Meilin Liab,
Bei Jiangab,
Shuoang Caoab,
Xinyi Songab,
Yuanqiao Zhangab,
Lijun Huangab and
Quanping Yuan*ab
aSchool of Resources, Environment and Materials, Guangxi University, Nanning 530004, China. E-mail: yuanquanping@gxu.edu.cn
bState Key Laboratory of Featured Metal Materials and Life-cycle Safety for Composite Structures, MOE Key Laboratory of New Processing Technology for Nonferrous Metals and Materials, Guangxi University, Nanning 530004, China
First published on 31st March 2023
High-performance flexible barium titanate (BaTiO3)-based piezoelectric devices have gained much attention. However, it is still a challenge to prepare flexible polymer/BaTiO3-based composite materials with uniform distribution and high performance due to the high viscosity of polymers. In this study, novel hybrid BaTiO3 particles were synthesized with assistance of TEMPO-oxidized cellulose nanofibrils (CNFs) via a low-temperature hydrothermal method and explored for their application in piezoelectric composites. Specifically, Ba2+ was adsorbed on uniformly dispersed CNFs with a large amount of negative charge on their surface, which nucleated, resulting in the synthesis of evenly dispersed CNF-BaTiO3. The obtained CNF-BaTiO3 possessed a uniform particle size, few impurities, high crystallinity and dispersity, high compatibility with the polymer substrate and surface activity due to the existence of CNFs. Subsequently, both polyvinylidene fluoride (PVDF) and TEMPO-oxidized CNFs were employed as piezoelectric substrates for the fabrication of a CNF/PVDF/CNF-BaTiO3 composite membrane with a compact structure, displaying the tensile strength of 18.61 ± 3.75 MPa and elongation at break of 3.06 ± 1.33%. Finally, a thin piezoelectric generator (PEG) was assembled, which output a considerable open-circuit voltage (4.4 V) and short-circuit current (200 nA), and could also power a light-emitting diode and charge a 1 μF capacitor to 3.66 V in 500 s. Its longitudinal piezoelectric constant (d33) was 5.25 ± 1.04 pC N−1 even with a small thickness. It also exhibited high sensitivity to human movement, outputting a voltage of about 9 V and current of 739 nA for only a footstep. Thus, it exhibited good sensing property and energy harvesting property, presenting practical application prospects. This work provides a new idea for the preparation of hybrid BaTiO3 and cellulose-based piezoelectric composite materials.
However, it is challenging to prepare homogeneous composite materials with high performance because most flexible substrates are sticky and hydrophobic, making it difficult for nanoparticles to be sufficiently separated and dispersed. Considering these difficulties, the approach to add conductive materials as dispersants and a third phase material in the composites to form a hybrid structure, such as carbon nanotubes,13 conductive polymers,14 graphene15 and metal nanorods,16 has been developed.17 Moreover, it is feasible to prepare polymer composites containing BaTiO3-based hybrid particles with a core–shell structure, which exhibit good dispersity, fast response and high piezoelectric performance.18,19 In addition, it has been demonstrated that three-phase BaTiO3-based nanocomposites with a combination of either fillers or polymer matrix exhibit enhanced dielectric properties.20
In the case of the synthesis of BaTiO3, traditionally, industry mainly employ the solid-state reaction, which has the drawbacks of producing materials with a large particle size, uneven distribution, impurities, and low chemical activity.21 The electrical properties of BaTiO3 are highly dependent on its high purity, sintering property and uniform distribution.22 Thus, many methods, such as precipitation method,23 sol–gel method,24 hydrothermal method25–27 and other wet chemical methods have been developed to overcome these problems. Particularly, BaTiO3 prepared via the hydrothermal method has the advantages of lower impurity content, higher chemical activity, intact grain structure, small and uniform particle size distribution, less agglomeration and high sintering activity, as well as low cost and environmental friendliness.28 Notably, although its stoichiometry is affected by the solvent and dosage, this disadvantage disappears during large-scale production.22 The published research on the synthesis of BaTiO3 mainly focused on the effect of the Ti/Ba mole ratio,29 reaction temperature,25,30 reaction time,30 and pH30,31 of the reaction system on the structure and properties of BaTiO3. Moreover, BaTiO3 can be grown on some substrates via hydrothermal synthesis, such as multi-walled carbon nanotubes32 and graphene oxide (GO) to enhance its structure. In the hydrothermal growth of BaTiO3, the base of GO with abundant oxygen-containing groups alters the morphology of BaTiO3 and narrows its size distribution, also achieving its homogeneous distribution. Specially, the oxygen-containing groups of GO can heal the oxygen vacancies in the hybridized BaTiO3, which improve its piezoelectric properties.33
Cellulose nanofibrils (CNF), as a type of natural cellulose material, have a high specific surface area, length–diameter ratio, strength and film-forming performance, as well as certain piezoelectric properties. Accordingly, they can be assembled into a variety of nanostructures to meet the design requirements of energy devices. The addition of eco-friendly nanocellulose to energy-related devices is very promising in solving the related environmental problems. Moreover, it has been demonstrated that nanocellulose is an excellent dispersion medium.34 Therefore, it can further solve the problem of easy aggregation of the filler in the polymer matrix to a certain extent. After TEMPO treatment, the hydroxyl groups can be oxidized to carboxy groups, and consequently CNFs exhibit higher dispersity,35,36 which can play a similar role to GO.33
In this work, CNFs with abundant carboxy groups were prepared using a method involving the TEMPO-NaBr-NaClO system and directly added to synthesize BaTiO3 via a low-temperature hydrothermal method. Subsequently, BaTiO3 was combined with two substrates of PVDF and CNFs via ultrasonic dispersion, self-assembly, and hot pressing to fabricate the CNF/PVDF/CNF-BaTiO3 piezoelectric composite membrane. In the reaction system, the metal cations (Ba2+) adsorbed on the surface oxygen-containing groups of CNFs acted as nucleation points to improve the size distribution and crystal structure. The excessive contact and aggregation of BaTiO3 particles could be inhibited by the stable network structure constructed by TEMPO-oxidized CNF. Furthermore, the uniform dispersion of the synthesized BaTiO3 was effectively improved and its particle size reduced. Intriguingly, CNF-BaTiO3 is compatible with PVDF and CNFs in aqueous media, and the combination of CNF-BaTiO3 and the substrates should be very compact. Consequently, the flexible piezoelectric composite membranes exhibited a considerable piezoelectric effect to collect mechanical energy and sensing performance for health monitoring. This study has high reference value for the modification and improvement of the structure and properties of BaTiO3 and piezoelectric functionalization of CNF.
CNFs with various oxidation degrees were prepared using various contents of NaClO (4, 6, 8, 10, 12, and 14 mmol g−1) and adopted to synthesize a series of CNF-BaTiO3, denoted as 4CNF-BaTiO3, 6CNF-BaTiO3, 8CNF-BaTiO3, 10CNF-BaTiO3, 12CNF-BaTiO3, and 14CNF-BaTiO3, respectively. In addition, BaTiO3 powder without CNF was prepared via the same method, which was named 0CNF-BaTiO3.
The above-mentioned three types of solution were mixed via an ultrasonic process (1000 W, 30 min), followed by vacuum filtration using a 0.22 μm organic filter, and then left in the air for 1 h. Afterwards, the obtained composite membrane was placed in two plates of a pressing machine at 60 °C for 8 h, and then the composite membranes were obtained.
The composite membrane was cut into small pieces with a size of 1 cm × 1 cm. Subsequently, it was directly affixed with Cu–Ni conductive tape (0.9 cm × 0.9 cm) to a polyimide (PI) film, as shown in Fig. 1. The composite membranes prepared with the series of CNF-BaTiO3 were named CNF/PVDF/4CNF-BaTiO3, CNF/PVDF/6CNF-BaTiO3, CNF/PVDF/8CNF-BaTiO3, CNF/PVDF/10CNF-BaTiO3, CNF/PVDF/12CNF-BaTiO3, CNF/PVDF/14CNF-BaTiO3 and CNF/PVDF/0CNF-BaTiO3 piezoelectric composite membrane, respectively. Alternatively, the cut composite membrane was further hot pressed for 30 min at 170 °C under 20 MPa, and then affixed to electrodes to form the hot-pressed piezoelectric composite membranes.
After the piezoelectric composite membranes were encapsulated with two pieces of PI films, piezoelectric generators (PEGs) containing the various CNF-BaTiO3 were finally fabricated according to the above-mentioned process. The specific process for the preparation of the composite membrane and PEG can is presented in Fig. 1.
The spacing of the crystal plane of the synthesized 10CNF-BaTiO3 was determined to be 0.28 nm via HRTEM analysis, as shown in Fig. 2d and e, and the (111), (200), and (220) crystal faces corresponding to BaTiO3 were observed in the SAED pattern and FFT analysis, as shown in Fig. 2f.42,43 As shown in Fig. 2g, the diffraction peaks of CNF-BaTiO3 appeared at the 2θ values of 22.16°, 31.52°, 38.83°, 45.12°, 50.79°, 56.04°, and 65.66°, respectively, corresponding to the Bragg reflection of the (100), (110), (111), (200), (210), (211), and (220) crystal faces, respectively. Based on the XRD diffraction pattern of BaTiO3 and the PDF card (JCPDS card no. 31-0174), it was confirmed that BaTiO3 was synthesized on the CNF substrate, and the weak peak appearing at around 24° indicates the presence of a small amount of BaCO3 impurity in CNF-BaTiO3 (JCPDS card No. 05-0378).44 However, the relatively weak characteristic peak of CNFs could be hardly seen in the pattern of CNF-BaTiO3 due to their small addition amount. Thus, the results proved that CNFs were uniformly distributed in BaTiO3 and was completely incorporated in BaTiO3.45,46 According to the calculated data in Table S2,† the c/a ratio of all the samples was greater than 1. When the CNFs were prepared with 10 mmol g−1 NaClO, the c/a ratio of the synthesized BaTiO3 grain was the lowest with a higher crystallinity of 87%. All the diffraction peaks observed in Fig. 2g mainly correspond to that of BaTiO3, indicating that the products obtained under CNF-assisted hydrothermal synthesis are BaTiO3 with a small amount of impurities. In addition, all the diffraction peaks have high intensity, indicating its high crystallinity. Compared with the sample without CNFs, all the CNF-BaTiO3 samples exhibited stronger diffraction peaks attributed to the lattice (200) plane at around 45.12°, which shows the effective assistance of CNF in the synthesis of BaTiO3.
As shown in Fig. 2h, the strong absorption peak at 500–700 cm−1 corresponds to TiO32− in CNF-BaTiO3 synthesized with the help of various CNFs,46,47 indicating the existence of BaTiO3. The other obvious strong absorption band at about 2900–3700 cm−1 is attributed to the stretching vibration absorption of –OH41 and the hydrogen bonds between the oxygen-containing groups in CNFs and water of crystallization. The peaks at 2928 cm−1 and 2858 cm−1 are the asymmetric and symmetric stretching peaks of –CH2–, respectively. The peak at around 1630 cm−1 is attributed to the stretching vibration of CO and the stretching vibration peak of H–OH, and the peak at 1000–1200 cm−1 corresponds to the C–O stretching vibration and absorption peaks of structural water. These peaks in the FTIR spectra represent the presence of TEMPO-oxidized CNFs in the synthesized product. Thus, combined with the XRD analysis, it can be concluded that CNF-BaTiO3 was successfully synthesized. The value of the peak for CO slightly shifted to a lower wavenumber in CNF-BaTiO3 compared to that without CNF assistance because the hydroxide ion (OH−) on the BaTiO3 surface may be bonded with CNFs through hydrogen bonds.48,49 Furthermore, a weak absorption band appeared at 860 cm−1, corresponding to the out-of-plane bending vibration of the CO32− group, and an absorption peak at 1450 cm−1, which is attributed to the asymmetric stretching vibration of the CO32− group, indicating the presence of very few BaCO3, similar to the result for BaTiO3-based piezoelectric composites.42 Among the peaks, the absorption intensity of the peak for the CNF oxygen functional group decreased obviously, indicating the presence of a high content of BaTiO3 in the hybrid particles. The results of the FTIR analysis are in good agreement with the XRD analysis results. The BaTiO3 prepared with the assistance with CNF had fewer OH− defects compared with that without the assistance of CNFs. Given that CNFs with a high oxidation degree were adopted, CNF-BaTiO3 contained little BaCO3 impurity. The above-mentioned results demonstrate that the addition of CNFs contributed the small particle size, uniform dispersion and high crystallinity of the hybrid BaTiO3.
It can be observed in the cross section image (Fig. 3b–d, f–h and j–l) that the composite membranes have a significantly layered stack structure, which became similar fiber-crosslinked structures after hot pressing. In the magnified cross-section image of that with CNF-BaTiO3, obvious gap exists before hot pressing (Fig. 3h), which were also retained to a certain degree after hot pressing (Fig. 3l). The content of hybrid BaTiO3 particle (50 wt%) in the composite membrane was high, and the PVDF fused in the hot-pressing process could not completely fill the gaps among the particles, thus forming slight pores. The elemental analysis at the cross section of the piezoelectric composite membrane (Fig. 3m–p and S2d†) further demonstrated that CNF, PVDF and CNF-BaTiO3 were evenly distributed in the composite membrane.
As shown in Fig. 4a, the Bragg reflection of the (100), (110), (111) and (200) crystal faces of BaTiO3 appear in the composite membrane, while that of PVDF is very weak (Fig. 4b), which can be attributed to the combination of BaTiO3 and presence of CNF. After hot pressing, the characteristic diffraction peak at 21.9° of CNFs decreased obviously (Fig. 4c), while the absorption peak of BaTiO3 increased. According to the FTIR analysis, as shown in Fig. 4d and e, the characteristic absorption peaks of the α-phase of PVDF appeared at 762 cm−1 and 799 cm−1 for the hot-pressed composite membrane, while the characteristic peaks of the β-phase of PVDF were located at 847 cm−1, 876 cm−1, and 1284 cm−1 for the hot-pressed composite membrane. In the case of the unpressed composite membrane, the characteristic absorption peaks of the α-phase of PVDF were found at 761 cm−1 and 795 cm−1, as well as the characteristic peaks at 842 cm−1, 877 cm−1, and 1280 cm−1 for the β phase.50,51 By contrast, the ratio of β phase to α phase in the composite membrane after hot pressing increased.
According to the tensile performance of the CNF/PVDF/CNF-BaTiO3 piezoelectric composite membrane, as shown in Fig. 4f and Table S3,† the tensile strength of the pure CNF membrane is 24.98 ± 4.17 MPa with the elongation at break of 10.13 ± 3.18% and Young's modulus of 873.39 ± 260.25 MPa. These values for the piezoelectric composite membranes prepared using various CNF-BaTiO3 without hot pressing were 22.54 MPa, 3.46%, and 1130.30 MPa, respectively. There is little difference in the tensile performance of the various composite membranes prepared using different contents of NaClO. Among them, the CNF/PVDF/10CNF-BaTiO3 composite membrane exhibited considerable tensile strength of 18.61 ± 3.75 MPa and elongation at break of 3.06 ± 1.33%. Combined with the particle size and FTIR analysis, it can be seen that the structure of the composite membrane is denser because the particle size of CNF-BaTiO3 was relatively small and its –OH defect was less due to the assisted synthesis with CNFs, which is conducive to the interface bonding. Compared with that of the composite membrane containing the synthesized BaTiO3 without CNFs, the tensile strength was slightly enhanced with a considerable elongation at break. This confirms that the assistance of CNF elevated the surface activity on the synthesized CNF-BaTiO3, which contributes to the interface bonding of CNF-BaTiO3 to CNF and PVDF.
After hot pressing, the tensile performance of the composite membrane, as shown in Fig. 4g and Table S4,† gradually increased with an increase in the oxidation degree of the CNFs, resulting in the construction of a network gluing structure among the particles (as seen in Fig. 3l). The tensile performance reached the highest at 14 mmol g−1 with the tensile strength of 18.32 ± 3.31 MPa, as well as the higher elongation at break of 4.66 ± 1.32% than that of the unpressed composite membrane, indicating its enhanced flexibility. However, when the oxidation level of CNFs was low, the tensile strength decreased by more than 50% relative to the unpressed composite membrane, which may be caused by the large holes formed in the compressed composite membrane (Fig. S2e and f†).
Moreover, the piezoelectric output performance of the PEGs prepared using BaTiO3 synthesized with the assistance of CNFs with different oxidation degrees was measured under repeated impact compression test with the maximum force of 40 N at the frequency of 2.2 Hz (Video S1†) using a charge acquisition system, which was exhibited in our previous work,54 and the output is shown in Fig. 5d, e, g, and h. The test results show that all samples demonstrated typical piezoelectric properties under periodic external force. Initially, when there was no impact or vibration on the PEG, there was no piezoelectric output because its electric dipoles randomly oscillated within a degree of their respective alignment axes, maintaining a macroscopic equilibrium state in the composite membrane. When the PEG was subjected to a vertical mechanical impact, which made it compressed, a potential difference was formed between the two electrodes, resulting in the flow of electrons between the two electrodes, and thereby a positive signal was observed. Conversely, when the impact force disappeared, the deformation of the PEG was restored and a negative electrical signal could be detected. Obviously, the output performance of the PEGs with CNF-BaTiO3 was better than that of the PEG with the pure CNF membrane. With an increase in the oxidation degree of CNFs, the output signal strength of the PEG increased firstly, and then decreased, among which the CNF/PVDF/10CNF-BaTiO3 PEG exhibited the highest output with the VOC of 3.6 V and ISC of 200 nA. It can be found that the changing trend of the d33 of the PEGs is consistent with the output results, as shown in Fig. 5d and e. The functional groups of –COO− on the CNF molecular chains serve as nucleation sites for the growth of the BaTiO3 NPs,33 and then the dispersed BaTiO3/CNFs can support the growth of BaTiO3. Simultaneously, the existence of CNFs also limited the growth of BaTiO3. As the dosage of NaClO increased, the prepared CNFs contained more –COO− groups, while the molecular chain length decreased. The output current value increased gradually, and then decreased, which reached the maximum value at 10CNF. It is possible that the BaTiO3 prepared with 10CNF had fewer surface defects and agglomeration, and thus it exhibited better piezoelectric property.
After hot pressing, the output signal changed, and the PEG assembled by using the composite membrane incorporating CNFs with a low oxidation degree showed an increasing trend, while that of the PEG assembled using CNFs with a high oxidation degree did not increase and exhibited a decreasing trend. Among them, the PEG with 4CNF-BaTiO3-based composite membrane exhibited the largest increasing trend. The existing slight difference in the peak value may be due to the difference in strain rate during extrusion or release. The asymmetric positive peak value and negative peak value can be caused by external force during extrusion.40 The specific mechanism for its piezoelectric performance can be seen in Fig. 5a. The PEG remains balanced in the absence of external force, and when mechanical stress was applied, the dipoles in the PEG rearranged and generated a piezoelectric potential between the top and bottom electrodes. The instantaneous internal potential then moved the electrons through an external circuit to neutralize the electric field generated by the substituted dipole. When the PEG was not stressed, the piezoelectric potential disappeared and the opposite built-in potential in the circuit built up simultaneously. Consequently, the electrons flowed back in the opposite direction.55
Subsequently, the unpressed CNF/PVDF/10CNF-BaTiO3 PEG was applied to further explore its potential in actual sensing and energy harvesting application. Fig. 5f and i show the long-term test results of the CNF/PVDF/10CNF-BaTiO3 PEG, where its output performance was normal even in the 1300 cycles after being stable, displaying its good durability. It also showed a gradually increasing trend of VOC from 4 V to 6 V in 500 s. The CNF/PVDF/10CNF-BaTiO3 PEG was connected to a rectifier bridge to charge a 1 μF capacitor (Fig. 5j). Under the exciting force of 40 N at the frequency of 2.2 Hz, the voltage of the capacitor could be charged to reach 3.66 V in 500 s, which is comparable to that of a previously reported cellulose-based generator.56 In addition, the PEG could power a light-emitting diode, as shown in Fig. 5k and Video S2.†
The piezoelectric sensing performance of the PEG (as a sensor) was further explored. As shown in Fig. 6a and b, a polytetrafluoroethylene (PTFE) film was placed on a subplate to avoid the triboelectricity effect, on which the sensor was fixed with PI insulating tape. Then an iron block with a weight of 150 g was dropped vertically from different heights, and the recorded piezoelectric output VOC and ISC are shown in Fig. 6c and d, respectively. The output signal strength was proportional to the stress, where the maximum output VOC and ISC of the sensor could reach as high as 4.5 V and 0.7 μA, respectively, under the stress stimulation of about 20 kPa by the block. Moreover, Fig. 6e shows the piezoelectric signal generated by vertically dropping iron blocks with different masses from a height of 4 cm on the composite membrane sensor, also displaying a high ISC of 0.6 μA under stimulation by a block with the light weight of 6 g. Thus, these results prove that the composite membrane exhibited a considerable sensing performance with high sensitivity, and even captured weak mechanical energy.
As shown in Fig. 6f–h, when the PEG was repeatedly pressed by a finger (Video S3†), the output VOC of about 2 V and ISC of 180 nA were generated, which are comparable to the results in a similar work.57 Then, the PEG was transferred to a keyboard (Fig. 6i–k) and it could generate an output of about 1–2 V and 170 nA under the knock by a finger (Video S4†), similar to that in Fig. 6f–h. In addition, the PEG was fixed on the ground to simulate the energy harvesting from human movement (Fig. 6l–n), and then it was stepped on with a foot, exhibiting a higher output with VOC of about 9 V and ISC of 739 nA, which are comparable to the results of similar work.58 Of course, the output data fluctuated slightly during the test, which is due to the fact that the loading magnitude and point of the force cannot be ensured to be completely consistent.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ra00604b |
This journal is © The Royal Society of Chemistry 2023 |