Startseite The effects of nanoparticles on morphology and thermal properties of erythritol/polyvinyl alcohol phase change composite fibers
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The effects of nanoparticles on morphology and thermal properties of erythritol/polyvinyl alcohol phase change composite fibers

  • Haishan Che , Qianqiao Chen EMAIL logo , Qin Zhong und Si He
Veröffentlicht/Copyright: 3. Juli 2018
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e-Polymers
Aus der Zeitschrift e-Polymers Band 18 Heft 4

Abstract

Erythritol (E)/polyvinyl alcohol (PVA) phase change composite fibers in which PVA acts as supporting material and different contents of erythritol act as phase change materials (PCMs) were prepared by electrospinning. The effects of different nanoparticles on fiber morphology and thermal properties of composites were also studied. The morphology and thermal properties were characterized by using scanning electron microscopy (SEM), differential scanning calorimetery (DSC) and a thermal conductivity test, respectively. The results showed E/PVA composite fibers were cylindrical with a smooth surface. The content of erythritol in composites could reach a high of 80 wt% with good shape stability, and a high enthalpy value of 258.9 J/g after 100 thermal cycles. The effects of nanoparticles on composites were mainly embodied in decreasing average fiber diameters (AFDs), phase change temperatures and enthalpies with the increase of particle concentrations, and improving fiber stability and thermal conductivity. Among them, the smallest AFDs (0.56 μm) and the lowest heat loss rate (1.0%) were obtained from composites with 4% nano C and 4% nano Al2O3, respectively. The 4% nano SiO2 composites possessed the best shape stability. In addition, the composites that contains 4% nano carbon could decrease the erythritol’s supercooling of 7.55°C, and showed the highest thermal conductivity of 1.55 W/m·K, which was 167% of E/PVA composites. These results demonstrate that E/PVA composites possess high enthalpy values while they improve shape stability and thermal conductivity.

1 Introduction

Energy is the foundation of human existence and development, with the development of world economy, the reality for mankind is not only the impending energy shortage, but also the environment pressure of consuming large amounts of fossil energy. Because of its simple equipment, low cost and other unique advantages, phase change thermal storage has become one of the key technologies of energy storage and energy efficiency (1). Meanwhile, it has attractive application prospect in solar energy and waste heat saving. The phase change material (PCM) is the core of the phase change thermal storage.

For the PCMs, solid-liquid PCMs are the most valuable due to their huge latent heat. Compared with the inorganic PCMs, organic PCMs, such as paraffin (2), fatty acids (3) and polyols (4) have several advantages; large thermal storage density, corrosion resistance, good thermal stability and being less expensive, etc. To the best of our knowledge, from the present relevant literature, among the current study of organic PCMs, erythritol is closely watched because of its excellent thermal properties. The phase change enthalpy of erythritol (about 340 J/g) (5, 6) is at least twice that of molten salts, and three times that of the solar salts. The thermal conductivity of the solid state is 0.733 W/(m·K) (7), which is higher than molten salts and solar salts. In addition, its phase change temperature (about 118°C) is higher, so it can also be used for the medium temperature phase change system (7) and in industrial waste heat recovery systems (8), etc. At present, the research on erythritol is focused on improving the thermal conductivity and preparation of the form-stable phase change composites like other PCMs.

The form-stable phase change energy storage composite materials can be obtained through the study or the encapsulation of PCMs; it can not only solve the leakage during the phase change process and it can also enhance its applicability in a variety of spaces. The most common type of encapsulation methods can be divided into four categories: pressing-sintering, micro-encapsulation, adsorption and electrospinning. Pressing-sintering was the earliest encapsulation method (9). It calcines the mixture of carrier materials and phase change materials after pressing it into the required shape and grinding it to a certain size. Because of the simple process, low demands for containers and low cost, the research on this method has retained much interest. Micro-encapsulation phase change composites use using membrane materials to encase solid or liquid PCMs to form particles of 1~300 μm (10). Its preparation methods mainly include in situ, interface, suspending, emulsion and noumenon polymerization. It can increase the heat transfer area, reduce the activity of PCMs with the external environment, and control the volume change during the phase transformation. Adsorption is also a common phase change preparation method for composites, which uses infiltrating penetration or vacuum adsorption of PCMs into the base materials including metallic foams (11) or graphite materials (12). It is characterized by high thermal conductivity and rapid rates of heat storage and release.

Electrospinning is an effective way of preparing fibers. The solution droplets are gradually stretched and squirted out by the force of the electric field, which eventually forms the fiber mat on the receiving device. The electrospinning is not only a straightforward and versatile technology, but it also has various spinning materials, such as polymers, mixtures, semiconductors, etc. Due to the advantages of structure and controllable performance, and its adjustable size, the fiber mats can be used in various applications, such as in catalytic (13, 14), lithium-ion batteries (15) and biomedical applications (16, 17), etc.

As a versatile method of preparing fibers, electrospinning was also applied in preparing phase change composite fibers. Chen et al. (18) firstly prepared phase change composite fibers in which polyethylene glycol (PEG) acted as a PCM and cellulose acetate (CA) acts as supporting material by electrospinning in 2007, the results demonstrated that the composites can still maintain good shape and high enthalpy values after thermal cycles. In the following years, different kinds of phase change composite fibers were prepared via electrospinning. For example, Chen et al. (19, 20) and Cai et al. (21) developed series of composite fibers by combining pure organic materials (22) and their eutectics (23, 24) as PCMs with different supporting materials. At the same time, the effect of factors of electrospun fibers, such as spinning conditions, parameters and additives were also studied. At present, electrospinning has become a more mature technique to prepare form-stable phase change materials.

Thermal conductivity enhancement materials such as inorganic matrixes (15), expanded graphite (5), graphite foam (25, 26) and nanoparticles have been applied to improve the thermal conductivity of PCMs. Among these thermal conductivity enhancers, nanoparticles have attracted the most attention due to their large surface area, excellent heat stability, good chemical resistance and high thermal conductivity. Harish et al. (27) found the enhancement of thermal conductivity of lauric acid was markedly improved with the loading of a single-walled carbon nanohorn. Nano aluminum was used to improve the thermal conductivity of paraffin in the paper by Zhou et al. (28). In addition, nanoparticles were also found to have effects on the morphology and thermal properties of phase change composite fibers. Cai et al. (29) and Susiani and Harsoyo (30) selected nano-SiO2 and nano-TiO2 as additives in their phase change composite fibers, respectively. The results revealed that nanoparticles have appreciable effects on fiber morphology as well as thermal properties. Babapoor et al. (31) found that the fiber diameter decreased by increasing the nanoparticles (SiO2, Al2O3, Fe2O3 and ZnO) loading in phase change composite fibers. In addition, graphite (32) and carbon nanotube (33) were also proven have obvious effects on fiber shape as well as thermal properties including thermal conductivity of phase change composite fibers.

At present, to the best of our knowledge, erythritol has not been prepared into phase change composites via electrospinning, and there is no literature studying the differences of inorganic nanoparticle (SiO2), metal oxide nanoparticle (TiO2 and Al2O3) and nano carbon on the effects of phase change composite fibers at the same time. So, in this paper, high performance phase change E/PVA composite fibers with various contents of erythritol were prepared by electrospinning. The effects of erythritol percentage on fiber morphology and thermal properties were investigated. Different nanoparticles (SiO2, TiO2, Al2O3 and carbon) were added into E/PVA-3 composites, in order to study the effects of nanoparticles on the fiber morphology and thermal properties of composites by SEM, DSC, thermal conductivity test, respectively.

2 Experimental

2.1 Materials

The PVA (MW=130,000) was obtained from the Shanghai Kaiyuan Chemical Technology Co., Ltd. China. The erythritol (E) powder was obtained from Zibo Zhongshi Biotechnology Co., Ltd. (China). Nano SiO2 (<15 nm, purity of 99.5%, 2.3~4.5 W/m·K), TiO2 (<25 nm, purity of 99.8%, ~1.6 W/m·K), Al2O3 (<30 nm, purity of 99.99%, ~2.5 W/m·K) and carbon (<25 nm, purity of 99.5%, <2000 W/m·K) were obtained from Aladdin. All of the chemicals were used without further purification.

2.2 Sample preparation and electrospinning process

Firstly, the different contents of nanoparticles (0.5 wt%, 2 wt% and 4 wt%) were dispersed into deionized water under ultrasonic dispersion for 30 min to obtain uniform nanofluids. Heating the aforementioned solutions to above 95°C dissolved the PVA to prepare 10 wt% PVA solutions. Then, a series of mixture solutions were prepared by adding the appropriate mass of erythritol into the above uniform solutions by magnetic stirring for 30 min. After standing for 2 h, the mixture solutions become homogeneous and clear liquids which can be used for electrospinning. For comparison, pure PVA solution without nanoparticles was also prepared.

Electrospinning was performed at room temperature in air. The spinning device (DFS-100, Beijing Technova Technology Co., Ltd.) was used to fabricate composite fibers using a distance of 15 cm, flow rate of 2.4 ml/h, and a voltage power of 8 kV. All the fibers were dried in a vacuum at 80°C for 24 h to remove the residual solvent. For convenience, the composites which contain 60 wt%, 70 wt% and 80 wt% of erythritol are identified as E/PVA-1, E/PVA-2 and E/PVA-3, respectively.

2.3 Thermal cycles test

Thermal cycle test was used to study the structure, shape and thermal stabilities of composites by using a drying oven (WGL-45B, Tianjin, Instrument Co., Ltd.), in the temperature interval 20–160°C in air.

2.4 Characterization of the samples

The solution properties were composed of viscosity, surface tension and electric conductivity, which were measured using a viscometer (LVDV-I Prime, Brookfield, NY, USA), a surface tension apparatus (BZY-A, Shanghai Fangrui Instrument Co., Ltd., China) and a conductivity meter (DDSJ-308F, Shanghai Leici Instrument Co., Ltd., China), respectively. All measurements were carried out at 25°C and an average value was obtained from at least three repeated measurements.

Fibers were gold-coated and the morphology was observed by field emission-scanning electron microscopy (FE-SEM) (FEI Quanta 250F) at an acceleration voltage of 20 kV under low vacuum. The average fiber diameter (AFDs) of electrospun fibers was obtained by using an UTHSCSA Image Tool Program to measure from at least five SEM images for each sample. Thermal analysis was performed (each used about 10.0 mg) by differential scanning calorimetry (DSC) (DSC8500, PerkinElmer, USA). Both the heating rate and the cooling rate were 2°C/min ranging from 20 to 160°C in a nitrogen atmosphere. The thermal conductivities of composites were measured by thermal conductivity apparent (DRL-III, Xiangtan Xiangyi Co., Ltd.). An average value was obtained from at least three repeated measurements for every sample.

3 Results and discussion

3.1 Fiber morphology

Figure 1 shows the SEM images of nanoparticles, the particles are granulated in shape. The nanoparticles are clustered into groups because of the high surface energy with such a small size (34).

Figure 1: SEM images of nanoparticles: (a) SiO2, (b) TiO2, (c) Al2O3 and (d) Carbon.
Figure 1:

SEM images of nanoparticles: (a) SiO2, (b) TiO2, (c) Al2O3 and (d) Carbon.

Figure 2 shows the typical morphology of E/PVA-1, E/PVA-2 and E/PVA-3 composite fibers. Both the AFDs and the solution properties including viscosity, surface tension and electric conductivity are shown in Table 1. As shown in Figure 2, composite fibers possess smooth surfaces and a cylindrical shape same as PVA fibers (Figure S1). As displayed in Table 1, the AFDs of both PVA and composite fibers are 0.51 μm, 0.72 μm, 1.01 μm and 1.25 μm, respectively. Obviously, the addition of erythritol into PVA solution markedly increase the diameter of the resulting fibers. Such a result might be attributed to the property variations of mixture solutions compared with those of PVA solution, in which viscosity and surface tension increased, whilst the corresponding conductivity decreased as shown in Table 1. Based on the data in Table 1, electric conductivity of solution had the biggest influence on AFDs, followed by viscosity and surface tension. A similar phenomenon was reported in the literature (19).

Figure 2: SEM images of composite fibers: (a–a′) E/PVA-1, (b–b′) E/PVA-2 and (c–c′) E/PVA-3 before and after 100 heating-cooling cycles.
Figure 2:

SEM images of composite fibers: (a–a′) E/PVA-1, (b–b′) E/PVA-2 and (c–c′) E/PVA-3 before and after 100 heating-cooling cycles.

Table 1:

Properties of E/PVA solutions and the AFDs of fibers.

SolutionsElectric conductivity (µS/cm)Surface tension (mN/m)Viscosity (cP)AFDs (μm)
PVA67635.24660.51
E/PVA-159136.15530.72
E/PVA-250436.75761.01
E/PVA-331537.25811.25
0.5% SiO2/E/PVA-342337.55921.16
2% SiO2/E/PVA-351638.06060.84
4% SiO2/E/PVA-367138.36150.61
0.5% TiO2/E/PVA-338437.65881.21
2% TiO2/E/PVA-349838.16010.97
4% TiO2/E/PVA-361338.56130.73
0.5% Al2O3/E/PVA-345137.35851.12
2% Al2O3/E/PVA-352937.75930.89
4% Al2O3/E/PVA-368338.26020.65
0.5% Carbon/E/PVA-348137.35841.17
2% Carbon/E/PVA-362637.85910.85
4% Carbon/E/PVA-377238.16050.56

In order to investigate the shape stability of composite fibers, the representative SEM images of E/PVA-1, E/PVA-2 and E/PVA-3 composite fibers before and after 100 heating-cooling thermal cycles are also shown in Figure 2. It can be found from Figure 2 that due to the high tackiness of sugar alcohol materials, the fibers look like an interconnected network with some conglutinations and crosslinks occurring between fibers after thermal cycles. Even so, the cycled composite fibers can still maintain a cylindrical shape, it can be attributed to the restriction of PCMs by the physical adsorption of fiber networks. The E/PVA-3 composites can retain good morphology after thermal cycles, it means the content of erythritol in composites can reach as high as 80 wt%, and possess high shape stability.

3.2 Thermal properties

DSC analysis was conducted to investigate the thermal properties of the samples. DSC curves of erythritol powder and E/PVA composites before and after 100 thermal cycles are illustrated in Figure 3. The DSC characteristics of the samples such as phase change temperatures and enthalpy values are summarized in Table 2. The theoretical enthalpy values of composites are calculated by multiplying the latent heat of pure erythritol powder and the mass percentage of erythritol in composites. For the composites, the melting and crystallization temperatures are 118.10°C and 38.83°C, however, the melting points of composites gradually get bigger and the crystallization temperatures become gradually with the decreasing amount of erythritol in the composites, this is led to the low thermal conductivity of PVA as the supporting material in composites.

Figure 3: DSC curves of samples before: (A) and after (B) 100 thermal cycles.
Figure 3:

DSC curves of samples before: (A) and after (B) 100 thermal cycles.

Table 2:

Thermal properties of erythritol powder and composites.

SampleTm (°C)∆Hm (J/g)Tc (°C)∆Hc (J/g)
Erythritol118.10340.638.83252.3
Erythritol (cycled)118.15332.338.76250.2
E/PVA-1118.61196.738.75151.4
E/PVA-1 (cycled)118.65194.538.73149.8
E/PVA-2118.67227.538.72176.6
E/PVA-2 (cycled)118.72224.738.68174.7
E/PVA-3118.74262.738.67201.8
E/PVA-3 (cycled)118.80258.938.65199.6

Table 2 confirmed that the latent heat of composites depends on the mass ratio of erythritol as PVA shows no phase transition in this temperature range (<160°C), and the enthalpy values increase with increasing the erythritol percent in composites. As shown in Table 2, the ∆Hm (∆Hc) of pure erythritol and three composites after thermal cycles are 332.3 (250.2) J/g, 194.5 (149.8) J/g, 224.7 (174.7) J/g and 258.9 (199.6) J/g, respectively. From these data, it can be indicated that the content of erythritol in composites can reach a high of 80 wt%, and the E/PVA-3 composites exhibit high thermal storage performance and excellent reusability.

It can be concluded from combining the results of the analyses in Section 3.1 with 3.2, that the erythritol content in the composites can reach as high as 80 wt%, the E/PVA-3 composites possess good shape stability and excellent thermal stability after thermal cycles. Therefore, the effects of nanoparticles on morphology and thermal properties of E/PVA composites are studied based on E/PVA-3 composites.

3.3 The effect of nanoparticles on fiber morphology

The morphology of E/PVA-3 composite fibers with nanoparticles (SiO2, TiO2, Al2O3 and carbon) before and after 100 thermal cycles are shown in Figure 4. These images demonstrate that composites are still cylindrical fibers. The AFDs decrease with increasing the percentage of nanoparticles, such a result is caused by the increase of solution electric conductivity as displayed in Table 1, the higher electric conductivity, the more slender AFDs. After thermal cycles, the morphology of composite fibers appeared the have some variations for the same reasons explained for Figure 2, however, fortunately, the addition of nanoparticles alleviate the conglutination phenomena between fibers.

Figure 4: SEM images of E/PVA-3 composites with different content: (a) 0.5 wt%, (b) 2 wt%, (c) 4 wt% of nanoparticles and (d) 4 wt% composites after cycles.
Figure 4:

SEM images of E/PVA-3 composites with different content: (a) 0.5 wt%, (b) 2 wt%, (c) 4 wt% of nanoparticles and (d) 4 wt% composites after cycles.

It can be concluded that the smallest AFD is obtained from E/PVA-3 composite fibers with 4% nano carbon because of the highest solution for electric conductivity, and the addition of nanoparticles can markedly improve the morphology of composites after cycles; composites with 4% nano SiO2 possess the best shape stability.

3.4 The effect of nanoparticles on composites thermal properties

In order to investigate the effects of nanoparticles on the thermal properties of composites, DSC curves of E/PVA-3 composites with nano SiO2, TiO2, Al2O3 and carbon are shown in Figure 5. The corresponding DSC data are illustrated in Table 3. In addition, the heat loss rates are the percentage difference of ∆H before and after thermal cycles.

Figure 5: DSC curves of E/PVA-3 composites with different content of nanoparticles: (A) SiO2, (B) TiO2, (C) Al2O3 and (D) carbon.
Figure 5:

DSC curves of E/PVA-3 composites with different content of nanoparticles: (A) SiO2, (B) TiO2, (C) Al2O3 and (D) carbon.

Table 3:

Thermal properties of E/PVA-3 composites with different nanoparticles before and after thermal cycles.

SamplesTm (°C)ΔHm (J/g)Heat loss rate (%)Tc (°C)ΔHc (J/g)Heat loss rate (%)
0.5% SiO2116.46256.52.341.13198.60.5
2% SiO2115.73254.73.041.18196.41.6
4% SiO2114.82250.14.841.23195.91.8
4% SiO2 cycled114.16247.91.241.26194.22.7
0.5% TiO2116.23257.12.141.28197.31.2
2% TiO2115.54254.63.141.36196.61.5
4% TiO2114.97250.94.541.47195.22.2
4% TiO2 cycled114.28247.51.341.49193.82.9
0.5% Al2O3116.32256.82.239.49195.91.8
2% Al2O3115.17254.03.339.56194.82.4
4% Al2O3114.96250.44.739.68194.02.8
4% Al2O3 cycled114.26247.81.039.69192.73.4
0.5% Carbon116.77256.92.246.18190.54.5
2% Carbon115.39254.53.146.27188.65.5
4% Carbon114.83250.54.646.32187.36.1
4% Carbon cycled114.36247.61.146.30186.56.5

Comparing the data of Table 2 with Table 3, the composites with nanoparticles have forward phase transition temperatures ranging from 114.82 to 116.77°C, and short melting processes. This is caused by the increase of heat transfer rates on fibers after the addition of nanoparticles. The enthalpy values decrease in different degrees with the increase of nanoparticle contents, such a phenomenon has also appeared in the literature (24). Moreover, the addition of nanoparticles, especially nano carbon, have a positive effect on the supercooling phenomenon of erythritol, it decreases 7.55°C of supercooling when the additive amount is 4%. This phenomenon might be caused by the nucleation of nanoparticles during the crystallization process of molten erythritol. After thermal cycles, there are no obvious variations in phase change temperatures, but there is a slight decrease in the enthalpies of the composites. The composites with 4% nano Al2O3 possess the best thermal stability with the lowest heat loss rate of 1.0%.

3.5 Thermal conductivity

Thermal conductivity is also one of the important symbols of phase change composites. Figure 6 displayed the effects of nanoparticles on thermal conductivity of E/PVA-3 composites. The thermal conductivity of E/PVA-3 composites is calculated to be 0.58 W/m·K. As shown in Figure 6, the addition of nanoparticles can effectively improve the thermal conductivity of composites, among these nano carbons have the strongest effect. The markedly enhanced thermal conductivity for 0~2% nano carbon in composites can be contributed to the high thermal conductivity of carbon and the increase of particle content per unit area in composites. The slight increase for 2~4% of nano carbon is due to the content (2%) of nano carbon being enough to build a heat conduction network on the surface and within the composites. Nevertheless, the thermal conductivity of E/PVA-3 composites is improved 167% after adding 4% nano carbon to it, it means the heat transfer rate of composites can be increased efficiently.

Figure 6: Thermal conductivity of composites.
Figure 6:

Thermal conductivity of composites.

4 Conclusion

A series of high performance E/PVA phase change composite fibers were prepared by electrospinning, and different nanoparticles were added in composites in order to investigate the effects on the fiber morphology and thermal properties of composites. SEM, DSC and thermal conductivity tests were used to characterize the morphology and thermal properties, respectively. According to the results, composite fibers without nanoparticles showed a cylindrical shape with smooth surfaces. The AFDs of fibers ranged from 0.72 to 1.25 μm and increased with the increase of erythritol contents. The E/PVA-3 composites could still maintain good fibrous shapes and showed a heat loss rate of 1.47% after 100 thermal cycles. The addition of nanoparticles decreased the AFDs, phase transition temperatures and enthalpy values gradually, and improved the morphology stability after cycles as well as thermal conductivity significantly. Among them, the smallest AFDs (0.56 μm) and the lowest heat loss rate (1.0%) were obtained from composites with 4% nano carbon and 4% nano Al2O3, respectively. The 4% nano SiO2 composites possess the lowest phase change temperature of 114.16°C and the best shape stability. In addition, the composites containing 4% nano carbon could decrease the erythritol’s supercooling of 7.55°C, and showed the highest thermal conductivity of 1.55 W/m·K at the same time, which was 167% of E/PVA composites. Therefore, as form-stable phase change composites, E/PVA composite fibers can be applied in many medium temperature energy storage fields.

Award Identifier / Grant number: 51408309

Award Identifier / Grant number: 51578288

Funding statement: This work was financially supported by the Key Project of Chinese National Programs for Research and Development (2016YFC0203800), the National Natural Science Foundation of China (51408309 and 51578288).

References

1. Du Y, Ding Y. Towards improving charge/discharge rate of latent heat thermal energy storage (LHTES) by embedding metal foams in phase change materials (PCMs). Chem Eng Process. 2016;108:181–8.10.1016/j.cep.2016.08.003Suche in Google Scholar

2. Xu B, Li Z. Paraffin/diatomite composite phase change material incorporated cement-based composite for thermal energy storage. Appl Energ. 2013;105:229–37.10.1016/j.apenergy.2013.01.005Suche in Google Scholar

3. Li M, Wu Z, Kao H. Study on preparation, structure and thermal energy storage property of capric–palmitic acid/attapulgite composite phase change materials. Appl Energ. 2011;88:3125–32.10.1016/j.apenergy.2011.02.030Suche in Google Scholar

4. Qian T, Li J, Ma H. Adjustable thermal property of polyethylene glycol/diatomite shape-stabilized composite phase change material. Polym Compos. 2016;37:854–60.10.1002/pc.23243Suche in Google Scholar

5. Shin HK, Rhee KY, Park SJ. Effects of exfoliated graphite on the thermal properties of erythritol-based composites used as phase-change materials. Compos Part B. 2016;96:350–3.10.1016/j.compositesb.2016.04.033Suche in Google Scholar

6. Luo Z, Zhang Q, Wu G. Preparation and enhanced heat capacity of nano-titania doped erythritol as phase change material. Int J Heat Mass Tran. 2015;80:653–9.10.1016/j.ijheatmasstransfer.2014.09.069Suche in Google Scholar

7. Agyenim F, Eames P, Smyth M. Experimental study on the melting and solidification behaviour of a medium temperature phase change storage material (erythritol) system augmented with fins to power a LiBr/H2O absorption cooling system. Renew Energ. 2011;36:108–17.10.1016/j.renene.2010.06.005Suche in Google Scholar

8. Kaizawa A, Kamano H, Kawai A. Technical feasibility study of waste heat transportation system using phase change material from industry to city. ISIJ Int. 2008;48:540–8.10.2355/isijinternational.48.540Suche in Google Scholar

9. Sun ZL, Zhou Y, Jia DC. Mechanical and thermal physical properties of amorphous SiCN(O) ceramic bulks prepared by hot-press sintering. Mater Lett. 2012;72:57–9.10.1016/j.matlet.2011.12.053Suche in Google Scholar

10. Qiu Z, Ma X, Zhao X. Mechanical and thermal physical properties of amorphous SiCN(O) ceramic bulks prepared by hot-press sintering. Appl Energ. 2016;165:260–71.10.1016/j.apenergy.2015.11.053Suche in Google Scholar

11. Xiao X, Zhang P, Li M. Preparation and thermal characterization of paraffin/metal foam composite phase change material. Appl Energ. 2013;112:1357–66.10.1016/j.apenergy.2013.04.050Suche in Google Scholar

12. Ling Z, Chen J, Xu T. Thermal conductivity of an organic phase change material/expanded graphite composite across the phase change temperature range and a novel thermal conductivity model. Energ Convers Manag. 2015;102:202–8.10.1016/j.enconman.2014.11.040Suche in Google Scholar

13. Berber E, Horzum N, Hazer B. Solution electrospinning of polypropylene-based fibers and their application in catalysis. Fiber Polym. 2016;17:760–8.10.1007/s12221-016-6183-7Suche in Google Scholar

14. Li C, Xu G. Preparation of the high dielectric performance flexible materials achieved by polyacrylamide/poly(vinylidene fluoride) blends. e-Polymers 2011;11:127.10.1515/epoly.2011.11.1.892Suche in Google Scholar

15. Yang Q, Yu J, Ma J. Electrospinning of GeO2–C fibers and electrochemical application in lithium-ion batteries. Chinese Chem Lett. 2016;27:412–6.10.1016/j.cclet.2015.12.025Suche in Google Scholar

16. Suwantong O. Biomedical applications of electrospun polycaprolactone fiber mats. Polym Advan Technol. 2016;27:1264–73.10.1002/pat.3876Suche in Google Scholar

17. Zhang C, Yuan X, Wu L. Drug-loaded ultrafine poly(vinyl alcohol) fibre mats prepared by electrospinning. e-Polymers. 2005;5:750.10.1515/epoly.2005.5.1.750Suche in Google Scholar

18. Chen C, Wang L, Huang Y. Electrospinning of thermo-regulating ultrafine fibers based on polyethylene glycol/cellulose acetate composite. Polymer 2007;48:5202–7.10.1016/j.polymer.2007.06.069Suche in Google Scholar

19. Chen C, Liu K, Wang H. Morphology and performances of electrospun polyethylene glycol/poly (dl-lactide) phase change ultrafine fibers for thermal energy storage. Sol Energ Mater Sol C. 2013;117:372–81.10.1016/j.solmat.2013.07.001Suche in Google Scholar

20. Chen C, Zhao Y, Liu W. Electrospun polyethylene glycol/cellulose acetate phase change fibers with core–sheath structure for thermal energy storage. Renew Energ. 2013;60:222–5.10.1016/j.renene.2013.05.020Suche in Google Scholar

21. Cai Y, Xu X, Gao C. Structural morphology and thermal performance of composite phase change materials consisting of capric acid series fatty acid eutectics and electrospun polyamide6 nanofibers for thermal energy storage. Mater Lett. 2012;89:43–6.10.1016/j.matlet.2012.08.067Suche in Google Scholar

22. Chen C, Wang L, Huang Y. Ultrafine electrospun fibers based on stearyl stearate/polyethylene terephthalate composite as form stable phase change materials. Chem Eng J. 2009;150:269–74.10.1016/j.cej.2009.03.007Suche in Google Scholar

23. Ke H, Li Y, Wang J. Ag-coated polyurethane fibers membranes absorbed with quinary fatty acid eutectics solid-liquid phase change materials for storage and retrieval of thermal energy. Renew Energ. 2016;99:1–9.10.1016/j.renene.2016.06.033Suche in Google Scholar

24. Lu Z, Xu B, Zhang J. Preparation and characterization of expanded perlite/paraffin composite as form-stable phase change material. Sol Energ. 2014;108:460–6.10.1016/j.solener.2014.08.008Suche in Google Scholar

25. Ge Z, Ye F, Ding Y. Composite materials for thermal energy storage: enhancing performance through microstructures. Chemsuschem. 2014;7:1318–25.10.1002/cssc.201300878Suche in Google Scholar PubMed PubMed Central

26. Ji H, Sellan DP, Pettes MT. Enhanced thermal conductivity of phase change materials with ultrathin-graphite foams for thermal energy storage. Energ Environ Sci. 2013;7:1185–92.10.1039/C3EE42573HSuche in Google Scholar

27. Harish S, Orejon D, Takata Y. Thermal conductivity enhancement of lauric acid phase change nanocomposite in solid and liquid state with single-walled carbon nanohorn inclusions. Thermochim Acta. 2015;600:1.10.1016/j.tca.2014.12.004Suche in Google Scholar

28. Zhou Y, Jiang Y, Liu F. Thermal conductivity and thermal mechanism of aluminum nanoparticles/octadecane composite phase change materials from molecular dynamics simulations and experimental study. J Ovo Res. 2016;12:49.Suche in Google Scholar

29. Cai Y, Ke H, Dong J. Effects of nano-SiO2 on morphology, thermal energy storage, thermal stability, and combustion properties of electrospun lauric acid/PET ultrafine composite fibers as form-stable phase change materials. Appl Energ. 2011;88:2106–12.10.1016/j.apenergy.2010.12.071Suche in Google Scholar

30. Susiani, Harsoyo. Fabrikasi fiber PVA yang memuat partikel TiO2 dengan metode elektrospining dan potensi aplikasinya. Chem Ing Tech. 2014;57:715.Suche in Google Scholar

31. Babapoor A, Karimi G, Khorram M. Fabrication and characterization of nanofiber-nanoparticle-composites with phase change materials by electrospinning. Appl Therm Eng. 2016;99:1225–35.10.1016/j.applthermaleng.2016.02.026Suche in Google Scholar

32. Cai Y, Gao C, Zhang T. Influences of expanded graphite on structural morphology and thermal performance of composite phase change materials consisting of fatty acid eutectics and electrospun PA6 nanofibrous mats. Renew Energ. 2013;57:163–70.10.1016/j.renene.2013.01.044Suche in Google Scholar

33. Cai Y, Gao C, Wang L. Effects of carbon nanotubes on morphological structure, thermal and flammability properties of electrospun composite fibers consisting of lauric acid and polyamide 6 as thermal energy storage materials. Fiber Polym. 2012;13:837–45.10.1007/s12221-012-0837-xSuche in Google Scholar

34. Wang J, Xie H, Guo Z. Improved thermal properties of paraffin wax by the addition of TiO2 nanoparticles. Appl Therm Eng. 2014;73:1541–7.10.1016/j.applthermaleng.2014.05.078Suche in Google Scholar


Supplementary Material:

The online version of this article offers supplementary material (https://doi.org/10.1515/epoly-2017-0176).


Received: 2017-09-02
Accepted: 2017-12-26
Published Online: 2018-07-03
Published in Print: 2018-07-26

©2018 Walter de Gruyter GmbH, Berlin/Boston

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