Open Access Article
Pranav Mecheri,
Swathi Vaidyanatha Iyer,
Lekshmi Bindu Raveendran and
Mini Mol Menamparambath
*
Department of Chemistry, National Institute of Technology Calicut, Calicut-673601, Kerala, India. E-mail: minimol@nitc.ac.in
First published on 17th June 2026
Epinephrine (EP), a critical hormone secreted by the adrenal glands, is a vital clinical biomarker linked to various neurological and cardiovascular disorders, making its accurate monitoring essential for diagnosis and patient management. Herein, we report a nonenzymatic electrochemical sensor for EP detection based on carbon yarn (CY) functionalized with cobalt molybdenum oxide (CMO) nanorods. A liquid/liquid interface-assisted strategy using n-butanol and water was employed to tailor the growth of CMO nanostructures. Importantly, the influence of metal precursor concentration on morphology evolution and electrochemical performance was systematically investigated. Controlled nanorod architectures of CMO were formed at optimized concentrations, whereas higher concentrations yielded irregular flake-like structures with minor impurity phases and reduced activity. The optimized CMO-modified carbon yarn exhibited excellent electrochemical activity for EP detection, demonstrating high selectivity, stability, repeatability, and a low detection limit of 2.14 nM. The sensor's practical applicability was validated using real samples, including EP injection solutions and human serum. Finally, a flexible device was fabricated, delivering promising performance.
A range of analytical methods is available for the detection of epinephrine, which includes ratiometric,2 colorimetric,7 high-pressure liquid chromatography,8 and surface-enhanced Raman scattering.9 Although these approaches offer good sensitivity and reliability, many of them require complex instrumentation, extensive sample preparation, and higher operational costs. In contrast, electrochemical sensing has circumvented these barriers and emerged as a more practical and efficient alternative due to its rapid response, simplicity, and low cost. Electrochemical strategies can be broadly classified into enzymatic and non-enzymatic approaches. Enzymatic sensing relies on immobilizing specific enzymes onto the electrode surface, but this process is intricate and requires tightly controlled reaction conditions to maintain enzyme activity. Non-enzymatic electrochemical sensing overcomes these limitations by employing catalytically active electrode materials that directly facilitate the redox reaction of the analyte, enabling stable and reliable detection.10–12 Metals and metal oxides/hydroxides have therefore become attractive coating materials for non-enzymatic electrochemical sensors owing to their strong catalytic activity, stability, crystallinity, and high surface area.13–18 When integrated onto the electrode surface, these materials provide abundant active sites, thereby improving sensitivity and overall sensing performance.
In this work, cobalt molybdenum oxide nanostructures were synthesized using a liquid/liquid interface-assisted strategy, employing n-butanol and water as two immiscible phases. The influence of metal precursor concentration in the aqueous phase on the material properties was systematically examined. X-ray diffraction (XRD), Raman, and Fourier transform infrared (FTIR) analyses confirmed the successful formation of cobalt molybdenum oxides, while higher precursor ratios were found to introduce impurity phases. Field-emission scanning electron microscope (FE-SEM) imaging revealed notable morphological changes with varying precursor concentrations. Low and moderate metal concentrations result in nanorod-like morphologies, whereas higher concentrations yield larger flakes. Electrochemical studies using CV and EIS indicated that CY coated with the sample synthesized at 1 mmol of metal precursors in 20 ml of aqueous medium (CM-B) exhibited superior activity. The materials were subsequently coated onto single strands of carbon yarn and assessed for their performance in detecting the neurotransmitter epinephrine. The sensor demonstrated excellent electrocatalytic activity toward EP, with high stability, selectivity, and repeatability. Its real-time applicability was further validated using human serum and EP injection samples. Finally, a flexible, miniaturized version of the sensor was fabricated, showing promising sensing performance.
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3, v/v), collected by vacuum filtration, and dried in a hot-air oven at 60 °C to yield the final products.
For the fabrication of the flexible sensor, a rectangular substrate (5 × 2 cm2) was prepared using a transparent polyester film. The surface of the film was laminated with a polyimide heat-resistant adhesive tape to provide mechanical stability and thermal protection. A rectangular strip of pyrolytic graphite sheet was attached to one end of the substrate, serving as the counter electrode. The same pyrolytic graphite surface, coated with silver paste to function as the reference electrode. The material-coated carbon thread was positioned at the center of the substrate to act as the working electrode. Electrical connections for all electrodes were established using copper tape, ensuring stable and low-resistance contact throughout the setup.
| 6CO(NH2)2 → C3H6N6 + 6NH3 + 3CO2 |
| NH3 + ROH → NH4+ + OR− |
OR− + H2O ROH + OH− |
| (NH4)6Mo7O24·4H2O + H2O → 6NH4+ + Mo7O246− + 5H2O |
| Mo7O246− + 8OH− → 7MoO42− + 4H2O |
| 7Co2+ + 7MoO42− + nH2O → 7CoMoO4·nH2O |
The crystal structure and crystallinity of the synthesized compounds were examined using XRD, and the corresponding diffractograms are presented in Fig. 1a. The diffraction patterns confirm the formation of monoclinic cobalt molybdenum oxide hydrate (CoMoO4·nH2O) in all samples, consistent with the ICDD reference pattern 00-026-0477. A schematic representation of the crystal structure generated using VESTA is illustrated in Fig. 1b. Notably, the CM-C sample, prepared at a higher precursor concentration, exhibits additional diffraction peaks corresponding to cobalt hydroxide (ICDD 00-046-0605) and residual ammonium molybdate (ICDD 00-027-1013), indicating the presence of minor impurities. The formation of these secondary phases can be attributed to incomplete interfacial reaction kinetics under high precursor concentration, where excess cobalt ions tend to hydrolyze, leading to the precipitation of Co(OH)2, while the surplus molybdate ions reprecipitate as ammonium molybdate. In contrast, CM-A and CM-B exhibit relatively pure-phase cobalt molybdenum oxide without secondary phases. Among all the samples, CM-B displays the highest peak intensity and sharpest diffraction features, indicative of superior crystallinity of a well-ordered crystal structure.
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| Fig. 1 (a) XRD patterns, (b) schematic view of the crystal structure, (c) Raman spectra, (d) FTIR spectra, (e) EIS spectra, and (f) bar graph showing Rct values of bare and CMO-coated carbon yarns. | ||
The vibrational characteristics of the synthesized compounds were further investigated using Raman spectroscopy, and the corresponding spectra are shown in Fig. 1c. The intense bands observed at approximately 929 cm−1 and 868 cm−1 are assigned to the Co–O–Mo stretching vibrations of CMO.21,22 The band at 810 cm−1 corresponds to the asymmetric stretching of O–Mo–O, while the bands at 334 and 361 cm−1 are attributed to the asymmetric and symmetric bending modes of O–Mo–O, respectively.21,23 In the CM-C sample, additional peaks indicating the presence of impurity phases appeared at 219, 723, and 944 cm−1 for ammonium molybdate24 and 460 cm−1 for cobalt hydroxide,15,25 in agreement with the XRD observations. FTIR analysis was conducted in the range of 400–4000 cm−1, and the corresponding spectrum is shown in Fig. 1d. The bands around 735, 847, and 958 cm−1 correspond to the stretching and bending vibrations of Mo–O–Mo in the MoO42− unit.26 A broad band around 3000–3500 and 1631 cm−1 is assigned to bending and stretching vibrations of crystallisation or adsorbed water.26 Bands that are observed at 1396 and 1109 cm−1 are likely to be associated with the intercalation of NO32−, CO32− ions, respectively.27,28 Similar to the XRD and Raman results, the CM-C sample exhibits additional impurity-related bands. The signals observed at 881 and 480 cm−1 are assigned to the Mo
O stretching and Mo–O–Mo flexural modes of ammonium molybdate,29 while the band at 626 cm−1 corresponds to the δ(Co–O–H) vibration of cobalt hydroxide.30
The charge transfer characteristics of the synthesized compounds were evaluated using EIS with CMO-coated carbon yarn as working electrodes. The corresponding Nyquist plots for the coated and bare electrodes are shown in Fig. 1e. Each plot displays a semicircular region followed by a linear portion, where the diameter of the semicircle corresponds to the charge transfer resistance (Rct). The equivalent electrical circuits used for fitting are presented in Fig. S1. The electrodes coated with the synthesized samples exhibit significantly lower Rct values compared to the bare electrode (Fig. 1f), confirming their enhanced charge transfer characteristics. Among the tested samples, CM-B/CY demonstrates the lowest Rct, indicating superior charge transfer capability, facilitating the electrochemical activity of the electrodes.
The morphology of the synthesized nanostructures was examined using SEM, as shown in Fig. 2a–c & S2a–c. Samples CM-A and CM-B exhibit nanorod-like morphologies, whereas CM-C displays a agglomerated flake-like structure. In solution-phase nanocrystal growth, both surface reaction and mass transport through the boundary layer can act as the rate-determining step, depending on precursor concentration and localised diffusion characteristics.31,32 In the present system, increasing the metal ion concentration enhances nucleation density and reduces diffusion length, thereby promoting faster ion supply to the growing crystal. Consequently, the growth rate is limited by the surface reaction, resulting in surface-controlled growth and the formation of flake-like morphologies. In contrast, at lower precursor concentrations, the slower ion diffusion renders mass transport the rate-limiting step, resulting in anisotropic, diffusion-controlled growth of nanorods. The average diameter of CM-A nanorods is about 600 nm, that of CM-B ranges from 300 to 500 nm, and the flake thickness in CM-C is approximately 270 nm.
The morphology and crystallinity of CM-B were further evaluated by TEM and SAED, as shown in Fig. 2d–g. TEM images Fig. 2d and e reveal uniformly distributed, rod-like nanostructures of 223 nm thickness with smooth surfaces and well-defined morphology. The high-resolution TEM image (Fig. 2f) clearly displays distinct and periodic lattice fringes with an interplanar spacing of 3.3 Å, corresponding to the (012) plane, consistent with the XRD results. The continuous and uninterrupted lattice fringes across the entire nanorod indicate a coherent crystal lattice without defects or misorientations, confirming its single-crystalline nature. The SAED pattern (Fig. 2g) reveals sharply defined Bragg spots indexed to distinct crystal planes, further corroborating the single-crystalline nature and high degree of structural order in CM-B nanorods. Together, these results demonstrate that the synthesized CM-B nanorods possess superior crystallinity and atomic uniformity. The distribution of elements in the crystal was subsequently analyzed by TEM mapping, and the corresponding mapping images are given in Fig. 2h–l. The EDS spectrum shown in Fig. S3 further supports these results. The uniform distribution of cobalt, molybdenum, and oxygen confirms the homogeneous composition and successful formation of CMO.
The chemical states of the elements in the CMO sample were analyzed using XPS, and the corresponding survey and deconvoluted spectra are presented in Fig. 3. The survey spectrum (Fig. 3a) confirms the presence of cobalt, molybdenum, and oxygen in the material. The high-resolution Co 2p spectrum (Fig. 3b) displays distinct peaks at 781.1 eV and 797.1 eV, assigned to Co 2p3/2 and Co 2p1/2, respectively, along with two shake-up satellite peaks at 785.7 eV and 802.9 eV, indicating the presence of Co2+ species.33,34 The deconvoluted Mo 3d spectrum, as depicted in Fig. 3c, shows peaks at 232.0 eV and 235.2 eV, corresponding to Mo 3d5/2 and Mo 3d3/2, respectively, confirming the presence of Mo in the +6 oxidation state.34,35 The O 1s spectrum (Fig. 3d) exhibits peaks at 530.3 eV and 532.2 eV, where the lower binding energy peak is attributed to lattice oxygen (metal–oxygen bonds), while the higher energy peak is related to surface-adsorbed oxygen species.35,36
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| Fig. 3 XPS spectra of CM-B: survey scan (a), deconvoluted spectra of cobalt (b), molybdenum (c), and oxygen (d). | ||
The synthesized materials were subsequently coated onto carbon yarns peeled off from carbon cloth for electrochemical characterization. A detailed schematic representation of the process is provided in Fig. 4a. Carbon yarns, each approximately 6 cm in length, were first pretreated with acetone to remove any surface impurities or organic residues adsorbed. The pretreated yarns were then dried in an oven maintained at 60 °C to ensure complete removal of residual solvent. Following the cleaning step, the yarns were immersed in a well-dispersed CMO suspension prepared in DMSO and mechanically agitated for one hour to promote uniform deposition of the active material onto the carbon fibers. Finally, the coated yarns were dried in an oven to obtain the CMO-coated carbon yarn electrodes with a stable and adherent surface layer. The SEM images of the bare carbon yarn (i, ii) and CMO-coated yarns (iii) are given in Fig. 4b. This CMO-coated carbon yarn was used as the working electrode for all electrochemical measurements. The schematic representation of the oxidation of epinephrine at the surface of CMO-coated carbon yarn (CMO/CY) is given in Fig. 4c.
The electrochemical activity of the prepared materials was evaluated using cyclic voltammetry in 5 mM K3[Fe(CN)6] containing 0.1 M KCl, and the corresponding voltammogram is shown in Fig. 5a. As evident from the figure, the CM-B/CY sample exhibits significantly higher redox peak currents than bare carbon yarn as well as CM-A/CY and CM-C/CY coated yarns, indicating its superior electrochemical activity. To further assess the materials' performance toward epinephrine sensing, CV was performed in 1 mM EP prepared in PBS (Fig. 5b). It further validates that CM-B/CY delivers the highest peak current response among all samples, as shown in Fig. 5c. This enhanced electrochemical performance of CM-B/CY is attributed to its relatively smaller sized nonorods with an expected higher surface area compared to CM-A. Furthermore, the CM-C shows highly agglomerated nonoflake-like structures, which may reduce the accessibility of the active surface area for electrochemical reactions. The presence of impurity phases will also disrupt the continuity of the electroactive matrix in CM-C, which introduces interfacial heterogeneity, leading to inefficient electron-ion transport and diminished overall electrochemical performance. The optimum pH for EP electrocatalytic detection was determined by performing CV and DPV measurements at pH values ranging from 5 to 9, and the corresponding graphs are presented in Fig. 5d and S4, respectively. Based on the highest anodic current response, pH 7 was identified as the optimal condition for electrocatalytic oxidation of EP. DPV analysis was performed at varying EP concentrations to determine the lowest limit of detection (Fig. 5e). The corresponding calibration curve, showing the relationship between peak current and concentration, is plotted in Fig. 5f. The curve follows the linear regression equation y = 0.0006x + 0.2015 with an R2 value of 0.9982. The limit of detection (LOD) was calculated using the standard equation LOD = 3Sb/m, where Sb is the standard deviation of the blank signal and m is the slope of the calibration plot. The resulting LOD was 2.14 nM, which is comparable to or even better than previously reported values, as illustrated in Table S2.
The electrocatalytic mechanism at the electrode surface was evaluated by the scan rate. For this, CV was performed at different scan rates ranging from 10 to 100 mV s−1, as shown in Fig. 5g. The calibration plot of peak current versus scan rate is given in Fig. 5h. This plot follows the linear regression equation y = 0.6195x + 21.1910 with an R2 value of 0.9972. The linear nature of this curve indicates that the electrocatalytic mechanism at the electrode surface is surface-controlled. The influence of common interfering species on EP detection was assessed by performing DPV measurements (Fig. S5) using 1 μM EP in the presence of interfering agents at 100-fold higher concentrations (100 μM). The corresponding current responses in the preferred potential range are presented in Fig. 5i as a bar graph. The markedly lower currents obtained for the interfering species compared to EP confirm the high selectivity of the prepared material toward EP detection.
Stability and repeatability are other important factors that influence the application of sensors. The stability of the sensor was evaluated by conducting 10 continuous cycles of CV in 0.5 mM EP at a scan rate of 50 mV s−1, and the corresponding curve is shown in Fig. 6a. A perfect overlap of each cycle with 99.32% retention of anodic current (0.24% RSD) indicates the sensor's high stability. Repeatability of the sensor was tested by carrying out CV using three different carbon yarns coated with CMO (Fig. 6b). The anodic current obtained for each electrode was almost similar, demonstrating the sensor's remarkable reproducibility. Since EP serves as an important neurotransmitter and regulates several vital physiological functions, accurately detecting its levels in real biological and medicinal samples is essential. Therefore, the applicability of the sensor was evaluated using real samples, including EP injection and human serum. Both solutions were diluted 20 times with 0.1 M PBS prior to electrochemical detection. Standard EP solutions were prepared, and known concentrations of these solutions were spiked into the diluted real samples. The DPV curves and the corresponding parameters for recovery of different additions are given in Fig. S6 and Table S3 for EP injection, and Fig. S7 and Table S4 for serum. The comparative current responses for the EP injection and serum with the standard EP solution are illustrated in Fig. 6c and d, respectively. The comparable current for both the real sample and the standard solution indicates the efficacy of the proposed sensor in detecting real samples.
A flexible, miniaturized form of the sensor was fabricated to check the practical usage of the sensor. Here, a polyimide-taped polyester film was employed as the substrate. The counter electrode was made from a pyrolytic graphite sheet, and the reference electrode was formed by applying a layer of conductive silver paste onto the graphite sheet. The CMO-coated carbon yarn positioned at the center functioned as the working electrode. The structural schematic and photographic images of the fabricated sensor are shown in Fig. 7a and b–f, respectively. DPV analysis was done using the sensor at different EP concentrations (100–200 μM), and the response obtained for the EP solutions is given in Fig. 7g. With increasing EP concentration, the peak current exhibited a gradual rise, confirming the sensor's potential applicability for practical EP detection.
Supplementary information: experimental details of the interface-assisted synthesis of CMO with their corresponding product code. EIS equivalent circuits of bare carbon yarn, CMO-coated carbon yarns. EDS spectra of CM-B. Comparison of electrochemical sensors for EP detection. DPV of EP and interfering agents. DPV of serum at different additions of standard EP. Recovery results of EP in EP injection. DPV of serum at different additions of standard EP. Recovery results of EP in serum. See DOI: https://doi.org/10.1039/d6sd00040a.
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