In addition to their established biocompatibility upon degradation, excellent sensing performance is also an important consideration for this application. Figure
2(a) shows representative I-V curves of the device under different relative humidity (RH) conditions. We observed increases in current as different humidity sources were moved closer to the humidity sensor. During the experiment, the hysteresis increases with increasing humidity, which may be due to the increase in charge accumulation/depletion [
20]. The increase in current in degradable biocomposite film under humid conditions should be due to the formation of hydrogen bond networks between the water and polysaccharides in the polysaccharide films [
22]. Higher water absorption results in a more proton-conducting hydrogen bonds, which form a three-dimensional network, and protons can move along these chains via Grotthuss-type mechanisms [
20,
23]. The phenomenon of proton conduction is ubiquitous in biomacromolecule-derived materials. For degradable biocomposite film, we propose that the carboxyl group on the chitosan side chain is deprotonated, donating a proton to the surrounding proton wires and forming a protonic conductor with H
+ as the major charge carrier (Figure
2(b)) [
22]. Namely, the proton current in the degradable biocomposite film at 75%RH is threefold higher than that at 65%RH. At 85%RH, more water was adsorbed on the surface of the degradable biocomposite film, forming more hydrogen-bonded proton wires, which increased proton transfer, thus increasing the current [
24]. To rationalize the experimental results and estimate the effects of humidity on the proton density in the channels of the degradable biocomposite film, we simulated changes in the proton charge density in degradable biocomposite film using the finite element method (FEM) (detailed parameters are provided in Materials and Methods). The mechanistic model is based on the Gompertz equation, and when the electronic density is replaced by the proton density (see Materials and Methods), the change in the proton charge density at different humidities was obtained. The thickness of the degradable biocomposite film was 20
μm (Figure S1). The modeling results showed (Figure
2(c)) no obvious changes in the potential distribution at the same humidity due to the homogeneity of the degradable biocomposite film; that is, the electronic field distribution is not affected by humidity. Figures
2(d)–
2(g) show that exposing the flexible device to a humid environment leads to a change in proton density. The proton density increases with increasing humidity (Figure S4). In a high-humidity environment (85%RH), a high number of protons gather in the conductive channels to form a highly conductive region (Figure
2(g)). Similar effects of humidity on current and charge density distributions have been reported for other organic humidity sensors [
20,
25]. Figure
2(h) shows the simulated and experimental current responses of the degradable biocomposite film-based flexible humidity sensor at 55%RH, 65%RH, 75%RH, and 85%RH. The results of the simulations were close to the experimental data at high humidity and show a linear dependence of current on humidity at 55-85%RH, which demonstrated that the degradable biocomposite film-based flexible humidity sensor responds to humidity [
20].