3.1 Effect of Nacl on the mechanical properties of CSIA
The output force and time curves of different CSIA samples were shown in Fig. 1(a), from which it could be concluded that from S0 to S4, with the increase of the doping ratio of Nacl, the maximum output force of the CSIA sample S4 reached 2.939 mN, which was 3.4 times higher than that of the control group S0. With the doping ratio continuously increased, the output force decreased to 0.3020 mN for S5 sample, and it reached 54.72% of S0. This showed at an appropriate amount Nacl doping, it had a certain optimization of the network structure of the actuate membranes of CSIA, this could improve the ion transfer rate inside the actuate membranes, thereby the output force of the CSIA was improved, but an excessive doping would change the arrangement frame of the internal structure of the actuate of CSIA, it weakened its performance, leading to serious deformation bubbling and energy loss in the sample during the electrical stimulation response.
The relationship between the maximum output force of the sample CSIA and the porosity of the actuate membranes were shown in Fig. 1(b), the trend of the two sets of data were the similar, with the increase of Nacl doping ratios, the change trend of porosity and output force increased first, and the porosity of actuate membranes CSIA of Nacl-doped reached the maximum at S4, and the maximum attained 12.98%, The lowest of porosity decreased at S5. This showed that Nacl had a certain optimization of the internal three-dimensional network structure of CS, which could improve the ion transfer rate inside the actuate membranes of CSIA, but over Nacl cross-linking doping would lead to beyond ion blockage inside the actuate membranes, the water content of the actuate membranes would decrease, and the CSIA would lose water and harden, resulting in the greater internal stress during deflection, thereby it weakened the output force. The performance parameters of CSIA were detailed in Table S2.
Researchers[29] showed that the deflection mechanism of the ion actuator aceration mechanism of the cellulose backbone was that under the action of electric field, the charge was injected into the cathode and the anode to form an electric double layer. The positively charged cation –NH3+ was bound by the polymer CS backbone and was fixed with the action of Van der Waals force. The anion –CH3COO− moved towards the anode side of the electrode, and accumulates with increasing concentration over time, while the cation moved in the direction of the cathode. Based on above, the cathodic deflection of the actuator on a weakly acidic solution biogel was used, and this cathodic deflection phenomenon was mainly the result of internal ion movement.
As shown in Fig. 1(c), the CS molecule contained a large amount –NH2, in the aqueous acetic acid solution, the backbone chain hydrolysis of CS, many free amino groups on the internal ions bind H+ in the solution, so that chitosan became –NH3+ polyelectrolyte, while the remaining anions were in a free state to dissolve –CH3COO− of CS. As shown in Fig. 1(d), in the CSIA actuate membranes after Nacl doping, Na+ ions were concentrated near the cathode electrode membrane, because the ion radius of Na+ ions (0.97Å) was less than –CH3COO− ion radius (4.50 Å), so when the concentration on both sides accumulated to a certain amount, the ion concentration difference on both sides was inside the actuate membranes under the action of Van der Waals force to make the surface of the electrode showing stress and bending strain. Since the ionic radius of the anion was significantly larger than the ionic radius of the cation, the volume difference of the actuate membranes was generated, so that actuator exhibited cathodic deflection. When voltage was applied across the electrode, ion migration changed from the previous disordered state to ordered. The ion migration rate enhanced. Then, the ion concentration gradient was quickly established, which correspondingly reduced the resistance of the actuator membrane and enhanced the internal ion concentration and mechanical properties of the ion actuator sample.
3.2 Effect of Nacl on the electrochemical performance of CSIA
The electrochemical performance of CSIA with different doping ratios was tested by cyclic voltammetry, and the cyclic voltammetry characteristic curves at different scanning speeds were shown in Fig. 2(a-c), taking the specific capacitance at 50 mV s− 1 scanning speed as an example, with the increase of the doping rate of Nacl, the specific capacitance of the actuate membranes firstly increased to S4 and then decreased to S5. Specifically, the specific capacitance of CS was up to 0.07719 F g− 1 in S4, which was 1.58 times higher than that of 0.0299 F g− 1 of the capacitance of CSIA S0. The specific capacitance value indicated the efficiency of ion migration in the sample to a certain extent, which might be due to the over crosslinking of the CSIA of the Nacl doped to interrupt the channel of ion migration in the actuate membranes, making its internal structure dense and uniform, thereby affecting the ion migration rate. In addition, the specific capacitance trend of the actuate membranes under different doping ratios and different scanning speeds were shown in Fig. 2(d, e). The specific capacitance of the actuate membranes gradually decreased as the scanning rate increased, which indicated that the scanning speed increase rate was faster than the area increases ratios of the CV curve. Finally, the relationship between the resistance of the actuate membrane and the specific capacitance was shown in Fig. 2(f). The two generally showed an inverse ratio, in the experimental group of S4. The specific capacitance reached the maximum, the resistance reached the minimum, which corresponded to the output force of S4, reflecting that the smaller the resistance, the larger the specific capacitance, the better the mechanical properties of the corresponding ion actuator.
The relationship between the real resistance and virtual reactance of the CSIA actuate membranes were shown in Fig. 3(a, b), and it could be seen that there was a good linear relationship between them. The line obtained by linear fitting intersects the x-axis, and the abscissa value of the intersection point was the resistance value of the actuate membrane of CSIA[30]. The resistance of the actuate membranes of CSIA were shown in Fig. 3(c). The resistance of the CSIA sample \({R}_{s}\) could reflect the conductivity of the sample to a certain extent, taking 0.1-100000 Hz as an example, the resistance of the CSIA actuate membranes showed a trend of first decreasing and then increasing, in which the resistance of the actuate membrane at S4 was 13.48 Ω, which was 4.937% lower than that of the control group of S0. This showed that the CSIA sample achieved a better conductive effect at S4 and appropriate Nacl cross-linking doping could improve the electrochemical performance of the CSIA, while excessive doping would intensify and change the molecular structure arrangement inside the actuate membrane of CSIA.
This causes the ion channels to become clogged and crowded, increasing the resistance, and decreasing the electrochemical performance of CSIA.
3.3 Effect of Nacl on the surface morphology and functional groups of CSIA
3.3.1 Electron microscopy scan of CSIA
The micromorphology of the substrate surface and the side section under doped samples of CSIA S0-S5 were shown in Fig. 4. It could be seen from Fig. 4(a-f) that the surface of the CSIA actuate membranes in the control group were smooth, and with the increase of Nacl doping ratio, the particle size and roughness of the surface of the actuate membranes began to gradually increase. The particle size and roughness of CSIA increased significantly at S5. In addition, the interface change between the electrode membranes and the actuate membranes of the CSIA doped with Nacl was shown in Fig. 4(g-i). After observation and comparison, it was found that the undoped CSIA was in smooth contact, while the interface of the CSIA doped with Nacl had an obvious three-dimensional physical cross-network structure. This showed that the doping of Nacl had obvious changes to the internal structure of CSIA, which might be helpful to the performance of CSIA, but excessive doping would also be counterproductive.
3.3.2 Fourier transform infrared spectroscopy of CSIA
The FTIR spectra of CSIA sample S0-S5 was shown in Fig. 5. At 3376.79 cm− 1 and 2929.28 cm− 1, they matched to the telescopic vibration peaks of − OH and − NH2, respectively. The flexural vibration peaks was caused by − CH2 and − CH3 group near 1566.79 cm− 1 and 1411.96 cm− 1.A tensile vibration peak was caused by − CH2 − O−CH2 group narrowing 1045.12 cm− 1 and bending vibration of − CH2 − O−CH2 group neared 854.10 cm− 1. From this group of functional groups, it could be preliminarily inferred that it was a functional group in the structure of CSIA, and the peaks of S1-S5 in the experimental group were basically the same as those in the control group, indicating that the CSIA of Nacl-doped had no significant effect on its functional groups.