Figure 2(a) shows a typical SEM image of BTONWs synthesized through hydrothermal method, and the diameter of the BTONWs range from 80 to 200nm. To investigate the crystalline property, the as-grown BTONWs were analyzed by XRD. It can be seen from the Fig. 2. that all the reflection peaks show a tetragonal crystal structure, similar work has been found in [17]. Figure 2(b) show the distribution of the electric field around a rectangular electrode at different electric field strengths. The upper figure shows the distribution at lower electric field strengths, while the lower figure shows the distribution at higher electric field strengths. The electric field strength in the lower figure is significantly higher than that in the upper figure, indicating that the strength and range of the electric field can be significantly enhanced by increasing the electric field strength for the same electrode arrangement.
When the two films are squeezed close together, the potential difference reaches a minimum value. With the gradual release of the external force, the potential difference between the two films gradually increases. The whole process keeps cycling and the potential difference is minimised again. In the experiment, the operation mechanism of TENG is the vertical contact separation method of reciprocating motion.
Figure 3 (a) This figure shows the physical image of TENG fabricated using nylon11/BTONWs -PVDF. Figure 3(b) This figure shows the SEM image of nylon 11 fibres. It can be clearly shown in the image that the nylon 11 fibres exhibit a homogeneous network structure with relatively uniform fibre diameters, which are tightly aligned and have no obvious breaks or defects. This homogeneous fibre network helps to increase the surface area of the material, thus enhancing the friction electric effect. The smoothness and continuity of the fibre surface indicate that better process parameters were controlled during the preparation process to ensure the integrity and consistency of the fibres. Figure 3(c) is the SEM image of the negative friction electric layer BTONWs-PVDF. it shows in the image that the BTONWs-PVDF fibres form a more dense network structure, with the fibres interleaved with each other, constituting a complex three-dimensional network. Compared with the nylon 11 fibres, the BTONWs-PVDF fibres have a slightly different diameter distribution and a slightly rougher surface. This rough surface property contributes to the fibres' friction electrical properties, as the larger surface area increases charge generation and accumulation. The interwoven structure of the fibres ensures the mechanical stability and durability of the material while enhancing its potential as a friction material for TENG. These structural features enable the BTONWs-PVDF fibres to exhibit excellent performance in energy harvesting and conversion. Figure 3(d) demonstrates the SEM images of PVDF fibres doped with different mass ratios of BTONWs. The PVDF fibres doped with 1 wt% BTONWs formed a uniform and dense network structure, and the fibres were interspersed with each other to form a stable three-dimensional structure. The PVDF fibres doped with 2 wt% BTONWs had a denser network and increased surface area compared to 1 wt% doping, indicating that more BTONWs nanowires were successfully doped into the fibres. The structure of PVDF fibres doped with 3 wt% BTONWs was denser than the first two doping ratios, indicating that more BTONWs nanowires were contained within the fibres. Figure 3(e) is a scaled SEM of different doping ratios of BTONWs up to 1 um. The PVDF fibres doped with 1 wt% BTONWs show the details of the fibres. The surface of the fibres was slightly rough and the nanowires of BTONWs were uniformly distributed in the PVDF fibres, which enhances the mechanical strength and electrical properties of the material. The PVDF fibres doped with 2 wt% BTONWs show a higher percentage of BTONWs nanowires uniformly distributed inside the fibres, with a rougher fibre surface. This roughness further enhanced the friction electrical properties and helped to improve the electrical output of TENG. The PVDF fibres doped with 3 wt% BTONWs demonstrated a highly doped fibre structure. Although the surface roughness and the distribution of BTONWs increased further, excessive doping may lead to a decrease in the mechanical properties of the fibres. The surface roughness and structural density of the PVDF fibres increased as the percentage of BTONWs doping increased. These changes contribute to the improvement of the friction electrical properties, but there is also a need to find a balance between the mechanical and electrical properties to optimise the overall performance of the TENG. The XRD pattern of BTONWs is illustrated in Fig. 3(f), which shows the main diffraction peaks of BTONWs. Several distinct diffraction peaks are labelled in the figure, which appear in the range of 20° to 60°, corresponding to different crystal planes of the barium titanate crystals. The strongest diffraction peak is obtained from the (110) crystal plane, which appears at about 31.5 degrees, showing that the barium titanate nanowires have the strongest crystal orientation at the (110) crystal plane, and indicating the high crystallinity and good crystal structure of BTONWs. The clarity and intensity of the peaks show that the barium titanate nanowires have good crystal quality and well-defined orientation, and the high crystallinity and good orientation help to improve the electrical properties of the material. Figure 3(g) demonstrates the IR patterns of BTONWs doped PVDF with different mass ratios. Significant absorption peaks appear at about 1275 cm-¹ and 840 cm-¹, which correspond to the characteristic vibrations of the α-phase and β-phase crystalline forms of PVDF, respectively. The intensity of the β-phase vibration peaks (1275 cm-¹) increased with the increase of the mass ratio of BTONWs, while the α-phase vibration peaks (840 cm-¹) did not change much.The intensity of the β-phase vibration peaks increased while the α-phase vibration peaks gradually weakened at 840 cm-¹. The β-phase content of PVDF increases and the α-phase content decreases as the doping ratio of BTONWs increases. These IR spectral patterns indicate that the doping of BTONWs effectively promotes the crystallisation of the β-phase of PVDF, thus enhancing the friction electrical properties of the material. The β-phase crystallisation of PVDF is most significant at 3 wt% doping of BTONWs, indicating that the electrical properties of the material are optimal at this doping ratio. Through these IR spectra, Fig. 3(h) shows the XRD patterns of doped BTONWs in PVDF with different mass ratios. These XRD patterns indicate that the doping of BTONWs effectively promotes the crystallisation of the β-phase of PVDF, which enhances the friction electrical properties of the material. The β-phase crystallisation of PVDF is most significant at 3 wt% doping of BTONWs, indicating that the electrical properties of the material are optimal at this doping ratio.
Figure 4(a-c) display the performance metrics of a TENG with varying weight percentages of a material, likely BaTiO₃nanoparticles, mixed with PVDF. The graphs illustrate the short-circuit current, open-circuit voltage, and transferred charge quantity over time for TENGs containing 0 wt%, 1 wt%, 2 wt%, and 3 wt% of the material. The TENG with 2 wt% achieves the highest short-circuit current, peaking around 12㎂, demonstrating the most significant enhancement in electrical output. The 2 wt% TENG shows the highest open-circuit voltage, peaking around 240V, indicating the best performance in this series. The 2 wt% TENG exhibits the highest charge transfer quantity, peaking near 120nC. The 2 wt% concentration of BaTiO₃ in PVDF consistently provides the highest short-circuit current, open-circuit voltage, and transferred charge quantity, making it the optimal concentration for maximizing the TENG's electrical output. The 3 wt% concentration, while still improved over the baseline, does not perform as well as the 2 wt%, suggesting that an excess of the material might hinder the performance improvements. This analysis underscores the importance of optimizing material concentrations in the design and fabrication of high-performance TENGs.
Figure 4(d) demonstrates the variation of dielectric constant of BTONWs doped PVDF with different mass percentages as a function of frequency, ranging from 102 to 106 Hz.The dielectric constants of PVDF were significantly increased with the increase in the doping ratio of BTONWs. This indicates that the doping of BTONWs can effectively enhance the electrical properties of PVDF. The trend of decreasing dielectric constant with increasing frequency at all doping ratios may be related to the agglomeration. The aggregation reduces the effective surface area of the nanoparticles, weakens the interfacial polarisation effect, increases the conductivity loss, and leads to inhomogeneity in the internal structure and electric field distribution of the material.
Figure 5(a) plots the relationship between load resistance and both voltage and current. As the load resistance increases, the voltage initially rises, reaching a peak around 175V at an optimal resistance. Conversely, the current decreases with increasing resistance, indicating a trade-off between voltage and current. Figure 5(b) illustrates the power output as a function of resistance. The power output shows a sharp increase, peaking at around 0.648㎽ at 90㏁, and then gradually decreases as the resistance increases further. This confirms the optimal resistance for maximum power output, highlighting the importance of matching the load resistance to the TENG for efficient energy harvesting. Figure 5(c) shows the voltage as a function of time under different patting speeds. Initially, the TENG is subjected to slow patting, resulting in lower and more spaced-out voltage peaks. When the patting speed increases, the voltage peaks become more frequent and higher in magnitude, demonstrating the TENG’s responsiveness to varying mechanical inputs. Returning to slow patting shows a decrease in both frequency and magnitude of the voltage peaks. The external circuit diagram used for the experiment is shown in Fig. 5(d), Fig. 5(e) shown physical diagram of TENG of BTONWs-PVDF. In this experiment, a TENG was tested for its capability to generate and store electrical energy by continuously patting the device. The TENG's performance was evaluated by its ability to power a calculator, a timer, and an array of LED lights. The objective was to demonstrate the practical application of TENG in powering everyday electronic devices.The initial step involved connecting the TENG to a calculator. The calculator, as shown in Fig. 5(f), was initially off. After a series of pats on the TENG, the calculator powered on, displaying "666" on its screen. This indicated that the TENG successfully generated enough power to operate the calculator and was connected to a digital timer, depicted in Fig. 5 (g). Similar to the calculator, the timer was initially off. After patting the TENG, the timer powered on, displaying the time "1:37." This further validated the TENG's capability to generate and store sufficient energy for practical use. Finally, TENG drives an array of LEDs by rectifying them.. Figure 5 (h-i) shown the yellow and green LED array before and after being powered by the TENG. Initially, the LEDs were off. Upon patting the TENG, the yellow and green LEDs lit up, demonstrating the TENG's ability to provide continuous and reliable power to light multiple LEDs. This part of the experiment showcased the TENG's potential for lighting applications, especially in low-power scenarios.
Through these experiments, the TENG demonstrated its efficiency in generating and storing energy, enough to power common electronic devices like calculators, timers, and LED lights. The results underline the practical potential of TENG technology for sustainable and portable energy solutions in real-world applications.