*Article* **Fabrication and Properties of Electrospun and Electrosprayed Polyethylene Glycol/Polylactic Acid (PEG/PLA) Films**

**Weichang Ke <sup>1</sup> , Xiang Li <sup>2</sup> , Mengyu Miao <sup>2</sup> , Bing Liu <sup>1</sup> , Xiaoyu Zhang <sup>2</sup> and Tong Liu 2,\***


2017302650114@whu.edu.cn (X.L.); 2015302650129@whu.edu.cn (M.M.); 2016302650148@whu.edu.cn (X.Z.) **\*** Correspondence: liu\_tong@whu.edu.cn

**Abstract:** Polylactic acid (PLA) film is an alternative filter material for heat-not-burn (HNB) tobacco, but its controllability in cooling performance is limited. In this work, polyethylene glycol (PEG) was introduced to form a polyethylene glycol/polylactic acid (PEG/PLA) film by electrospinning or electrospraying techniques to enhance the cooling performance, due to its lower glass transition and melting temperatures. The PEG/PLA films with typical electrospun or electrosprayed morphologies were successfully fabricated. One typical endothermic peak at approximately 65 ◦C was clearly observed for the melting PEG phase in the heating process, and the re-crystallization temperature represented by an exothermic peak was effectively lowered to 90–110 ◦C during the cooling process, indicating that the cooling performance is greatly enhanced by the introduction of the PEG phase. Additionally, the wetting properties and adsorption properties were also intensively studied by characterizing the contact angles, and the as-prepared PEG/PLA films all showed good affinity to water, 1,2-propandiol and triglyceride. Furthermore, the PEG/PLA film with a PLA content of 35 wt.% revealed the largest elasticity modulus of 378.3 ± 68.5 MPa and tensile strength of 10.5 ± 1.1 MPa. The results achieved in this study can guide the development of other filter materials for HNB tobacco application.

**Keywords:** polylactic acid; polyethylene glycol; electrospinning; heat-not-burn tobacco; cooling performance

## **1. Introduction**

Smoking has an extremely long history and is deeply rooted in society. The total consumption of conventional cigarettes, the most popular tobacco product, reached 5.7 trillion in 2016 [1]. As a result, smoked cigarette butts have become one of largest contributors of litter in the world. It has been largely reported that smoked cigarette butts contain over 7000 chemicals, including many harmful and/or carcinogenic effects, which can be released or leached after being released into the environment [2–4]. Therefore, new cigarette types, such as heat-not-burn (HNB) tobacco and electronic cigarettes, have been developed to overcome these threats to life and to the environment. HNB tobacco devices heat tobacco but do not burn it, which can reduce the release of harmful products from its combustion [5–7]. Bentley et al. reported that the emission of toxic products can be reduced by approximately 95% [8]. However, harmful gases, including formaldehyde, acetaldehyde and acrolein, may still be generated in mainstream smoke due to the use of propylene glycol and vegetable glycerin in HNB tobacco [9,10].

Recently, adsorbing materials, such as zeolites, metal–organic frameworks, activated carbon, fibers, coordination polymers and carbon nanotubes, have been developed to further remove the toxic chemicals in mainstream smoke due to their excellent adsorbing properties provided by their extremely high specific surface areas [11–13]. However, there are still many limitations in processing and production, such as the material safety, high

**Citation:** Ke, W.; Li, X.; Miao, M.; Liu, B.; Zhang, X.; Liu, T. Fabrication and Properties of Electrospun and Electrosprayed Polyethylene Glycol/Polylactic Acid (PEG/PLA) Films. *Coatings* **2021**, *11*, 790. https:// doi.org/10.3390/coatings11070790

Academic Editors: Csaba Balázsi and Kevin Plucknett

Received: 10 June 2021 Accepted: 28 June 2021 Published: 30 June 2021

**Publisher's Note:** MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

**Copyright:** © 2021 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https:// creativecommons.org/licenses/by/ 4.0/).

cost and tedious preparation process. Therefore, it is critical to design and manufacture novel, more efficient adsorbing materials for HNB tobacco products.

Biodegradable natural polymer polylactic acid (PLA) is an abundant renewable biomass polymer, which has been applied as an HNB filter material due to its low cost, lightweight and apparently environmentally superiority alternative to synthetic materials [14–16]. It is proven that the harmful pollutants to the environment during the smoking process have been greatly eliminated by the application of PLA filters for HNB tobacco, thus presenting strongly positive effects on the economy, human beings and society [17]. However, the cooling performance can only be narrowly tailored by the use of single-phase PLA. Moreover, the controllability in cooling properties is limited.

Currently, the introduction of polymer materials with lower glass transition and melting temperatures to form blending materials has been considered as one of the most effective strategies to manipulate the cooling performance as the as-prepared blending materials effectively exhibit lowered thermal properties, including glass transition temperature, melting temperature and recrystallization temperature [18–23]. Polyethylene glycol (PEG) material, which has a much lower glass transition temperature (below 40 ◦C) and melting temperature (lower than 70 ◦C) than those for classic PLA filter materials, is one of the most commonly used polymer additives to adjust cooling properties due to its biodegradability, good cooling performance, easy processing and low cost [18–21]. Therefore, PLA and PEG materials are chosen as the main material and polymer additive to form polyethylene glycol/polylactic acid (PEG/PLA) blending film, respectively, and the cooling performance of PEG/PLA blending material can be enhanced by the glass transition and melting of PEG phase at a lower temperature than PLA material, thus leading to a reduced outlet temperature of the filter of HNB tobacco.

The objective of this work is to prepare novel films with high cooling performance, good wetting and adsorption properties, as well as considerable mechanical properties for HNB tobacco application. The electrospinning technique has been considered as one of the most efficient ways to fabricate continuous fibers in the submicron to nanometer scale range, and the microstructure of the fibers is highly dependent on electrospinning parameters such as precursor electrospinning solution, operating voltage and the distance from the collector to the needle [23–35]. Therefore, in the present work, three typical electrospun/electrosprayed PEG/PLA films with different morphologies were prepared by using the simple electrospinning or electrospray method and adjusting the PLA content and precursor electrospinning solution. Their morphologies were measured by using scanning electron microscopy (SEM), while the thermal properties were determined by differential scanning calorimetry (DSC) and thermal conductivity meters (TCM). Finally, the wetting properties and mechanical properties were evaluated using the contact angle meter and universal material testing machine, respectively.

#### **2. Materials and Methods**

#### *2.1. Materials*

Polylactic acid (PLA) with an average molecular weight (Mw) of 80,000 g/mol was purchased from Macklin Biochemical Co. Ltd (Shanghai, China). Polyethylene glycol (PEG) with Mw of 10,000 g/mol was supplied by Aladdin Biochemical Technology Co. Ltd (Shanghai, China). Dimethylacetamide (DMAc), the solvent of the electrospinning solution, was purchased from Sinopharm Chemical Reagent Co., Ltd (Shanghai, China). Note that the chemicals used in this work were all of analytical reagent (AR) grade.

#### *2.2. Preparation and Characterization of the Spinning Solutions*

PLA and PEG were dissolved in DMAc solvent and stirred at 50 ◦C till the homogeneous spinning solutions were obtained, and the composition parameters of three spinning solutions used in this work are listed in Table 1. For simplification, these three spinning solutions were marked as PLA25, PLA35 and PLA45, respectively.


**Table 1.** Composition parameters of the three spinning solutions used in this work.

#### *2.3. Electrospinning Conditions*

A commercial electrospinning apparatus (Model SS-1, Beijing Ucalery Technology Development Co. Ltd., Beijing, China) was applied to prepare PEG/PLA fiber films. A grounded aluminum cylinder with an outer diameter of 10.0 cm and a length of 32.0 cm, which was covered by silicon paper, was used as the fiber collector, and its rotation speed was fixed at 30 rpm. During the electrospinning process, the distance from the collector to the needle was fixed at 12.0 cm. Meanwhile, the flow rate of the solution was precisely controlled at 2 mL/h by using a syringe pump, while the working temperature and the relative humidity in the compartment were controlled at approximately 40 ◦C and 35% relative humidity (RH). The high voltage applied in the electrospinning/electrospray process was +15 kV. The PEG/PLA fiber films obtained by electrospinning for more than 3 h were dried at 50 ◦C in a vacuum oven for 5 h to completely remove the residual solvent. The obtained PEG/PLA films were named PLA25, PLA35 and PLA45, respectively.

#### *2.4. Characterization*

The morphology of the PEG/PLA films was examined by using scanning electron microscopy (SEM; MIRA 3, Tescan, Brno, Czech), which was then further analyzed by using the ImageJ software (ImageJ bundled with 64-bit Java 1.8.0\_172, National Institutes of Health, Bethesda, MD, USA) to calculate the diameters of the fibers.

The Fourier transform infrared (FTIR) spectra of these films were collected by using an FTIR spectrometer (Nicolet 5700, Thermo Fisher, Waltham, MA, USA).

The thermal characteristics of these films were recorded by differential scanning calorimetry (DSC, Q2000, TA Instruments, New Castle, DE, USA) in the temperature range from 30 to 200 ◦C under pure N<sup>2</sup> conditions with a flow rate of 30 mL/min. For each sample, a 10 mg PEG/PLA film was placed in an aluminum crucible and then sealed hermetically during a heating and cooling cycle with a heating and cooling rate of 5 ◦C/min. The phases composition of the fiber films was detected by using an X-ray diffractometer (XRD, X'pert Pro, Malvern Panalytical, Worcester, UK) in the 2-theta (2θ) range of 20◦–80◦ , while the three films with a size of 50 × 50 mm were exposed to pure N<sup>2</sup> to measure their corresponding thermal conductivities at 30 ◦C by using a thermal conductivity meters (TPS 2500S, Hot Disk, Göteborg, Sweden).

The surface wetting properties of the three PEG/PLA films to water, glycerol and 1,2-propanediol were determined by performing contact angle (CA) measurements via a CA meter (JC2000C, POWEREACH, Shanghai, China) to study their adsorption properties. The average CA values were obtained based on at least 5 independent measurements for each sample.

The mechanical properties of these PEG/PLA films were determined using a universal material testing machine (CMT 6103, MTS Systems Corporation, Yokohama, Japan). The stretching rate was 25 mm/min with an initial length between the clamps of 10 mm at 25 ◦C. All samples with a size of 30 mm (length) × 3 mm (width) × 0.5 mm (thickness) were cut along the collector rotation direction, and at least 5 samples for each film were tested to calculate the average values for the interpretation of the results.

#### **3. Results and Discussion**

#### *3.1. Morphology and Phase Composition*

The microstructure of the as-prepared PEG/PLA films shown in Figure 1 significantly changed due to varying the precursor electrospinning solution. PLA25 and PLA35 PEG/PLA films exhibited typical morphologies for the electrospinning method [23–35], while the PLA45 PEG/PLA film showed the characteristic electrosprayed microstructure [33–35]. For the PLA25 film derived from solution PLA25 with the lowest PLA content of 25 wt.%, the outerdiameter (O.D.) of the electrospun PEG/PLA fibers is in the range of 0.10–0.19 µm, while the calculated average O.D. value is 0.14 µm (Figure 1A,a). As the PLA content increased to 35 wt.%, the O.D. of the electrospun PEG/PLA fibers strongly increased to 0.33–2.00 µm, with an average value of 0.80 µm (Figure 1B,b). These phenomena can be explained by the increased viscosity of the solutions induced by the decreased DMAc solvent content and increased PLA binder content, which is also consistent with the previously reported literature [33–37]. However, when further increasing the PLA content to 45 wt.%, no fiber was formed, but homogeneous spherical microsize particles were formed by the PLA45 film (Figure 1C,c), which may be related to the solubility in the solvent, where the intrachain interactions may result in the polymer chains coiling on themselves to form spherical microsize particles [33–35].

Figure 2 shows the XRD patterns of three electrospun/electrosprayed PEG/PLA films mentioned above. Two typical diffraction peaks for PEG (PDF No: 50-2158) and PLA (PDF No: 49-2174), as well as an amorphous bump centered at approximately 23◦ , can be clearly observed in the 2-theta range of 10◦–40◦ , indicating that these PEG/PLA films are a mixture of amorphous phase and crystalline phase, and no secondary phase was formed during the preparation process. In addition, it was found that the signal of the PLA phase became more observable, while the diffraction peaks for the PEG phase became weaker for the three PEG/PLA films, which can be explained by the gradual increase in PLA content.

Figure 3 shows the FTIR infrared absorption spectra of the three PEG/PLA films. It was noticed that with the increasing PLA content in the films, the absorption bands located at approximately 867, 1161 and 3500 cm−<sup>1</sup> , which can be attributed to the O–H stretch and associated with PEG content [38], receded. Meanwhile, the C=O stretching vibration peak at 1758 cm−<sup>1</sup> [39], which can be used to reflect PLA content, was enhanced. These results are strongly consistent with the fact that the PLA content is gradually increased, and no obvious reaction occurs during the preparation process.

**Figure 1.** SEM images of (**a,A**) PLA25, (**b,B**) PLA 35 and (**c,C**)PLA45 PEG/PLA films with the magnification of (**a–c**) 5000× and (**A–C**) 20000×. **Figure 1.** SEM images of (**a**,**A**) PLA25, (**b**,**B**) PLA 35 and (**c**,**C**)PLA45 PEG/PLA films with the magnification of (**a**–**c**) 5000× and (**A**–**C**) 20,000×. *Coatings* **2021**, *11*, x FOR PEER REVIEW 6 of 12

**Figure 2.** XRD patterns of the three electrospun/electrosprayed PEG/PLA films. (Note that the PDF card numbers for neat PEG and PLA materials are both obtained from MDIJade 6.5 software with the 2004 PDF database.). **Figure 2.** XRD patterns of the three electrospun/electrosprayed PEG/PLA films. (Note that the PDF card numbers for neat PEG and PLA materials are both obtained from MDIJade 6.5 software with the 2004 PDF database.).

cated at approximately 867, 1161 and 3500 cm−1, which can be attributed to the O–H stretch and associated with PEG content [38], receded. Meanwhile, the C=O stretching vibration peak at 1758 cm−1 [39], which can be used to reflect PLA content, was enhanced. These results are strongly consistent with the fact that the PLA content is gradually increased,

DSC curves of the three electrospun/electrosprayed PEG/PLA films were measured in the temperature range of 25–200 °C with a cooling and heating rate of 5 °C/min and holding at 200 °C for 30 min to study the thermal transition properties of these samples. Melting temperature, glass transition temperature and crystallization temperature, as well as exothermic and endothermic heat, can be determined in the DSC curves. As shown in Figure 4, in the temperature range of 25–100 °C, during the heating process, typical

and no obvious reaction occurs during the preparation process.

**Figure 3.** FTIR spectra of the three electrospun/electrosprayed PEG/PLA films.

*3.2. Thermal Properties* 

and no obvious reaction occurs during the preparation process.

**Figure 3.** FTIR spectra of the three electrospun/electrosprayed PEG/PLA films. **Figure 3.** FTIR spectra of the three electrospun/electrosprayed PEG/PLA films.

#### *3.2. Thermal Properties 3.2. Thermal Properties*

the 2004 PDF database.).

DSC curves of the three electrospun/electrosprayed PEG/PLA films were measured in the temperature range of 25–200 °C with a cooling and heating rate of 5 °C/min and holding at 200 °C for 30 min to study the thermal transition properties of these samples. Melting temperature, glass transition temperature and crystallization temperature, as well as exothermic and endothermic heat, can be determined in the DSC curves. As shown in Figure 4, in the temperature range of 25–100 °C, during the heating process, typical DSC curves of the three electrospun/electrosprayed PEG/PLA films were measured in the temperature range of 25–200 ◦C with a cooling and heating rate of 5 ◦C/min and holding at 200 ◦C for 30 min to study the thermal transition properties of these samples. Melting temperature, glass transition temperature and crystallization temperature, as well as exothermic and endothermic heat, can be determined in the DSC curves. As shown in Figure 4, in the temperature range of 25–100 ◦C, during the heating process, typical endothermic peaks at approximately 65 ◦C could be observed, which are possibly attributed to the glass transition of PLA phase as well as the melting of PEG phase. However, no characteristic peak for the glass transition of PLA phase, a step change in the base line of the scan at approximately 65 ◦C, was observed. A possible reason for this is that the endothermic peak for the glass transition of PLA phase may be buried due to the stronger melting peak of PEG phase, which can be confirmed by the lowered strength of the endothermic peak with the increasing amount of PLA phase. It should be highlighted that the endothermic peak for the melting of PEG phase can serve as the additional heat absorber during the cooling process, thus reducing the temperature of the flowing gas and improving the cooling performance of PLA material. The characteristic endothermic peak with an onset temperature of approximately 160 ◦C is ascribed to the melting of PEG/PLA films, which is lower than approximately 170 ◦C for PLA phase [16]. At the same time, the only typical exothermic peak observed at 90–110 ◦C during the cooling process is probably associated with the recrystallization of PEG/PLA composite materials, and the temperature is obviously lower than that for pure PLA material [16]. These results, including the low-temperature endothermal peak at 65 ◦C for melting PEG phase, decreased melting temperature from 170 to 160 ◦C and lowered onset recrystallization from approximately 130 to 110 ◦C, indicate that the addition of PEG can effectively improve the cooling performance, and the increase in PEG content can further optimize the cooling performance. Note that a small exothermic peak was observed at approximately 70 ◦C, which is possibly ascribed to the evaporation of the remaining DMAc solvent in the film.

**Figure 2.** XRD patterns of the three electrospun/electrosprayed PEG/PLA films. (Note that the PDF card numbers for neat PEG and PLA materials are both obtained from MDIJade 6.5 software with

Figure 3 shows the FTIR infrared absorption spectra of the three PEG/PLA films. It was noticed that with the increasing PLA content in the films, the absorption bands located at approximately 867, 1161 and 3500 cm−1, which can be attributed to the O–H stretch and associated with PEG content [38], receded. Meanwhile, the C=O stretching vibration peak at 1758 cm−1 [39], which can be used to reflect PLA content, was enhanced. These results are strongly consistent with the fact that the PLA content is gradually increased,

Figure 5 shows the thermal conductivities of the three electrospun/electrosprayed PEG/PLA films measured at 30 ◦C. The thermal conductivity effectively increased from 0.1072 W·m−<sup>1</sup> ·K −1 for the PLA25 film to 0.2046 and 0.2237 W·m−<sup>1</sup> ·K −1 for the PLA35 film and the PLA45 film, respectively. These results imply that a higher PLA content and lower porosity in the electrospun/electrosprayed PEG/PLA films can benefit heat transfer and can further enhance the cooling performance.

**Figure 4.** DSC curves of the three electrospun/electrosprayed PEG/PLA films. **Figure 4.** DSC curves of the three electrospun/electrosprayed PEG/PLA films.

ascribed to the evaporation of the remaining DMAc solvent in the film.

endothermic peaks at approximately 65 °C could be observed, which are possibly attributed to the glass transition of PLA phase as well as the melting of PEG phase. However, no characteristic peak for the glass transition of PLA phase, a step change in the base line of the scan at approximately 65 °C, was observed. A possible reason for this is that the endothermic peak for the glass transition of PLA phase may be buried due to the stronger melting peak of PEG phase, which can be confirmed by the lowered strength of the endothermic peak with the increasing amount of PLA phase. It should be highlighted that the endothermic peak for the melting of PEG phase can serve as the additional heat absorber during the cooling process, thus reducing the temperature of the flowing gas and improving the cooling performance of PLA material. The characteristic endothermic peak with an onset temperature of approximately 160 °C is ascribed to the melting of PEG/PLA films, which is lower than approximately 170 °C for PLA phase [16]. At the same time, the only typical exothermic peak observed at 90–110 °C during the cooling process is probably associated with the recrystallization of PEG/PLA composite materials, and the temperature is obviously lower than that for pure PLA material [16]. These results, including the low-temperature endothermal peak at 65 °C for melting PEG phase, decreased melting temperature from 170 to 160 °C and lowered onset recrystallization from approximately 130 to 110 °C, indicate that the addition of PEG can effectively improve the cooling performance, and the increase in PEG content can further optimize the cooling performance. Note that a small exothermic peak was observed at approximately 70 °C, which is possibly

**Figure 5.** Thermal conductivities of the three electrospun/electrosprayed PEG/PLA films measured at 30 °C. **Figure 5.** Thermal conductivities of the three electrospun/electrosprayed PEG/PLA films measured at 30 ◦C.

#### *3.3. Wetting and Adsorption Properties 3.3. Wetting and Adsorption Properties*

The wetting properties of the three electrospun/electrosprayed PEG/PLA films towards water, 1,2-propanediol and triglyceride were also studied and are summarized in Figure 6. The contact angles were 88.4° ± 1.5°, 34.4° ± 1.7° and 42.3° ± 1.2° when the PLA25 film was exposed to water, 1,2-propandiol and triglyceride, respectively. As the PLA content increased to 35 wt.%, the corresponding contact angle values for the PLA35 film gradually increased to 111.4° ± 0.8°, 36.7° ± 3.6° and 51.2° ± 2.5 o, respectively. However, by further increasing PLA content, the contact angle to water slightly decreased to 100.9° ± 3.2°, while the values to 1,2-propanediol and triglyceride continually increased to 43.7° ± 2.8° and 53.0° ± 3.5 o, respectively. The increase in contact angle value implies the decrease in wetting properties and adsorption properties of the films, which may be explained by the increased PLA content with lower adsorption properties [40]. The wetting properties of the three electrospun/electrosprayed PEG/PLA films towards water, 1,2-propanediol and triglyceride were also studied and are summarized in Figure 6. The contact angles were 88.4◦ ± 1.5◦ , 34.4◦ ± 1.7◦ and 42.3◦ ± 1.2◦ when the PLA25 film was exposed to water, 1,2-propandiol and triglyceride, respectively. As the PLA content increased to 35 wt.%, the corresponding contact angle values for the PLA35 film gradually increased to 111.4◦ ± 0.8◦ , 36.7◦ <sup>±</sup> 3.6◦ and 51.2◦ <sup>±</sup> 2.5 <sup>o</sup> , respectively. However, by further increasing PLA content, the contact angle to water slightly decreased to 100.9◦ ± 3.2◦ , while the values to 1,2-propanediol and triglyceride continually increased to 43.7◦ <sup>±</sup> 2.8◦ and 53.0◦ <sup>±</sup> 3.5 <sup>o</sup> , respectively. The increase in contact angle value implies the decrease in wetting properties and adsorption properties of the films, which may be explained by the increased PLA content with lower adsorption properties [40].

**Figure 6.** Contact angles for the three electrospun/electrosprayed PEG/PLA films.

**Figure 6. Figure 6.** Contact angles for the three electros Contact angles for the three electrospun/electrosprayed PEG/PLA films. pun/electrosprayed PEG/PLA films.

the increased PLA content with lower adsorption properties [40].

#### *3.4. Mechanical Properties 3.4. Mechanical Properties*

at 30 °C.

*3.3. Wetting and Adsorption Properties* 

The typical strain–stress curves for three different PEG/PLA films shown in Figure 7 were measured by using the tension method. The mechanical properties, involving maximum elasticity modulus, tensile break stress, tensile strength, tensile yield stress and maximum force, are summarized in Table 2. It was found that the PLA35 film exhibited the largest value with the maximum elasticity modulus of 378.3 ± 68.5 MPa, the tensile break stress of 4.3 ± 0.5 MPa, the tensile strength of 10.5 ± 1.1 MPa, the tensile yield stress of 9.5 ± 1.0 MPa and the maximum force of 0.31 ± 0.03 N, respectively. The PLA45 film showed the peak tensile strain at break of 67.9% ± 21.4%, while the PLA25 film revealed the worst mechanical properties. The mechanical properties are different for these three films, which is possibly attributed to their different porosities and morphologies, requiring further study in the future. The typical strain–stress curves for three different PEG/PLA films shown in Figure 7 were measured by using the tension method. The mechanical properties, involving maximum elasticity modulus, tensile break stress, tensile strength, tensile yield stress and maximum force, are summarized in Table 2. It was found that the PLA35 film exhibited the largest value with the maximum elasticity modulus of 378.3 ± 68.5 MPa, the tensile break stress of 4.3 ± 0.5 MPa, the tensile strength of 10.5 ± 1.1 MPa, the tensile yield stress of 9.5 ± 1.0 MPa and the maximum force of 0.31 ± 0.03 N, respectively. The PLA45 film showed the peak tensile strain at break of 67.9% ± 21.4%, while the PLA25 film revealed the worst mechanical properties. The mechanical properties are different for these three films, which is possibly attributed to their different porosities and morphologies, requiring further study in the future.

**Figure 5.** Thermal conductivities of the three electrospun/electrosprayed PEG/PLA films measured

The wetting properties of the three electrospun/electrosprayed PEG/PLA films towards water, 1,2-propanediol and triglyceride were also studied and are summarized in Figure 6. The contact angles were 88.4° ± 1.5°, 34.4° ± 1.7° and 42.3° ± 1.2° when the PLA25 film was exposed to water, 1,2-propandiol and triglyceride, respectively. As the PLA content increased to 35 wt.%, the corresponding contact angle values for the PLA35 film gradually increased to 111.4° ± 0.8°, 36.7° ± 3.6° and 51.2° ± 2.5 o, respectively. However, by further increasing PLA content, the contact angle to water slightly decreased to 100.9° ± 3.2°, while the values to 1,2-propanediol and triglyceride continually increased to 43.7° ± 2.8° and 53.0° ± 3.5 o, respectively. The increase in contact angle value implies the decrease in wetting properties and adsorption properties of the films, which may be explained by

**Figure 7.** Strain–stress curves for the three electrospun/electrosprayed PEG/PLA films. **Figure 7.** Strain–stress curves for the three electrospun/electrosprayed PEG/PLA films.

**Table 2.** Summary of the mechanical properties of the three electrospun/electrosprayed PEG/PLA **Table 2.** Summary of the mechanical properties of the three electrospun/electrosprayed PEG/PLA films.


Maximum force (×10−1 N) 1.3 ± 0.2 3.1 ± 0.3 2.1 ± 0.5

film due to its desirable cooling performance and mechanical strength, as well as considerable wetting and adsorption properties to water, 1,2-propanediol and triglyceride, as

summarized in Table 3.

Consequently, the PLA35 film with wider fibers and lower porosity is the optimal film due to its desirable cooling performance and mechanical strength, as well as considerable wetting and adsorption properties to water, 1,2-propanediol and triglyceride, as summarized in Table 3.

**Table 3.** Summary of the physicochemical properties of the three electrospun/electrosprayed PEG/PLA films.


#### **4. Conclusions**

Herein, three PEG/PLA films with different morphologies were successfully prepared by varying the PLA content in the precursor solutions and by using the electrospinning or electrospray method. The morphology, phase composition, thermal properties, wetting properties and mechanical properties of the films were intensively studied, finding that the cooling performance of the PLA film was effectively improved by the addition of PEG due to its lower glass transition temperature and melting temperature. Moreover, the mechanical properties of the PEG/PLA films are greatly affected by their composition and morphology. It was demonstrated that the PLA35 film fabricated by the precursor electrospinning solution with a PLA content of 35 wt.% exhibited a desirable cooling performance, the best mechanical properties and acceptable wetting and adsorption properties towards water, 1,2-propanediol and triglyceride. As a result, the PLA35 film is a potential alternative film for HNB tobacco application.

**Author Contributions:** Conceptualization, W.K. and T.L.; methodology, X.L; software, X.L.; validation, M.M, B.L. and X.Z.; formal analysis, W.K.; investigation, W.K., X.L., M.M., B.L., X.Z. and T.L.; writing—original draft preparation, T.L.; writing—review and editing, W.K and T.L. All authors have read and agreed to the published version of the manuscript.

**Funding:** This research was funded by the Science and Technology Project of China Tobacco Hubei Industrial LLC, Grant No.: 2019420000340371.

**Institutional Review Board Statement:** Not applicable.

**Informed Consent Statement:** Not applicable.

**Data Availability Statement:** Data sharing not applicable.

**Conflicts of Interest:** The authors declare no conflict of interest.

## **References**


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