Pavar Sai
Kumar
a,
Vanmathi
S.
a,
Himanshi
Awasthi
a,
Imran
Khan
a,
Ritesh Kumar
Singh
a,
Vimal Kumar
Sharma
b,
Chandrani
Pramanik
*b and
Sanket
Goel
*a
aMEMS, Microfluidics and Nanoelectronics (MMNE) Lab, Department of Electrical and Electronics Engineering, Birla Institute of Technology and Science (BITS) Pilani, Hyderabad Campus, Hyderabad 500078, India. E-mail: sgoel@hyderabad.bits-pilani.ac.in
bGraphene Centre, Tata Steel Limited, Jamshedpur, Jharkhand 831007, India. E-mail: chandrani.pramanik@tatasteel.com
First published on 12th June 2024
The versatile properties of graphene and ancillary materials in various areas have accelerated the development of optimized methods, particularly using natural sources. Herein, natural shellac (biopolymer) (C25H51COOH), with inherent long carbon chains, is leveraged as a potential resource in improving the physiochemical properties of laser-induced reduced graphene oxide (rGO). A versatile 450 nm blue diode laser produced biopolymer-assisted rGO on environmentally friendly flexible paper and cloth samples. The methodology led to the formation of improved rGO with electrical sheet resistances as low as 2.3 Ω Sq.−1 Moreover, thorough characterizations revealed that the average number of rGO layers is as low as 11. The potential of shellac-assisted rGO was validated in four significant applications. First, a disposable 2-electrode enzymatic biofuel cell (EBFC) was developed on biopolymer-assisted paper samples, which led to the generation of a power density of 66.7 μW cm−2. Second, rGO interdigitated electrode (IDE) supercapacitors were patterned over dual shellac varieties of paper and showed a maximum areal capacitance of 31.25 mF cm−2 at a current density of 0.5 mA cm−2. Third, the rGO-patterned electrode system on biopolymer-assisted paper successfully yielded notable conventional ECG signals, specifically P, R, T, and QRS complexes. Moreover, the signal-to-noise ratio (S/N ratio) notably increased to 24%, surpassing the S/N ratio observed using the conventional Ag/AgCl electrode system. Ultimately, printed electronic circuits were demonstrated on cloth samples for wearable applications. The utilization of natural biopolymers to enhance rGO holds significant promise for a wide range of potential applications in the future.
Despite such unique properties of graphene and its progressive synthesis techniques, began the race for its potential findings.7,8 Numerous kinds of graphene-derived materials, including graphene oxide (GO), reduced graphene oxide (rGO), multilayered graphene, graphene composites, and graphene ribbons, have been synthesized for prominent specific applications.9–11 Conventional synthesis methods can be categorized as top-down methods via mechanical exfoliation (utilizing high-speed ball milling, high shear homogenizer, ultrasonication, etc.) and bottom-up synthesis methods (e.g., chemical vapor depositions (CVD), pulse vapor deposition (PVD) and electric arc discharge).12 However, these techniques exhibit certain drawbacks, such as toxic chemical treatments, exposure to high annealing temperatures, tedious post-processing such as drying and solvent recovery, and the release of harsh chemical byproducts. In addition, these techniques constrain affordability and qualitative stabilities, thus lowering scalabilities and posing environmental challenges.13
Alternatively, the current studies focus on synthesizing graphene oxide (GO) by chemical exfoliations of graphite as a graphene derivative with comparatively lower limitations.14 GO has graphene-like structural properties with covalently attached oxygen functional groups (carboxyl, hydroxyl, and carbonyl) as defects. However, GO could not meet the exceptional electrical, optical, and mechanical properties of graphene.15
Reduced graphene oxide (rGO) synthesis replaces the GO with its graphene-like properties, including higher conductivities, lower sheet resistances, and improved thermal properties.16 The standard method for obtaining rGO was through the thermal and chemical reductions of GO. The popular methods include microwave-assisted synthesis, wet-chemical processes, high-temperature thermal treatments, and often multi-step reductions.17 Nevertheless, the traditional processes involve toxic chemical reagents (hydrazine hydrates and dimethylhydrazines) and high annealing temperatures (from ∼1000 to 1200 °C), releasing hazardous gases into the environment.18 The challenge in obtaining high-quality rGO, a potential resource between GO and graphene, has been to explore single-step, non-toxic, and non-tedious production techniques.
Recent work from our group highlights the one-step methodology for obtaining high-quality rGO through laser irradiation on simple filter paper.19,20 One highlight of the work was obtaining rGO without utilizing GO as an intermediate precursor or a carbon source. Instead, rGO was acquired by laser irradiation onto a simple filter paper with controlled parameters.21,22 However, the work was limited by its lower electrical and physicochemical properties due to the insufficient penetration of laser fluence into the substrate, restricted by its thickness. The continued investigations found an attractive, biodegradable, and eco-friendly natural polymer, shellac, as a natural resource to suppress the limitations of our reported process.19
Natural shellac (C25H51COOH), containing longer carbon chains, could be leveraged as a supporting polymeric resource in treating the samples to develop an enhanced rGO material. Moreover, shellac is widely available as a natural resin or biopolymer secreted by the lac bugs on the trees of several countries, including India and Myanmar.23 Such natural polymers can be broadly classified into two types: Shellac and Dewaxed shellac.24
Shellac has already been proven to produce graphene film on various substrates stable for high temperatures.25 However, for the first time, to the best of our knowledge, the biopolymer was used as a supporting source on biodegradable substrates, such as paper and cloth, to obtain rGO material in a single step at room temperature and in a normal atmosphere with enhanced properties. The laser irradiations were optimized onto the treated paper and cloth samples to obtain high-quality rGO material. The obtained material was thoroughly characterized owing to its optical, structural, electrical, and morphological details. Moreover, the potential of biopolymer-assisted rGO was revealed by deploying it into three applications, including recording electrocardiogram (ECG) signals from miniaturized ECG electrodes. Exceptional results were obtained by developing an enzymatic biofuel cell on biopolymer-assisted rGO paper samples and energy harvesting using an interdigitated electrode (IDE) system for supercapacitor studies.
The biopolymer solutions of Dewaxed shellac (DS) and shellac (S) were prepared by varying the ratio of biopolymer to IPA solvent from 1/1 to 1/5 (w (g)/v (mL)), as shown in Fig. 1b. However, it was found that the ratios 1/1 and 1/2 were challenging to coat due to insufficient solvent consistency. Further, the uniform solutions were made possible through continuous hotplate stirring at 65 °C for 2 h. (solution B). The varying ratios (from 1/3 to 1/5 (w (g)/v (mL))) of biopolymer solutions (solution B) were then dip-coated onto the FR-treated samples and allowed to dry at 55 °C for 1 h. (Fig. 1c).
LIrGO/Dewaxed Shellac/FR/Paper | |||||
---|---|---|---|---|---|
Dewaxed shellac/IPA (w/v) | (1/3) | (1/4) | (1/5) | ||
Laser power (%) | Laser power (W) | Laser speed (%) | Avg. sheet resistance (Rs) (Ω Sq.−1) (n = 3) | ||
‘–’ insufficient dosage; ‘×’ higher dosage (i.e., substrate cut, discarded); laser max. Power: 2.8 W; laser max. Speed (300%): 120 mm s−1; LIrGO: laser-induced rGO. | |||||
15 | 0.42 | 100% or 40 mm s−1 | — | — | — |
20 | 0.56 | — | 15.9 | 14.4 | |
25 | 0.7 | 14.1 | 11.2 | 9.9 | |
30 | 0.84 | 11.7 | × | × | |
35 | 0.98 | × | × | × |
LIrGO/Shellac/FR/Paper | |||||
---|---|---|---|---|---|
Shellac/IPA (w/v) | (1/3) | (1/4) | (1/5) | ||
Laser power (%) | Laser power (W) | Laser speed (%) | Avg. sheet resistance (Ω Sq.−1) (n = 3) | ||
‘×’ higher dosage (i.e., substrate cut, discarded); laser max. Power: 2.8 W; laser max. Speed (300%): 120 mm s−1; LIrGO: laser-induced rGO. | |||||
15 | 0.42 | 100% or 40 mm s−1 | 69.8 | 48.7 | 27.8 |
20 | 0.56 | 31.8 | 21.8 | 15.6 | |
25 | 0.7 | 15.3 | 13.2 | × | |
30 | 0.84 | 9.3 | 9.0 | × | |
35 | 0.98 | 7.5 | 7.0 | × |
The experimental results validate the significance of the laser parameters in obtaining the optimized sheet resistance of the developed rGO material. As shown in Tables 1 and 2, the insufficient dosage (represented as ‘–’) resulted in the incomplete formation of the designed pattern. Further, the higher dosage (represented as ‘×’) pierced the substrate (e.g., shown in cf., Fig. S1, ESI†). In the Dewaxed shellac/FR/Paper, the 1/5 ratio of the solution was suitable for obtaining a minimum sheet resistance of 9.9 Ω Sq.−1 (cf., Table 1). Similarly, the Shellac/FR/Paper, 1/4 ratio provided a minimum sheet resistance of 7.0 Ω Sq.−1, as shown in Table 2.
The solution-optimized constituents were utilized in optimizing the laser parameters to obtain possible minimum sheet resistances on cloth substrates. Therefore, the optimizations on cloth substrates leveraged the optimum solution ratios of 1/5 and 1/4 for the Dewaxed shellac/FR/Cloth and Shellac/FR/Cloth, respectively. The plots of sheet resistance variation with the change in laser parameters are shown for rGO/Dewaxed shellac/FR/Cloth and rGO/Shellac/FR/Cloth in Fig. S2 and S3 (ESI†), respectively. Interesting results were obtained for the cloth samples, and the minimum average sheet resistance values of rGO/Dewaxed shellac/FR/Cloth and rGO/Shellac/FR/Cloth were 2.3 Ω Sq.−1 and 3.4 Ω Sq.−1, respectively. However, the observations found the piercing of substrate at higher dosages; therefore, the optimized sheet resistance values of 9.9 Ω Sq.−1 and 8.1 Ω Sq.−1, respectively, were considered for future experiments, as shown in Table 2 and Section S3 and Table S3 (ESI†).
Fig. 3 Field emission scanning electron microscopy images: (a) LIrGO/Dewaxed shellac/FR/Paper (Inset: 5 μm and 100 μm high-resolution images), (b) LIrGO/Shellac/FR/Paper, (c) LIrGO/Dewaxed shellac/FR/Cloth, and (d) LIrGO/Shellac/FR/Cloth (all insets: 100 μm high-resolution images, shown separately in ESI† (Fig. S19)). |
Fig. 3(c) and (d) show the SEM images of the crossing yarns transformed into biopolymer-assisted rGO yarns. In the assisted Dewaxed shellac and Shellac cotton cloths, the average thicknesses of the rGO yarns were 13.1 μm and 11.2 μm (±1 μm), respectively. Further, the cross-sectional information was provided for the developed laser-irradiated rGO on the biopolymer-assisted cloth sample in Fig. S8 (ESI†). Similar to the paper substrates, the LIrGO/Dewaxed shellac/FR/Cloth showed porous open yarn at 5 μm resolution (i.e., due to the minimal presence of wax content (0.2% v/v)), as shown in Fig. 3(c) inset. However, the LIrGO/Shellac/FR/Cloth showed thick polymer adsorption (i.e., due to the presence of its wax content (3% to 6% (v/v))) over the developed rGO yarns, as shown in Fig. 3(d) inset. Moreover, the untreated/bare paper and cloth FESEM images are presented in (Fig. S20, ESI†).
Subsequently, transmission electron microscopy (TEM) was performed to observe the atomic arrangements and morphological details. Fig. 4(a) and (b) show the distribution of rGO flakes developed on the biopolymer-assisted paper samples (I) – 500 nm; further, the higher resolution of material was shown in the inset image of (II) – 200 nm. In addition, the atomic orientation and arrangements can be observed in the inset image of (III) – 20 nm. At this higher resolution in the paper samples (both dewaxed shellac and shellac cases), it was observed that the atomic arrangement was short-range ordered with an increased number of grain boundaries with overlapping atomic distributions. In addition, the TEM observations of rGO developed on biopolymer-assisted cloth samples showed the rGO clusters in the Dewaxed shellac/FR/Cloth sample (Fig. 4c(I) – 500 nm) instead of flakes as in paper samples. However, distorted rectangular stands of rGO were found in the Shellac/FR/Cloth sample (Fig. 4d(I) – 500 nm). In addition, comparatively significant uniformity of atomic arrangements (i.e., relatively long-range ordered atomic arrangement) was observed in cloth samples than in paper (inset images (Fig. 4c(III) and d(III) – 20 nm)). The key finding derived from the transmission electron microscopy (TEM) study was that the transparency of reduced graphene oxide (rGO) on paper samples was more significant compared to that on cloth samples. This difference in transparency was due to the lesser number of rGO layers, as indicated by the data presented in Section S4 (ESI†) (Table S4).
Similar characteristics of rGO were observed in the laser-induced biopolymer-assisted cloth samples. Fig. S15(a) and (c) (ESI†) show the characteristic peaks of carbon (C) (285.1 eV), oxygen (O) (532.08 eV), and sodium (Na) (1072.3 eV). Further, the elemental atomic weight percentages were C: 89.9%, O: 9.39%, (C/O): 9.6, and Na: 0.71 for LIrGO/Dewaxed shellac/FR/Cloth. Moreover, the LIrGO/Shellac/FR/Cloth shows the atomic percentages as C: 88.9%, O: 10.6, (C/O: 8.4) and Na: 0.49. It was observed that the biopolymer-assisted cloth samples showed improved C/O ratios compared to the biopolymer-assisted paper substrates. In addition, the narrow scan survey of the C 1s spectra indicates the chemical bondings of rGO at 284.8 eV, 286.1 eV (±0.1 eV), and 289.1 eV (±0.1 eV), representing the CC, C–O, and O–CO bonds, respectively, as shown in Fig. S15(b) and (d) (ESI†).
Fig. 5 Electronic transitional characterization via UV-vis spectroscopy: (a) rGO developed on biopolymer-assisted paper samples and (b) rGO developed on biopolymer-assisted cloth samples. |
Fig. 6 Raman analysis in identifying structural disorders, (a) analysis of rGO developed on biopolymer-assisted paper samples and (b) analysis of rGO developed on biopolymer-assisted cloth samples. |
In addition, the Raman spectra of the rGO developed on biopolymer-assisted cloth samples are shown in Fig. 6b. The observations found a similar characteristic G band at 1587.6 cm−1 and the disordered D bands at 1346.1 cm−1 and 1351.3 cm−1 for rGO/Dewaxed shellac/FR/Cloth and rGO/Shellac/FR/Cloth samples, respectively. The qualitative analysis found that (ID/IG) = 0.67 for the rGO/Dewaxed shellac/FR/Cloth and (ID/IG) = 0.32 and (I2D/IG) = 0.46 for the rGO/Shellac/FR/Cloth. Moreover, the obtained rGO material followed the literature entirely.39 Further, the specific surface area (SSA) and pore size measurements with complete calculations are presented in Section S5 (ESI†).
Linear sweep voltammetry analysis was carried out to optimize the concentrations of glucose (10 mM to 60 mM). It was observed that the maximum current density (CD) (0.459 mA cm−2) was obtained at 40 mM, as shown in Fig. 7a. The performance of the anodic and cathodic electrodes was analyzed via cyclic voltammetry (CV) studies. The setup leveraged a standard Ag/AgCl electrode as a reference and a platinum electrode as a counter. Further, the experimental CV parameters include 50 mV s−1 scan speed, a −1 V to 1 V voltage range, 5 mL of cell volume, and 0.1 M PBS (pH 7). Fig. 7b shows the negligible anodic performance without glucose (40 mM). However, its presence promotes the efficiency of an immobilized enzyme (GOx), resulting in an oxidation peak at a CD of 0.25 mA cm−2 and 0.9 V. Similarly, the cathodic performance showed an improved CD of 5.2 mA cm−2 at 0.4 V in the presence of oxygen (O2) purge than its absence, as shown in Fig. 7c.
Further, the chronoamperometry (CA) was carried out to obtain the polarization performance analysis on the developed 2-electrode system of biopolymer-assisted rGO, as shown in (Fig. S9A, ESI†). Fig. 7d illustrates the maximum power density (PD) of 66.7 μW cm−2 at a CD of 634 μA cm−2 with a steady open circuit voltage of 394 mV. The polarization analysis indicates the possibility of superior electron kinetics and redox reactions through the developed rGO material and its active sites for enzyme immobilization.21
Moreover, a comparative CV curve is shown in Fig. 8(c) at a constant 50 mV s−1 scan rate, which indicates the produced capacitance by the sorption of ions from the electrolyte, leading to the formation of a double layer (EDL) over the electrode surface.42 The areal capacitance trends as a function of the scan rates (5 mV s−1 to 200 mV s−1) are shown in Fig. 8(d). The rGO SC developed on Dewaxed shellac paper substrate showed an areal capacitance of 68.8 mF cm−2 to 0.3 mF cm−2, and the rGO SC developed on Shellac paper substrate showed a higher areal capacitance of 91 mF cm−2 to 0.7 mF cm−2. It was observed that the increase in scan rate decreased the areal capacitance, following the equation below:
Further, the logarithmic decay in the areal capacitance was observed due to the diffusion limitations at higher scan rates, decreasing the EDL capacitances. Moreover, the EDL capacitance is in direct proportion to the specific capacitance. The decay may also be attributed to the increase in resistance within the electrode material's active surface or at the electrolytes and electrode surface interface.
The developed patterns of rGO on both paper samples were further characterized using the galvanostatic charge–discharge (GCD) analysis. The test conditions leveraged the varying current density inputs, including 0.1, 0.2, 0.25, 0.5 mA cm−2 and 0.25, 0.5, 1, 1.5 mA cm−2, on rGO/Dewaxed shellac/FR/Paper and rGO/Shellac/FR/Paper samples, as shown in Fig. S18(a) and (b) (ESI†). Moreover, the nearly obtained triangular shapes indicate the energy storage dynamics of the rGO on both paper samples.43 The comparative areal capacitance at a current density (CD) of 0.5 mA cm−2 showed a maximum capacitance of 31.25 mF cm−2 with the rGO/Shellac/FR/Paper. In contrast, the rGO/Dewaxed shellac/FR/Paper showed 16.87 mF cm−2 capacitance, as shown in Fig. S18(c) (ESI†). Further, the electrochemical impedance spectroscopy (EIS) study was performed at a frequency ranging from 10 kHz to 10 MHz, and the obtained Nyquist plot, as shown in Fig. S18(d) (ESI†), was analyzed to obtain the equivalent series resistance (ESR). An ESR of 118.6 Ω cm2 was obtained by calculations for the rGO/Shellac/FR/Paper, while a higher ESR of 224.5 Ω cm2 was derived for the rGO/Dewaxed shellac/FR/Paper. Moreover, a lower ESR indicates higher ion diffusion electrochemical behaviors with increased electrode conductivities and vice versa.44 In general, the utilization of biopolymer-assisted reduced graphene oxide (rGO) on paper samples demonstrates considerable promise in the field of supercapacitor applications.
The biopolymer-assisted rGO developed on shellac-assisted paper samples was used to develop the dry ECG electrodes by 1 v/v%, PEDOT: PSS/Dimethyl sulfoxide (DMSO) modifications, as shown in (Fig. S11, ESI† (inset)), and the Ag/AgCl conventional standard wet electrodes were used for comparison. Moreover, it has been shown that applying conductive gel to record signals through ordinary electrodes can lead to skin irritation and a gradual decrease in signal quality.47 To amplify the obtained signals, the Bioamp exg pill tool was connected to Arduino Uno (ATMEGA328P, processing microcontroller), and MATLAB programs (wavelet denoising and symlet 4 denoising) were leveraged to obtain high noise-to-ratio informative peaks, as shown in Fig. 9.
Fig. 9(a) and (b) show the unfiltered ECG signals derived from the developed dry electrode created on paper and the standard Ag/AgCl electrodes, in which the interpretation of data was difficult. Nevertheless, the filtered data show the characteristic P, R, and T peaks, indicating the electrical impulse response from the heart, as shown in Fig. 9(c) and (d). Moreover, the depolarization of the heart can be observed through the QRS complex peaks, as shown in Fig. 9(c) and (d).
Further, the impedance analysis establishes a comparative analysis between the standard and the developed system, as shown in (Fig. S11, ESI†). The frequency range was systematically adjusted from 0.1 Hz to 1000 Hz to measure the skin impedance. The measurements at a frequency of 10 Hz indicated a significantly higher impedance value of 87.85 kΩ, in contrast to the impedance of the standard electrode, which measured 49.12 kΩ. The disparities in electrode characteristics, namely between dry and wet gel electrodes, were the primary factors contributing to the notable variation in impedance. However, the as-developed rGO electrodes (S/N: 21.5 dB) significantly improved the signal-to-noise ratio by 24% compared to the standard electrodes (S/N: 17.32 dB).
Fig. 10 Printed electronic circuits on developed rGO patterns over dewaxed shellac and shellac cloth substrates. |
As shown in Fig. 10, when the battery was disconnected, the LEDs were off in both cases, while the LEDs were turned on by a battery connection. Further, this validates that the obtained patterns are highly conductive to transfer electrons and can be used in the near future for disposable, biocompatible wearable electronics.
Moreover, the efficacy of the generated reduced graphene oxide (rGO) was verified in four notable applications. This study involved the creation of a disposable enzymatic biofuel cell (EBFC) that can generate a power density of 66.7 μW cm−2 at a current density (CD) of 634 μA cm−2 while maintaining a consistent open circuit voltage of 394 mV. Furthermore, the interdigitated electrode (IDE) system, created to study supercapacitors (SCs) using rGO/Dewaxed shellac/FR/Paper and rGO/Shellac/FR/Paper, exhibited aerial capacitance values of 16.87 mF cm−2 and 31.25 mF cm−2, respectively, when subjected to a current density (CD) of 0.5 mA cm−2. Electrocardiogram (ECG) data were obtained using a dry rGO/Shellac/FR/Paper electrode system, which exhibited a superior signal-to-noise ratio (S/N) improvement of 24% compared to the conventional Ag/AgCl electrodes. Finally, the cloth-based printed electronics showcase the possibility of future endeavors in developing printed textiles for smart lifestyles. The proposed methodology for utilizing natural shellac to enhance the performance of reduced graphene oxide (rGO) has enormous potential for a wide range of flexible wearables, and edible electronic applications in the future.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ma00151f |
This journal is © The Royal Society of Chemistry 2024 |