3.1. Characteristics of Porous PVDF Fibrous Membrane
To evaluate the effect of PVP content on the performance of porous PVDF fibrous membranes, various analyses including microstructure morphology, porosity, mechanical strength, and FTIR tests were conducted.
Figure 2 illustrates the intuitionistic effect of PVP content on the microstructure of porous PVDF.
Figure 2a exhibits the scanning electron microscopy (SEM) microstructure of PVDF fibrous membranes. The diameter of the monoradicular PVDF fiber with orientation was about 4 μm.
Figure 2b shows the microstructure of PVDF with PVP. The addition of PVP maintained the original diameter of monoradicular PVDF fiber. But, the surface of the PVDF-PVP fibrous membrane was coarser than that of PVDF. The removal of PVP from the PVDF fibrous membrane led to the uniform porous structure on the surface.
Figure 2c demonstrated that the porosity of the porous PVDF fibrous membrane increased gradually with the increase in PVP mass fraction. The porosity of the membrane is 73.9% when the PVP content is 0 wt.%. However, with the increase in PVP content from 1 wt.%, 5 wt.%, 10 wt.%, 15 wt.% to 20 wt.%, the porosity increased to 77.1%, 78.2%, 79.4%, 81.2%, and 86.3%, respectively, as shown in
Figure 2d. Notably, the significant increase in porosity occurred in the range from 15 wt.% to 20 wt.%. Combined with the SEM microstructure analysis, PVP content controlled the porosity of the porous PVDF fibrous membranes.
Figure 3a displays the stress and strain values of the porous PVDF fibrous membrane under various porosity conditions. The maximum stress and strain values of the PVDF fibrous membrane were 1.69 MPa and 17.83%, respectively. With the increase in PVP contents, the stress of the porous PVDF fibrous membrane increased first and then decreased. When the PVP content was 5 wt.%, the porous PVDF reached the peak value of 0.93 MPa and then decreased to the minimum value of 0.14 MPa at 20 wt.%. The strain initially shows a gradual increase, which reached the maximum value of 13.28% at 15 wt.% and then decreased to the minimum value of 13.19% at 20 wt.%. Based on the stress–strain curve of the porous PVDF fibrous membrane, although the PVDF fibrous membrane endured the highest stress without PVP, it exhibited a lower strain. With the increase in PVP content, the porous PVDF fibrous membrane demonstrated a better strain value within the range from 1 wt.% to 10 wt.%. When the PVP content exceeded to 15 wt.%, the porous PVDF fibrous membrane was prone to fracture. The porous structure on the fiber surface was discontinuous micropores with a low PVP content. The micropores were interconnected on the base of high PVP content, leading to strength reduction.
Figure 3b shows the residual strain of the porous PVDF which owned excellent stress and strain performance. The experiment manifested that the porous PVDF fibrous membrane with a PVP content of 5 wt.% owned the highest mechanical strength and elasticity.
Figure 3c,d display the FTIR analysis of PVDF fibrous membrane and porous PVDF fibrous membrane with PVP. The results showed that the addition of PVP introduced new functional groups in the porous PVDF fibrous membrane, which can be found by the emergence of a characteristic peak of -C-N- at 1272.72 cm
−1 and a characteristic peak of -C=O within the range of 1660–1680 cm
−1. Compared with the -C-H stretching vibration peaks at 2900–3000 cm
−1, the higher PVP absorption peaks at 3000 and 3500 cm
−1 confirmed that the hydrophilic characteristics of the PVDF fibrous membrane were altered by the addition of PVP, which built an absorption base of silver ions. The addition of PVP maintained the original functional groups of PVDF and provided function base of porous structure for the preparation of conductive PVDF fibrous membrane. Combined with mechanical strength, the PVP content of 5 wt.% was selected as the optimal content of the preparation of porous PVDF fibrous membrane.
3.2. Characteristics of Conductive Porous PVDF
Multiple experiments including microscopic morphology, differential thermal analysis, conductivity, and FTIR analysis were carried out to investigate the effect of concentration variation in silver nitrate on the properties of AgNPs-PVDF conductive fibrous membranes and disclosed the optimal preparation parameters of the reduction reaction of silver particles.
Figure 4a,b show the microstructure of PVDF fibrous membranes with various concentrations of silver nitrate solution after reduction reaction. Silver particles of small size and amount are distributed sparsely on surfaces of PVDF fibrous membrane. When the concentration of silver nitrate solution increased to 1.2 mol/L, the amount of silver particles with a relatively small size was increased.
Figure 4c,d show the microstructure of porous PVDF fibrous membranes with various concentrations of silver nitrate solution after the reduction reaction. A large amount of silver particles with a small size were distributed uniformly on surfaces of the AgNPs-PVDF fibrous membrane. When the concentration of silver nitrate solution increased to 1.2 mol/L, a large amount of silver particles of a big size existed on surfaces of the AgNPs-PVDF fibrous membrane. The higher the concentration of the silver nitrate solution was, the denser and higher the amount of silver particles of a big size existed. Combined with the energy spectrum in
Figure 4e and XRD curves in
Figure 4f, the particles on PVDF surfaces and AgNPs-PVDF surfaces were a silver elemental substance.
Based on the microstructure and phase component analysis of silver particles on the AgNPs-PVDF fibrous membrane, the method of reduction reaction of silver particles was effective. Compared with PVDF fibrous membrane, the porous structure owned a large amount of silver particles with a bigger size, which proved the effectiveness of the preparation of porous structures. The large amount of dense silver elemental substance bonded tightly with the porous PVDF fibrous membrane and provided high conductivity and durability for the application of the AgNPs-PVDF fibrous membrane.
In order to verify whether the reduction reaction of silver particles affected the functional groups of the AgNPs-PVDF fibrous membrane or not, FTIR analysis of PVDF and conductive PVDF fibrous membrane, and PVDF with PVP and the AgNPs-PVDF fibrous membrane were conducted, as shown in
Figure 5. The PVDF and porous PVDF fibrous membranes owned -C=O characteristic peaks in the range of 1660–1680 cm
−1 and -C-N- characteristic peaks at 1272 cm
−1. After the reduction reaction, -C=O and -C-N- characteristic peaks were also existed in FTIR curves. Based on FTIR results, it can be found that reduction reaction of silver particles only realized conductivity of the AgNPs-PVDF fibrous membrane. There were no new functional groups existed in the AgNPs-PVDF fibrous membrane. The reduction reaction of silver particles maintained the original material characteristics of porous PVDF and realized conductive base.
Effects of silver nitrate concentration on the adsorption capacity and stability of reduced silver nanoparticles was investigated by the differential thermal analysis of PVDF and AgNPs-PVDF conductive fibrous membranes. Compared with
Figure 6a,b, the residual amount of AgNPs-PVDF (30.04%) after 800 °C heat treatment was higher than that of PVDF (25.44%) conductive fibrous membranes. Therefore, the porous structure of porous PVDF effectively absorbed higher amount of silver ions, which proved the feasibility of the porous structure.
Figure 6c displays the conductivity of PVDF and AgNPs-PVDF conductive fibrous membranes after reduced reactions with different concentrations of silver nitrate, which exhibited the positive correlation between the concentration of silver nitrate and the conductivity of the fibrous membrane. In the concentrations of 0.2–0.4 mol/L, the conductivity of the PVDF and AgNPs-PVDF fibrous membrane were approximately zero, exhibiting a high resistance and insulating behavior. In the range of 0.8–1.2 mol/L, the conductivity of the AgNPs-PVDF fibrous membrane increased rapidly, reaching 2272 S/m at 1.2 mol/L. In the range of 1.2–1.4 mol/L, the conductivity of the AgNPs-PVDF fibrous membrane increased gradually and attained a maximum conductivity of 2500 S/m. The conductive PVDF fibrous membrane still maintained a low conductivity in the range of 0–1.4 mol/L. Considering the effects of Moore’s law and the marginal effect on experiments, 1.2 mol/L was selected as the optimal concentration of silver nitrate for the reduction reaction of silver particles. Based on the conductivity comparation analysis of the PVDF and AgNPs-PVDF fibrous membrane, the method of conductive PVDF fibrous membrane was accurate, which maintained the original material characteristics of PVDF and combined high conductivity.
Combined with
Figure 2,
Figure 3,
Figure 4,
Figure 5 and
Figure 6, the construction of the porous structure with excellent absorption and mechanical strength and the preparation method of conductive AgNPs-PVDF fibrous membranes with excellent conductivity, mechanical strength, and bonding strength between silver particles and porous PVDF matrix are effective and feasible. Based on excellent conductivity and mechanical properties, the AgNPs-PVDF fibrous membrane owns the advantages of low resistance and strain-sensing properties. Therefore, the practical conductivity and sensing properties of the AgNPs-PVDF fibrous membrane were investigated to extend the application fields of electrospun conductive fibrous membrane.
3.3. Characteristics of Strain Sensing Property
The conductive AgNPs-PVDF fibrous membrane was connected to the LED circuit, which operated at a rated voltage of 2.0 V. As depicted in
Figure 7a, the LED light emitted a satisfactory level of illumination. When the AgNPs-PVDF fibrous membrane was subjected to a 0.5 cm displacement (15% strain), the brightness of the LED decreased, as shown in
Figure 7b. Compared with
Figure 7a,b, the PVDF conductive fibrous membrane can also light the LED circuit with a rated voltage of 2.0 V in
Figure 7c. But, the LED circuit was extinguished with tensile strain of 15%, as shown in
Figure 7d. Therefore, besides excellent conductivity, the prepared AgNPs-PVDF fibrous membrane owned excellent strain conductivity, which was not the characteristic of the PVDF conductive fibrous membrane.
Δ
R/
R0 curves of the strain sensitivity of the AgNPs-PVDF conductive fibrous membrane are presented in
Figure 7e. Prior to reaching the critical strain of 25%, the strain sensitivity of the conductive fibrous membrane obtained via 1.2 mol/L AgNO
3 solution was 24.3. Based on the fitted curve of ΔR/R
0 variation, the prepared AgNPs-PVDF conductive fibrous membrane owned excellent linearity and sensitivity. Before the strain of 20%, the Δ
R/
R0 variation in PVDF conductive fibrous membrane exhibited low sensitivity and linearity in
Figure 7f, which cannot reflect the real strain variation accurately. The sensing ability indicated that the disconnection and reconstruction of the conductive network was a dynamic process under strain load, manifesting as resistance fluctuations in the macroscopic realm. Consequently, the variation in the Δ
R/
R0 values can be considered the primary indicator in the strain-sensing test process. During the stretching of the conductive fibrous membrane, changes occurred in its length and width. As the stretching was performed along the axial direction of the conductive fibers, the length of the fibrous membrane increased while the width simultaneously decreased. In the strain range of 0–3%, the membrane width rapidly decreased due to stretching, resulting in a reduced gap between the conductive fibers. This reduction enabled the formation of conductive pathways through contact between silver particles. The pathways were formed more quickly than the disconnection of silver nanoparticles along the fiber axis. Consequently, the total resistance of the conductive fibrous membrane decreased. Within the strain range of 3–23%, the conductive fibrous membrane continued to stretch and lengthen. However, the rate at which conductive pathways of the conductive fibers decreased and became slower than that at which silver nanoparticles disconnect along the fiber axis. As a result, the total resistance of the fibrous membrane increased.
In order to verify the sensing properties of AgNPs-PVDF conductive fibrous membranes with different strain values, the cyclic stretch experiments were conducted. As shown in
Figure 8a, Δ
R/
R0 values increased gradually with the increase in strain values from 10% to 15%. When the strain values reached 20%, the PVDF conductive fibrous membranes were stretch ineffective before a cyclic stretch of 20 times. Moreover, the Δ
R/
R0 values of PVDF conductive fibrous membranes were not steady, which existed as an obvious fluctuation phenomenon. Compared with PVDF conductive fibrous membranes, AgNPs-PVDF conductive fibrous membranes exhibited steady Δ
R/
R0 variation in specific cyclic strain processes, as shown in
Figure 8b. Moreover, with the increase in strain, Δ
R/
R0 values of AgNPs-PVDF conductive fibrous membranes increased correspondingly. Based on
Figure 4,
Figure 6,
Figure 7 and
Figure 8, it can be found that the AgNPs-PVDF conductive fibrous membrane owned an excellent size and amount of silver particles, high conductivity, and continuous strain-sensing property, which can be used to detect practical strain signals.
Figure 9a,b present the test results of Δ
R/
R0 following 20 cycles of low-speed and high-speed stretching of AgNPs-PVDF conductive fibrous membranes with the strain of 25% and loading rate ranging from 20 mm/min to 1000 mm/min. It can be observed that Δ
R/
R0 exhibited minimal fluctuations, steady peak values, and stable signal variation at each stretching speeds. Notably,
Figure 9c demonstrated that the AgNPs-PVDF conductive fibrous membrane exhibited the excellent response time of 63 milliseconds at a stretching speed of 1000 mm/min.
Figure 9d illustrated the Δ
R/
R0 performance of the AgNPs-PVDF conductive fibrous membrane with a loading rate of 200 mm/min and 20% strain for 4000 cycles. Notably, the AgNPs-PVDF conductive fibrous membrane demonstrated remarkable durability throughout the test. The Δ
R/
R0 values increased with the increase in cycle times, which displayed two distinct signals characterized by an “M” shape. This shape was attributed to the mechanical hysteresis of the AgNPs-PVDF conductive fibrous membrane and the reorganization of the silver particles’ conductive network. The loading rate of 200 mm/min realized a balance between excessive speed and sluggishness, allowing the maximum elongation. AgNPs-PVDF conductive fibrous membrane exhibited a certain degree of rebound. With the decrease in Δ
R/
R0, the stretching machine continued the movement without returning to the original resistance. When the signal reached its peak and the stretching machine returned to its initial position, the signal also returned to its starting point. The prepared AgNPs-PVDF conductive fibrous membrane owned steady sensitivity, linearity, and durability, which built the function base for practical sensing applications.
In order to verify the practical sensing properties, AgNPs-PVDF conductive fibrous membranes are placed on throat, elbow, wrist, finger, and knee, to detect corresponding strain signals of the human body with different variation degrees, as shown in
Figure 10a. The AgNPs-PVDF conductive fibrous membrane is integrated into the throat with adhesive tape to investigate small-scale human motion. The repeatable Δ
R/
R0 signals were tested via the sensor when the volunteer spoke the words “Hello”. Obviously, the signals can be easily distinguished steadily during the repeatable process, as shown in
Figure 10b.
Figure 10c exhibits that the AgNPs-PVDF conductive fibrous membrane was used to detect an elbow bending process from 0° to 45° and 90°. The effective monitoring suggests that the AgNPs-PVDF conductive fibrous membrane strain sensor could be used to identify bending degree information by observing Δ
R/
R0 signals. Besides the throat and elbow, the motion of the wrist can also be detected. As shown in
Figure 10d, Δ
R/
R0 signals measured the wrist bending process from 0° to 45° and 90°. With the increase in bending degree, Δ
R/
R0 signals increased correspondingly, indicating the excellent sensing response rate. Fingers are the parts with a high freedom of movement in the human body.
Figure 10e shows the AgNPs-PVDF conductive fibrous membrane sensor which is also used to detect the bending degree via mounting on finger. When the finger bent from 0° to 45° and 90°, three diacritical Δ
R/
R0 curve parts are corresponding to the bending degrees of the finger. To investigate the viability as a strain sensor for detecting high-scale human motion, the strain sensors are integrated into the knee. The strain sensor effectively detected the bending process of the knee.
Figure 10 demonstrates the high sensitivity of the conductive fiber in detecting motion signals, facilitating the accurate detection of diverse movements of finger, wrist, elbow, knee, and throat vibrations. Consequently, the AgNPs-PVDF conductive fibrous membrane exhibits exceptional sensing capabilities. The practical sensing application in
Figure 10 proves the excellent sensing properties of AgNPs-PVDF conductive fibrous membranes. Moreover, the preparation of AgNPs-PVDF conductive fibrous membranes on the basis of the preparation of the porous PVDF fibrous membrane and the reduction reaction of silver particles was also verified feasibly and effectively. The investigation of the conductive PVDF fibrous membrane with high conductivity via electrostatic spinning builds and extends the material and functional base for the practical application of functional fibers in the field of man–machine interaction.