Subin Kaladi
Chondath
a,
Abhishek Pradeep Kumar
Sreekala
a,
Chalikkara
Farzeena
b,
Subramanyan Namboodiri
Varanakkottu
c and
Mini Mol
Menamparambath
*a
aDepartment of Chemistry, National Institute of Technology Calicut, Calicut-673601, Kerala, India. E-mail: minimol@nitc.ac.in
bSchool of Materials Science and Engineering, National Institute of Technology Calicut, Calicut-673601, Kerala, India
cDepartment of Physics, National Institute of Technology Calicut, Calicut-673601, Kerala, India
First published on 28th July 2022
An emerging aspect of research is designing and developing fully tunable metamaterials for various applications with fluid interfaces. Liquid/liquid interface-assisted methods represent an efficient and facile route for synthesizing two-dimensional (2-D) thin films of potential materials. The underlying mechanism behind thin film formation at the liquid/liquid interface involves the preferential adsorption of nano-sized particles at the interface to minimize high interfacial tension. Here, a water/chloroform interface-assisted method is employed for the one-pot synthesis of highly crystalline polypyrrole/manganese dioxide (PPy/MnO2) sheets. The temporal evolution in the dynamic interfacial tension (from 32 mN m−1 to 17 mN m−1) observed in pendant drop tensiometry proved the preferential adsorption of MnO2 atttached PPy oligomers at the water/chloroform interface. An ultra-thin sheet-like morphology and uniform distribution of ∼6 nm highly crystalline MnO2 nanoparticles are evidenced by transmission and atomic force microscopy techniques. The predominance of interfacial polymerization in retaining the electrochemical activity of the PPy/MnO2 sheets is elucidated for the electrochemical detection of nicotine. This study opens a new avenue for the realization of ultra-thin sheets of polymer–nanomaterial hybrids, enabling applications ranging from new classes of sensors to optics.
The paramount importance of L/L interface-assisted methods in processing and preparing potential materials is rooted in their ability to synthesize ultra-thin two-dimensional (2-D) films25,26 or reconfigure self-assembly on demand.1,27 The nanostructure tuning to ultra-thin 2-D films at the L/L interface is impelled by the self-organization of reactive molecular species at the interface of two immiscible liquids.24–26 The conventional methods are tedious to synthesize thin films due to the material characteristics (insolubility, dispersibility, transparency, and homogeneity) or stringent deposition conditions.22 The L/L interface-assisted method ensures the facile deposition of thin films of single or multi-component materials that are effortlessly transferred to any substrates (plastic or flexible substrates).22 The L/L interface-assisted synthesis route allows control over the thickness, homogeneity, and transparency of the thin film under ambient temperature and pressure conditions with a simple and economically viable procedure.22
To meet the challenges that lie ahead for targeted applications, thin films of various nanostructures are prepared by the self-assembly of these nanostructures, selectively dispersed in any of the two immiscible solvents.22,28,29 An interfacial film formation technique was employed to fabricate MXene thin films for ultra-compact passive photonic diodes.30 The in situ synthesis of multi-component (nanocomposite) materials is intricate to perform under ambient conditions, while the L/L interface-assisted method proved to be successful. Furthermore, the insolubility, infusibility, and dispersibility of reactive species limit the in situ distribution of nanostructures in a polymer matrix using conventional chemical or electrochemical routes. On the other hand, conductive polymers composited with multidimensional nanomaterials yielded free-standing thin films for several novel applications.31
Here, we investigated the self-assembly of in situ grown PPy/MnO2 at the water/chloroform interface, tuning the polymer composites to ultra-thin 2-D sheets without any hard or sacrificial templates. Experimental observations proved that the high interfacial tension at the water/chloroform interface acts as a driving force for the preferential adsorption of MnO2-bound oligomers. The dynamic interfacial tension of the water/chloroform interface as a function of time evidenced the stabilization of the interface with a persistent decrease in the IFT as the polymerization progressed at the interface. The water/chloroform interface acts as a soft template for the self-assembly of MnO2 attached PPy oligomers, leading to the confinement and tuning of PPy/MnO2 composites to ultra-thin sheets. The transmission electron microscopic images showed the growth and confinement of amorphous network-like structures to ultra-thin PPy/MnO2 sheets during the polymerization. The transition of diffused rings to bright Bragg spots in electron diffraction further confirmed the evolution of amorphous MnO2 agglomerates to highly crystalline MnO2 NPs. MnO2 NPs are widely accepted for electrochemical storage applications, and numerous works have been devoted to synthesizing diverse MnO2 nanostructures for energy applications.32,33 Herein, the uniform encapsulation of MnO2 NPs in PPy/MnO2 sheets was further explored for the electrochemical sensing of nicotine, a significant ingredient in cigarettes.34 The composites of PPy/MnO2 with multi-walled carbon nanotubes (MWCNTs) were used as electrochemical sensors for nicotine detection. The printable nature of the composite inks of PPy/MnO2 with MWCNTs was also tested on screen-printed electrodes and subsequently validated for electrochemical activity in nicotine oxidation.
Further morphological and physico-chemical properties of PPy/MnO2 were characterized using the as-synthesized product after 15 hours (filtered and washed several times with deionized water and ethanol). Field emission scanning electron microscopy (FESEM, FEI-Quanta FEG 200F), HRTEM with energy dispersive spectroscopy (EDS), and elemental mapping (Thermofischer Talos F200 S) were employed to obtain electron microscopy images and the elemental composition. The crystallinity of the PPy/MnO2 powder sample was analyzed using the powder XRD technique (Bruker D8 advance with Cu Kα radiation, scan rate: 0.013 steps per 26 to 32 s). The PPy/MnO2 films confined at the interface were transferred to mica sheets for atomic force microscopy (AFM, Bruker) by simply lifting the substrate in the film direction. The surface chemistry of the PPy/MnO2 samples was analyzed using XPS (PHI 5000 Versa Probe II, ULVAC-PHI Inc., USA) equipped with a micro-focused (200 μm, 15 kV) monochromatic Al-Kα X-ray source (hν = 1486.6 eV). Survey scans were recorded with an X-ray source power of 50 W and a pass energy of 187.85 eV. High-resolution spectra of the major elements were recorded at 46.95 eV pass energy. XPS data were processed using PHI's Multipak software. The binding energy was referenced to the C 1s peak at 284.8 eV.
To enhance the electrical conductivity and hence the electrochemical activity of PPy/MnO2, MWCNTs of high aspect ratio (1250–6500) were added as a conductive filler. A stable dispersion of MWCNTs was prepared by sonicating MWCNTs in water with the help of a 5% hydroxypropyl methylcellulose (HPMC) solution. The composites of PPy/MnO2 sheets with different concentrations of MWCNTs (1–5 wt%) were prepared by sonicating the required amount of PPy/MnO2 with MWCNTs, and their electrochemical activity was recorded by CV experiments in the presence of 5 mM K4[Fe(CN)6] in 0.1 M KCl. The electrochemical activity of the GCE modified with a mixture of pure PPy and MWCNT (PPy/MWCNT) was also investigated by a similar method.
Dissociation of KMnO4 in water is represented as KMnO4 → K+ + MnO4−
(1) |
(2) |
(3) |
(4) |
(5) |
(6) |
Thus, a significantly negative value of ΔG° (−103.44 kcal mol−1) predicts the feasibility of polymerization initiation, i.e., the spontaneous generation of pyrrole radical cations at the interface. The mechanism of the redox-initiated polymerization of pyrrole in the presence of KMnO4 to yield PPy/MnO2 is shown in Scheme 1.37
As shown in the photographic images, the initial stages of polymerization and the simultaneous adsorption of PPy/MnO2 at the 2-D interface of water and chloroform led to the confinement of 2-D PPy/MnO2 sheets within 15 hours. The 2-D L/L interface formed between water and chloroform serves as a reactive template for the organization of reactive molecules.38 Initially, the monomer pyrrole and oxidant KMnO4 meet at the interface, where they undergo a redox reaction to form pyrrole radical cations and MnO2 (eqn (1)–(3), Fig. 1A 1). The subsequent steps lead to the formation of charged PPy oligomers with attached MnO2 that are difficult to confine at the interface due to their continuous adsorption/desorption at the L/L interface.15,19,21,22,39,40 As per the Pieranski equation, the stabilization of the L/L interface by the minimization of Helmholtz free energy is influenced mainly by the size of the adsorbed particles.18 Hence, the abrupt nature of the L/L interface leads to continuous adsorption/desorption of smaller particles at the L/L interface;18 therefore, small-sized charged oligomers freely migrate towards the polar aqueous phase.13,15,41,42 The formation of intense dark coloration in the aqueous phase within 5 hours manifests PPy/MnO2 assembly formation within 5 hours, as shown in Fig. 1A 2. Within 7.5 hours of polymerization, a substantial increase in the chain length of oligomers or short-chain polymers and an increase in the size of attached MnO2 occur. The interface tends to adsorb MnO2 NP-attached PPy chains towards the interface to minimize the high interfacial tension and high interfacial free energy (Fig. 1A 3).18,24,43 The interfacial adsorption of MnO2 attached oligomers, or short-chain polymers, acts as the driving force for the confined 2-D growth of PPy sheets. The 2-D ordering of PPy chains and the layer-by-layer growth of π–π stacked 2-D aligned PPy chains at the water/chloroform interface resulted in PPy/MnO2 sheets at the end of 15 hours (Fig. 1A 4).44 The preferential adsorption of MnO2 attached PPy chains followed by jamming at the L/L interface could offer PPy sheets with uniformly distributed MnO2 NPs. The observation of transparency in the aqueous phase (upper layer) in the photographic image of Fig. 1A 4 implies the confinement of PPy/MnO2 sheets at the interface. The photographic images of the polymerization captured at 2.5, 10, and 12.5 hours during the reaction are shown in Fig. S1.† The control experiments of interfacial polymerization using lower (0.005 M) and higher (0.02 M) concentrations of the monomer and oxidant were performed (Fig. S3†). As observed in the photographic images (Fig. 1A 4 and Fig. S3A†), PPy/MnO2 illustrated final product confinement at the interface for lower concentrations (0.005 M and 0.01 M) of reactants. The final products were dispersed in the aqueous phase (Fig. S3B†) for higher concentrations of reactants (0.02 M). The top view photographic images in Fig. S4† demonstrated increased interfacial product confinement for a reaction conducted using 0.01 M concentrations of the monomer and oxidant. Since the middle concentration yielded a significant amount of product confinement at the interface, detailed investigations of nanoparticle-aided morphology tuning of polypyrrole were conducted using 0.01 M concentrations of reactants.
The adsorption of NP-attached oligomers at the interface results in the confinement of short-chain polymers, which may subsequently reduce the interfacial tension at the L/L interface. The pendant drop tensiometry studies evaluated the variation of interfacial tension due to the adsorption of products during the polymerization. The γ values were measured by suspending drops of different concentrations of oxidants (0.005 M, 0.01 M, and 0.02 M) in monomer dispersions (0.005 M, 0.01 M, and 0.02 M), and the results are summarized in Fig. 1B and C and Fig. S5.† The interfacial tension of pure water and chloroform was 34 mN m−1 under the same experimental conditions; the drops remained at the tip for less than 2 minutes. In the case of reaction mixtures of different concentrations, the pendant drops exhibited significant stability for up to 90 minutes, accompanied by a reduction of γ for all three concentrations (Fig. 1B and Fig. S5†). The pendant drops of 0.01 M concentration showed γ reduction from 32 mN m−1 to 17 mN m−1 (Fig. 1B). Similarly, 0.005 M and 0.02 M showed a γ reduction of 34 mN m−1 to 21 mN m−1 and 34 mN m−1 to 22 mN m−1 (Fig. 1B), respectively. Thus, as shown in the inset of Fig. 1B, the extent of decrease in IFT (Δγ) for 0.005 M, 0.01 M, and 0.02 M is 13 mN m−1, 15 mN m−1, and 12 mN m−1, respectively. The greater extent of IFT reduction could be attributed to the adsorption of nanoparticle-attached oligomers or short-chain polymers at the interface. A similar trend was reported for lignin nanoparticle adsorption for the 1-pentanol/water interface stabilization by IFT reduction during oil-spill recoveries.9 However, at a higher amount of product formation (for 0.02 M concentration), the IFT reduction is relatively minor. The preponderant solvent–polymer interaction as compared to the adsorption energy may promote the product confinement at the polar phase, as shown in Fig. S3B.† Therefore, it is confirmed that the monomer and oxidant molecules present in the respective phases initially meet at the interface and initiates polymerization, as shown in Fig. 1A 1 and C. Nano-sized PPy/MnO2 adsorbs at the interface as the reaction proceeds, and the product morphology gets tuned to 2-D sheets (Fig. 1C and 1A2–4).
The reaction mixture from the aqueous phase (2.5 to 7.5 hours) and the interface (10 to 15 hours) was collected and investigated using UV-Vis absorption spectroscopy, as shown in Fig. 2A and B. The absorbance variation and wavelength shift in the UV-Vis spectra of PPy/MnO2 was analyzed as a function of reaction time, and the results are shown in Fig. 2A. The relative trend in the absorption intensity for the samples synthesized in 2.5 to 7.5 hours follows a concentration dependence as per the Beer–Lambert law.45 The monomer absorption peak corresponding to the π to π* transition was observed at 230 nm (Fig. S6†). Hence, the absorption peak at 240–242 nm is assigned to Py˙+ which is detected in the reaction mixtures collected between 2.5 and 7.5 hours.46,47 The self-assembly of radical cations during the initial stages of polymerization is reflected in the absorbance profile. Maximum accumulation of Py˙+ adjacent to the interface was observed at 5 hours, and the subsequent decrease in the absorbance is due to the growth of polymeric chains. Furthermore, the absence of an absorption peak corresponding to Py˙+ after 7.5 hours is due to the total consumption of Py˙+ during the polymerization. The absorption peaks centered at 394–415 nm corresponding to the low molecular weight oligomers were detected in all the PPy/MnO2 samples (2.5 to 15 hours).46,47 Similarly, a maximum accumulation of oligomers was observed at 5 hours, and the subsequent decrease in the absorbance is due to the growth of polymeric chains. The bands attributed to the polar transitions of the PPy backbone are observed at 495–620 nm, which were absent at 2.5 hours. A distinguishable trend in the absorbance was not observed in the samples collected at 5–15 hours.46–48 However, a significant blue shift of 107 nm was observed for the PPy backbone absorptions for 5–10 hours, reflecting the random distribution of polymeric chains nearby the interface. Nonetheless, a red shift of 125 nm was observed from 10–15 hours due to the decrease of bandgap due to polymeric chain elongation.
The absorption peak corresponding to α-MnO2 at 315–350 nm (ref. 49 and 50) showed the maximum absorbance at 5 hours; however, the absorbance decreased as the reaction progressed. Furthermore, a red shift of 30 nm in the absorption wavelength could be due to the growth of MnO2 NPs. Since visible confinement of PPy/MnO2 was observed after 10 hours, the growth of MnO2 attached PPy chains was evaluated from the bandgap (E = hc/λ, λ = absorption wavelength) calculations, as plotted in Fig. 2B. The bandgap of oligomers remained constant after 10 hours, indicating the unequivocal conversion of oligomers to polymers. The apparent increase in the π conjugation length of oligomers and short-chain polymers in PPy/MnO2 after 10 hours decreased the bandgap, as observed in Fig. 2B.45,51,52 Furthermore, a consistent reduction in the bandgap of MnO2 observed within 10–15 hours predicts an increase in the size of MnO2 after 10 hours of polymerization.53
Additionally, the reaction mixtures collected at various time intervals were investigated using Raman spectroscopy, as shown in Fig. 2C. The Raman spectrum of PPy/MnO2 after 15 hours of reaction showed well-defined peaks corresponding to the PPy backbone and MnO2 NPs. The peaks at 484 cm−1 and 606 cm−1 correspond to α-MnO2,54,55 and the peaks at 800 cm−1, 1642 cm−1 and 1067 cm−1 can be attributed to the low-frequency C–C vibration,56 CC stretching mode48,57 and C–H in-plane bending vibrations of PPy,48,57 respectively. The intensity of Raman peaks is directly proportional to the concentration of active species.58 The peaks at 484 cm−1 and 606 cm−1 of α-MnO2, and 1642 cm−1 of PPy have remarkable intensity and consistency in all the samples. Hence these peaks were focused on investigating the mechanism of polymerization as a function of reaction time (Fig. 2C and D). The polymerized products are distributed in the aqueous phase for 2.5 to 7.5 hours, and the confinement becomes prominent from 10 hours. The MnO2 attached oligomers are initially formed at low concentrations at the interface within 2.5 hours. As a result, the Raman peaks corresponding to α-MnO2 and PPy are less intense, as shown in Fig. 2C and D. Due to the small size and high polarity, the MnO2 attached oligomers freely diffuse from the interface, leading to the formation of assemblies of MnO2 attached oligomers/short-chain polymers in the polar aqueous phase (Fig. 1A 2). Thus, after a reaction time of 5 hours, PPy/MnO2 is formed at the polar aqueous phase at a high concentration, and the intensity of the Raman peaks increases gradually (Fig. 2C and D). After 7.5 hours, the pervasive need for interfacial stabilization starts playing, and the interface begins to preferentially adsorb nano-sized MnO2 attached oligomers/short-chain polymers towards it (Fig. 1A 3). This led to a sudden decrease in the intensity of the Raman peaks, as can be seen in Fig. 2C and D. After 10 hours, the interface starts to confine the adsorbed nano-sized particles, and the 2-D growth of nano-sized MnO2 attached oligomers leads to the confinement of PPy/MnO2 sheets at the interface. The intensity of the Raman peaks shows a linear trend after 10 hours due to the possible increase in the concentration of PPy/MnO2 sheets formed at the interface (Fig. 2C and D). Furthermore, the interface promotes the layer-by-layer growth of sheets by π–π stacking interactions.44 The π–π interactions during the assembly of multilayer graphene sheets have been reported to furnish more intense Raman peaks.59
The practical 2-D nanostructural tuning of PPy/MnO2 nanocomposites was achieved by the combined effect of interfacial stabilization and the formation of NP-attached oligomers. The transmission electron microscopy images (Fig. 3) reveal the morphological evolution of PPy/MnO2 synthesized in the water/chloroform bisolvent medium over 15 hours. As indicated in TEM images (Fig. 3A1, B1, and C1), the agglomerated network-like structures strengthen the concept of self-assembly of MnO2 attached oligomers in the initial stages of polymerization as discussed in Fig. 1A 1–1A 3. However, as the reaction progressed from 10–15 hours, the evolution of 2-D sheet-like structures (Fig. 3D1, E1, and F1) further confirmed the confinement of oligomers or short-polymeric chains at the interface that tunes the polymers to the 2-D sheet-like structures. The TEM images show the 2-D sheet-like morphology of PPy/MnO2 formed at the interface for 10–15 hours. High magnification TEM images of all samples are shown in Fig. S7;† a relatively uniform distribution of MnO2 particles in the polymeric matrix is evident in Fig. 3F1 and Fig. S7F.† Furthermore, the corresponding selected area electron diffraction patterns support the formation of the tetragonal structure of α-MnO2.32,54,60,61 The planes (002), (200), (211), (220), (310), (400), (402), (411), (431), (440), (521), (541), (600), (602), (710), (730), and (741) are reported for α-MnO2 (JCPDS no. 00-044-0141).32,54,60,61 The planes corresponding to the polypyrrole backbone were not present in the samples. As the reaction progressed from 2.5 hours to 15 hours, the nature of diffraction patterns ranged from diffused rings to bright rings and bright Bragg spots analogous to a set of planes of α-MnO2. Furthermore, the TEM images and the diffraction patterns confirm the interface confinement-induced morphology and crystallinity tuning of PPy/MnO2 composites. This further confirms the synergistic effect of the high interfacial tension-induced confinement of MnO2 NPs, and confinement-induced morphology tuning. As reported previously, efficient interfacial stabilization is achieved for larger particles, which could be a possible reason for the visibly recognizable confinement of products only after 10 hours during the polymerization.18 Due to the varying size and shape of PPy/MnO2 agglomerates and evident transition from agglomerated network-like structures to a distinct 2-D sheet-like morphology, the SAED patterns of PPy/MnO2 synthesized at varying reaction times may lack a few identical diffraction planes. As observed in Fig. 3, a consistently observed highly intense diffraction peak of the (310) plane was chosen to compare crystallinity using SAED patterns. An S-shaped growth curve in the intensity of the (310) plane is provided in Fig. S8.† An inflection point was observed at 8 hours, and the intensity becomes constant after 10 hours of polymerization. Hence, the SAED investigations confirm the interfacial tension driven adsorption of MnO2 NPs and the π–π stacking of PPy/MnO2 sheets at the interface. The morphology of PPy/MnO2 composites synthesized in a single solvent was also analyzed and compared with that of PPy/MnO2 sheets prepared at the interface (Fig. S9†). The FESEM image in Fig. S9A† clearly shows the 2-D sheet-like morphology of PPy/MnO2 sheets synthesized at the water/chloroform interface. However, the PPy/MnO2 composites prepared in a single solvent medium exhibited an agglomerated spherical morphology (Fig. S9B†). This could be due to the three-dimensional diffusion of monomers and the resultant secondary growth of oligomers in the bulk aqueous phase.25 Thus, the superior nature of the L/L interface in fine-tuning the 2-D morphology is further validated.
The presence of characteristic elements (carbon, nitrogen, manganese, and oxygen) and the distribution of MnO2 NPs in the PPy/MnO2 sheets (after 15 hours) were further investigated with HRTEM images, elemental mapping images, and the EDS spectrum (Fig. 4A–D and Fig. S10 and S11†). The carbon and nitrogen represent the PPy backbone in 2-D sheets, and the corresponding elemental mapping images are shown in Fig. 4B and Fig. S10B.† The elemental mapping images (Fig. 4C and D) and the corresponding HRTEM images represent a uniform encapsulation of MnO2 NPs in PPy sheets (Fig. S10A, C and D†). The few-layer nature of PPy/MnO2 sheets is also visible in Fig. S10A, C and D,† where the MnO2 NPs exhibit less particle agglomeration. The uniform distribution of manganese and oxygen in PPy/MnO2 sheets is evident in Fig. 4C and D. The bright spots in the SAED pattern of Fig. 3F2 demonstrated the highly crystalline nature of PPy/MnO2 sheets synthesized in 15 hours. XRD studies further examined the long-range order crystallinity of the PPy/MnO2 sheets, and the spectrum is shown in Fig. 4E. The peak positions of the XRD spectrum match well with α-MnO2 (JCPDS card no. 00-044-0141). The peak corresponding to the Bragg reflections caused by the interplanar spacing of PPy chains is absent in the XRD spectrum.24 This could be due to the highly crystalline nature of MnO2 that subsides the diffractions caused by amorphous PPy.24 The peaks at 2θ = 13.461°, 20.874°, 28.829°, 37.507°, 62.818°, 69.688°, 77.101°, and 84.152° can be attributed to the Bragg diffractions caused by the (110), (200), (310), (211), (521), (541), (402) and (512) planes, respectively.32,54,60 The XRD spectrum (Fig. 4E) and SAED pattern (Fig. 3F2) of PPy/MnO2 sheets show dissimilar existence of diffraction planes. This could be because XRD records long-range order crystallinity over the bulk crystal, and SAED measures short-range order crystallinity in selected portions.24 The small shifts observed in the diffraction peaks could be due to the possible lattice deformations caused by the entrapment of MnO2 NPs inside the PPy sheet matrix.62 In addition, the shifts in the peak positions corresponding to the (110), (200), and (521) planes towards higher angles are observed as in Fig. 4E. This could be due to the compressive strain imposed by the amorphous PPy matrix on the crystalline MnO2 lattice that leads to a decrease in lattice spacing and an increase in Bragg angle.62,63 The XRD spectrum of PPy/MnO2 synthesized in a single solvent system demonstrated the characteristic crystalline peaks of MnO2 along with the peaks corresponding to Mn3O4 as impurity (Fig. S12†). The peaks at 2θ = 37.878°, 45.111°, 51.6°, 58.55°, 65.725°, 72.98°, 79.68°, and 87.078° are attributed to crystalline MnO2.64–67 The characteristic peaks of Mn3O4 are centered at 17.09°, 24.08°, and 30.83°.68,69 Thus, the L/L interface tunes the polymerization in a controlled manner, eliminating the formation of undesirable oxides of manganese and resulting in pure MnO2 NPs. The potential capability of the water/chloroform interface in thinning the PPy/MnO2 sheets to a few nanometres is also investigated using atomic microscopy images. The 3-D AFM image (Fig. 4F) and 2-D AFM image (Fig. S13A†) of PPy/MnO2 sheets synthesized in 15 hours exhibited densely populated MnO2 NPs submerged in PPy sheets over an area of 4 μm2. The surface profile plots attributed to the 2-D AFM image in Fig. S13A† predict an average thickness of ∼6 nm for ultra-thin PPy/MnO2 sheets (Fig. S13B†). The XPS spectrum shows the valence states and bonding nature of the characteristic elements of PPy/MnO2 sheets synthesized in 15 hours. The XPS survey scan spectrum reveals the existence of C, N, Mn, and O in PPy/MnO2 sheets (Fig. 4G). The high-resolution C 1s spectrum in Fig. 4H shows four prominent peaks at 284.7 eV, 285.7 eV, 288.25 eV, and 292.68 eV.70–72 The peaks at 284.7 eV, 285.7 eV, and 288.25 eV can be assigned to carbon–carbon, carbon–nitrogen, and carbon–oxygen, respectively.70–72 The peak at 292.68 eV corresponds to the carboxyl group that may be generated during the over-oxidation of the PPy backbone due to the oxidant KMnO4.71 The N 1s spectrum in Fig. S13C† shows the deconvoluted peak corresponding to pyrrolic nitrogen (–N–H).73 The core-level spectrum of Mn 2p shows a spin doublet of Mn 2p1/2 and Mn 2p3/2 located at 642.5 eV and 654.18 eV (Fig. 4I).70,74–76 The spin energy difference between these two peaks gives a binding energy of 11.68 eV, which confirms the presence of Mn4+ in PPy/MnO2.74 The spin doublets of Mn 2p1/2 and Mn 2p3/2 are further deconvoluted to few other peaks to confirm the possible valence states of Mn. The peaks at 642.45 eV and 654.18 eV are assigned to Mn4+.76,77 The deconvoluted Mn 2p spectrum also possesses a less intense peak at 644.9 eV corresponds to Mn2+.76,77 This indicates a small amount of Mn2+ formed during the reduction of KMnO4 to MnO2. The peak for O 1s at 532 eV can be deconvoluted into three prominent peaks at 530 eV, 531.45 eV, and 533.5 eV (Fig. 4J). The peak at 530 eV is assigned to the O–Mn bond, which further confirms the formation of MnO2.33,76,77 The low intense peak at 531.45 eV and 533.5 eV can be attributed to O–C and O–H bonds.33,76,77
The structure-related properties of PPy/MnO2 sheets can be utilized for various potential applications. The electrochemical detection of nicotine by interfacially synthesized PPy/MnO2 sheets was investigated, and the results are presented in Fig. 5. The CV scans of bare GCE and PPy/MnO2 modified GCE in 1 mM nicotine are shown in Fig. 5A. The inset in Fig. 5A shows the oxidation peaks for the bare GCE, and PPy/MnO2 modified GCE at 1.07 V (73 μA) and at 1.03 V (39 μA), respectively. To enhance the electrical conductivity and electrochemical activity of PPy/MnO2 sheets, a high aspect ratio MWCNT was incorporated into PPy/MnO2 sheets. MWCNTs as a conductive filler is highly promising because they promote enhanced electron transfer due to their high electrical conductivity and surface area.78 A required amount of PPy/MnO2 was mechanically mixed with varying wt% (1–5) of MWCNTs. The electrochemical activity of the as-prepared composites was examined using CV scans (Fig. 5B) in 5 mM K4[Fe(CN)6] in 0.1 M KCl, and the oxidation currents were compared (Fig. 5C) to evaluate the effect of MWCNTs in the composites. An optimum current (428 ± 9 μA) was exhibited on the addition of 3 wt% MWCNTs, and further addition decreased the oxidation current to 367 ± 1.5 μA. This could be due to particle agglomeration from dense MWCNT networks at an elevated amount of MWCNTs (Fig. 5C).79 Therefore, 3 wt% was identified as the optimum concentration required for the percolation threshold, and the composite with 3% MWCNTs was selected for the electrochemical detection of 1 mM nicotine (Fig. 5D). The PPy/MnO2 – 3% MWCNT modified GCE (Fig. 5D.i) showed an enhanced electrochemical activity with an onset oxidation potential of 0.68 V and a maximum current of 332 μA (inset of Fig. 5D).
The electrochemical oxidation of nicotine occurs at a very high oxidation potential.80 The main challenge in developing electrochemical nicotine sensors is to decrease the high overpotential of nicotine oxidation and enhance the overall performance. Here, MnO2 NPs uniformly attached in PPy sheets as in Fig. 3F1 and Fig. S7F† act as catalysts for the oxidation of nicotine. The incorporation of a minimal amount of MWCNTs as a filler in PPy/MnO2 improved the performance of the electrochemical nicotine sensor with a 355% increase in the oxidation current at a low onset potential of 0.68 V. Furthermore, the electrochemical detection of nicotine using various other modified electrodes, such as pure PPy (Fig. 5D.ii), pure MWCNTs (Fig. 5D.iii), and PPy – 3% MWCNTs (Fig. 5D.iv) was also analyzed. These modified electrodes did not give apparent peaks corresponding to nicotine oxidation, as shown in the inset of Fig. 5D. The maximum anodic currents from the respective CV scans of the three potential electrodes (bare GCE, PPy/MnO2 modified GCE, and PPy/MnO2 – 3% MWCNT modified GCE) were compared and are presented in Fig. S14.† The differential pulse voltammograms of all modified electrodes in 1 mM nicotine were also recorded (Fig. S15†). This further confirms the exclusive catalytic activity of MnO2 NPs in the oxidation of nicotine.
The printable nature of PPy/MnO2–MWCNT composites on the SPE opens a new route for successfully preparing miniaturized electrode set-ups for nicotine detection. The electrochemical sensing of nicotine in commercial screen printed electrodes (Zensor TE100) was also tested. The schematic representation of nicotine oxidation by PPy/MnO2–MWCNTs on the SPE is shown in Fig. 5E. The electrochemical oxidation of nicotine is a two-electron mediated N-methyl hydroxylation reaction (Fig. 5E).80,81 The PPy/MnO2–3% MWCNT modified SPE showed a high oxidation current of 175 μA towards the electrochemical detection of 1 mM nicotine (Fig. 5F). The difference in the anodic current of commercial SPE compared to that of GCE may be attributed to the difference in the electrode combinations, design, and materials used. The DPV scans of bare and modified SPE are shown in Fig. S16.† Thus, the conductive composites of PPy/MnO2 sheets are ideal for successfully developing high-performance electrochemical nicotine sensors.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2nr02130g |
This journal is © The Royal Society of Chemistry 2022 |