis of the secondary structure components of electrospun SF fibers treated with water vapor at different conditions: (a) annealed at 65°C for different times; (b) annealed for 3 h at different temperatures.
(a)
(b)


## 3.3. Crystalline Structure of SF Mats

It has been reported that silk fibroin from theB. mori contains two forms of crystalline modifications, silk I and silk II,as well as the amorphous structure. Moreover, silk II is commonly considered to be constituted of β-sheets [28]. To further investigate the effects of water vapor annealing temperature and time on SF fibers, WAXD diffractograms (Figure 4) were obtained to analyze the crystalline structure of SF according to Asakura’s assignments [29]. Regardless of the temperature, all samples posttreated for different times (Figure 4(a)) exhibit apparent diffraction peaks atD-spacing of 0.226, 0.36, 0.43 nm which correspond to the reflection of silk II structure [30, 31]. Meanwhile, the characteristic reflection of amorphous structure atD-spacing of 0.407 nm is observed in the as-spun fibers, while it is absent in water-vapor-annealed fibers. It indicates that the crystallization rate of SF during water vapor annealing at 65°C is quite rapid. This relationship can be seen more obviously from Figure 5(a). During water vapor annealing at 65°C, the crystallinity of SF mats improves promptly from 35.5% to 47.3% within 1 h. However, when the annealing time prolongs from 1 to 24 h, the crystallinity keeps improving gradually and further reaches 52.2%. It can be concluded that time is an important factor to control the crystallization of SF mats during water vapor annealing and the rise of annealing time leads to a higher crystallinity. Nevertheless, the influence of time is rather limited, especially under a high ambient temperature.WAXD diffractograms of electrospun RSF fibers: (a) samples treated with water vapor at 65°C for different times: (A) as-spun, (B) 0.5 h, (C) 1 h, (D) 3 h, (E) 6 h, (F) 9 h, (G) 12 h, (H) 15 h, (I) 18 h, and (J) 24 h; (b) samples treated with water vapor for 3 h at different temperatures: (A) 45°C, (B) 55°C, (C) 65°C, and (D) 75°C.
(a)
(b)Crystallinities of electrospun RSF mats treated with water vapor: (a) at 65°C for different times; (b) for 3 h at different temperatures.
(a)
(b)Figure4(b) shows the influence of temperature on SF mats during water vapor annealing. When the annealing time was fixed at 3 h, the characteristic reflection of silk I structure atD-spacing of 0.72 nm [32, 33] can be observed on the diffractograms at 45 and 55°C. At higher temperatures of 65 and 75°C, clear changes of the diffractograms occur. Not only silk I reflection at 0.72 nm disappears, but also silk II reflections become more intense with the increasing annealing temperature. It can be found from Figure 5(b) that the crystallinity of SF mats increases almost linearly from 45.1% to 51.5% with raising temperature from 45 to 75°C. The above results suggest that the temperature in water vapor annealing process could significantly influence the crystallization behavior of SF mats.


## 3.4. Mechanical Properties of SF Mats

The mechanical properties of the SF mats treated with water vapor at different temperatures and times are shown in Figure6. It can be seen from Figure 6(a) that the breaking strength of the SF mats is greatly improved after annealing in water vapor at 65°C and gradually increases with prolonged treating time. When temperature rises, a more significant increasing trend of breaking strength can be found in Figure 6(b). The two curves of breaking strength in Figure 6 present great consistency with the corresponding crystallinity changes shown in Figure 5. This indicates that the potential SF materials with tunable properties and structures can be achieved by controlling the annealing time and temperature. Although the water-vapor- annealed SF mats do not have mechanical properties comparable to those of the posttreated mats via uniaxial drawing in ethanol solution [20], the moderate characteristic of water vapor annealing is still quite attractive. The mild conditions would be favorable for drug loading and preparation of SF materials with enhanced and uniform mechanical properties [34]. When the mats are annealed at 65°C for 15 h, the breaking stress is improved to 6.0 MPa, which is about 4 times of the as-spun mats (1.8 MPa) [20]. The mats with similar properties could also be achieved within 3 h while raising the temperature to 75°C. This well exhibits the time-temperature equivalence, which may be attributed to the more energy that SF molecules absorbed for conformational transition in a longer annealing period or at a higher annealing temperature. From another aspect, the motion of SF molecules is time dependent. The longer time could result in a more complete structure transition, namely, an increased content of the stable β-sheet structure in SF.Breaking strength and breaking energy of electrospun RSF mats treated with water vapor: (a) at 65°C for different times; (b) for 3 h at different temperatures.
(a)
(b)However, the breaking energy of the mats changes irregularly with annealing condition. It increases with annealing time or temperature first but decreases at an annealing time longer than 15 h in Figure6(a) or at a temperature higher than 65°C in Figure 6(b). This may be attributed to the microstructure changes in SF fibers. With increasing treating time or temperature, the transformation from silk I to silk II is performed more completely. As the primary antiparallel β-sheet structure in silk II structure is more stable than the characterized β-turn type in silk I [35], the SF mats present a higher breaking elongation with increasing β-sheet content. When the crystallinity of SF mats is higher than 50%, the samples with low breaking strain become much brittle and the breaking energy decreases. This phenomenon is similar to the results of SF films [18].


## 4. Conclusions

An effective and easy-conducting approach was developed to fabricate regenerated SF mats through water vapor annealing under different conditions of time and temperature. Water vapor can effectively induce the conformational transition of SF from random coil/α-helix (silk I) to stable β-sheet (silk II) conformation and enhance the mechanical properties of the mats. The structures and properties of the SF mats significantly depend on the annealing time and temperature. Through improving the annealing temperature or prolonging the annealing time, we could achieve SF mats with tunable structures and enhanced mechanical properties. This water-based posttreatment provides a potential option to adjust the secondary structure and crystallinity of SF mats in mild conditions, thereby controlling the properties of SF mats for specific applications without using harmful chemicals. The water-vapor-annealed SF mats and other silk-based materials could be the promising candidates in biomedical fields, including drug delivery, wound dressing, and tissue engineering.



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*Source: 682563-2014-05-05.xml*