ABSTRACT Commercial wearable biosignal sensing technologies encounter challenges associated with irritation or discomfort caused by unwanted objects in direct contact with the skin, which

can discourage the widespread adoption of wearable devices. To address this issue, we propose a fabric-based lamina emergent MXene-based electrode, a lightweight and flexible shape-morphing

wearable bioelectrode. This work offers an innovative approach to biosignal sensing by harnessing the high electrical conductivity and low skin-to-electrode contact impedance of MXene-based

dry electrodes. Its design, inspired by Nesler’s pneumatic interference actuator, ensures stable skin-to-electrode contact, enabling robust biosignal detection in diverse situations.

those of commercial bioelectrodes. This work excels in recognizing various hand gestures through a convolutional neural network, ultimately introducing a shape-morphing electrode that

provides reliable, high-performance biosignal sensing for dynamic users. SIMILAR CONTENT BEING VIEWED BY OTHERS ADHESIVE FREE, CONFORMABLE AND WASHABLE CARBON NANOTUBE FABRIC ELECTRODES FOR

BIOSENSING Article Open access 09 December 2022 ALL-PRINTED NANOMEMBRANE WIRELESS BIOELECTRONICS USING A BIOCOMPATIBLE SOLDERABLE GRAPHENE FOR MULTIMODAL HUMAN-MACHINE INTERFACES Article

Open access 10 July 2020 3D PRINTABLE AND MYOELECTRICALLY SENSITIVE HYDROGEL FOR SMART PROSTHETIC HAND CONTROL Article Open access 21 January 2025 INTRODUCTION Wearable technology is

substantially gaining importance in the healthcare sector owing to various societal concerns, such as aging populations and the emergence of infectious diseases. Preventive medicine has the

potential to reduce social costs significantly by enabling early interventions against acute diseases1. However, the effective implementation of preventive medicine faces several challenges,

including difficulties in miniaturizing biodata acquisition systems, ensuring stable skin-to-bioelectrode contact, allowing continuous wear, and facilitating data analysis2. To address

these challenges, wearable healthcare systems have emerged as prominent candidates that can seamlessly collect and track user biodata3,4. Among the wearable healthcare systems,

tattoo-based5,6,7, and textile-based8,9 wearables have been extensively studied because of their potential for daily analysis of physiological diseases, such as cardiovascular diseases10,

muscle disorders11, Parkinson’s disease12, and Alzheimer’s disease13. Recent advancements in stretchable and flexible dry electrodes, which comprise one-dimensional (1D) or two-dimensional

(2D) conductive materials, have significantly improved their sensitivity, particularly for body suit-type applications14,15. Despite their advantages, wearable devices have persistently

caused issues of discomfort due to direct contact with the skin. Tokihiko et al. highlighted the importance of comfort-of-wear as a critical parameter for the future of wearables, similar to

selecting comfortable clothing16. This term describes the ability of a device to seamlessly integrate into a user’s daily life without causing any disruption or sense of irregularity

because of its physical presence. Although the size of current rigid wearable devices, such as wristwatches or rings, has been reduced to enhance comfort, the discomfort associated with

wearing such devices has failed to be eliminated16. Consequently, individuals sensitive to discomfort caused by irregular objects are discouraged from using these devices, which in turn

deters the adoption of wearable healthcare devices and limits the effectiveness of preventive medicine efforts. To tackle this issue, we present a fabric-based lamina emergent MXene-based

electrode (FLEXER) as a wearable biosensing electrode. This shape-morphing bioelectrode utilizes a laminar emergent mechanism crafted from thermoplastic polyurethane (TPU)-laminated cotton

fabric. The FLEXER has a symmetric whirlpool-shaped configuration that seamlessly transforms from a flat state to a scissor jack-like shape when pneumatic pressure is applied. The expanded

air pouch self-intersects, forming millimeter-sized joints that can be individually folded and unfolded, enabling conformal and stable electric contact with the skin even during motion. The

contact force of the FLEXER can be adjusted by controlling the air pressure and geometric characteristics of the joints. Additionally, the primary electrode material of the FLEXER is MXene,

a 2D material comprising transition metal and carbon with excellent electrical conductivity and mechanical durability17. To further enhance the mechanical properties18 and oxidation

resistance19,20 of MXene, it was supplemented with cellulose nanofiber (CNF)21 and polycarboxylate ether (PCE)22. This innovative FLEXER technology can seamlessly integrate into everyday

clothing, allowing for noninvasive monitoring of electrocardiogram (ECG) and electromyogram (EMG) signals. By combining the advantages of pneumatic lamina emergent systems and flexible MXene

electrodes, we were able to develop a concealable, fast, safe, and reliable biosensing electrode that revolutionizes the field of wearable health monitoring. RESULTS CONCEPT OF FLEXER AS A

WEARABLE DEVICE The FLEXER-based wearable healthcare system differs from conventional wearable healthcare systems in that it has a concealable design owing to its shape-morphing capability

(Fig. 1a (left)). Unlike other wearable systems that use bioelectrodes requiring constant direct skin contact, the FLEXER eliminates the constant need for physical contact. Traditional

bioelectrodes, particularly dry ones, require pressure application, which is usually accomplished with biomedical adhesives or pressure bandages23. However, the unique design of the FLEXER

allows it to be activated or deactivated as required (see Fig. 1a (right)), providing a user-friendly and adaptable solution. The operation of the FLEXER is elucidated by Nesler’s pneumatic

interference actuator (PIA) model24 (Fig. 1b). The PIA model can generate large deformation by strategically using the flexible structure’s crease. Specifically, when the flexible air pocket

is folded, it forms an overlapping volume at the creased section (Fig. 1b, State I). The overlapped volume decreases the overall volume of the air pocket below the original volume.

Consequently, the air pocket tends to revert to its original volume by flattening the crease (i.e., unfolding) when subjected to pneumatic pressure (Fig. 1b, State II). During this process,

the crease operates as a torque pivot point, inducing significant deformation in the structure24,25. The shape-morphing behavior of the FLEXER can be precisely controlled by coordinating

multiple PIA joints. The symmetrical arrangement of double-folded PIA joints, with one end touching the anchoring frame and the other end touching the center, enables the controlled movement

of the center electrode (CE) along an axis perpendicular to the contact plane of the FLEXER (Fig. 1c). The FLEXER system comprises three key components, as depicted in Fig. 1d. The first

component is the MXene/CNF/PCE (MX-CNF-PCE) composite electrode with a high electrical conductivity, flexibility, and oxidation resistance, and it is placed at the upper skin contact area.

This electrode is seamlessly integrated into cotton fabric using a solution spray method. It leverages the intricate 3D woven structure of the fabric to form a conductive network of MXene in

a 3D configuration. The 3D MXene electrode structure effectively confines mechanical damage to the outermost surface, thereby aiding in the preservation of conductivity in the event of

electrode delamination due to adhesion failure26. (Supplementary Fig. 1) The second component utilizes TPU, which is known for its mechanical resilience and stretchability, to create an air

pocket that is a fundamental part of the PIA system within the FLEXER27. TPU films have a low melting point of 140–150 °C, making them easy to meld28 using a customized XY plotter with a

soldering iron. The TPU-laminated cotton fabric was precisely cut using a customized computer numerical control (CNC) cutting machine (Fig. 1e and Supplementary Figs. 2 and 3). Finally, the

outer layer of the FLEXER is made from cotton fabric, which serves as its sheath. When users wear clothing embedded with the FLEXER, the overall appearance of the attire closely resembles

regular clothing (Supplementary Fig. 4). This distinguishes it from other wearable devices that usually have a tighter fit29. Notably, the FLEXER remains inconspicuous externally,

effectively reducing the possibility of social stigma associated with wearing it. The fabricated FLEXER was connected to an airline from a handheld air blower and stitched into the clothing

(Fig. 1f). The advantages of the FLEXER also include structural simplicity, which ensures durability without intricate mechanical component requirements; rapid actuation due to friction-free

pneumatic pressure; and paramount user safety, which stems from the absence of rigid parts and its PIA-based mechanism that allows for low pneumatic pressure usage and minimizes potential

risks. PHYSICAL AND DESIGN ANALYSIS OF FLEXER The straightforward linear structure with a double-fold design was examined to comprehensively explore the relationship between the pneumatic

structure of the FLEXER and its performance and design parameters. The linear PIA, measuring 11.8 cm in length and 1.9 cm in width (see Fig. 2a, top photographs), underwent an unfolding

actuation, which was recorded and analyzed using video analysis software (Kinovea). The inherent material characteristics of the cotton fabric caused the linear PIA to exhibit a

self-unfolding tendency even without the application of air pressure, as illustrated in Supplementary Fig. 5. To counteract this spontaneous unfolding, rubber magnets were affixed near the

linear PIA joints using magnetic force to impede undesired expansion (see Supplementary Fig. 6). Thereafter, the movement of the linear PIA end point and the angle changes of its joints were

observed during actuation. The graph in Fig. 2a (bottom right) illustrates that Joint 1 underwent rapid inflation and expansion between 100 and 125 ms, ultimately reaching a 180° angle by

175 ms (Supplementary Movie 1). Simultaneously, Joint 2 gradually expanded between 100 and 250 ms and then aggressively expanded at 250 ms after Joint 1 reached a straight angle. This

behavior is probably due to the folded portions of the linear PIA weakly obstructing airflow, leading to a sequential inflation process. By 375 ms, all the joints had fully expanded to their

maximum distance of 7.55 cm. Although the length of the linear PIA decreased from its initial value (11.8 cm) because of perpendicular expansion, the overall change in dimensions remained

minimal (see Supplementary Fig. 7 and Supplementary Movie 2 for further clarification). The linear PIA actuation behavior revealed that the joint close to the air pressure application point

tends to actuate faster than the joint at a further distance. This occurs because of the 180° bending angle of the airflow path that creates large drops of air velocity. Since the FLEXER has

multiple semicircular legs that require synchronized actuation, the parts that transfer air pressure to each leg were designed in a circular shape to minimize airflow interference when air

pressure is applied. As discussed earlier, the folded self-intersecting sections within the air pouch joints function as springs, directing the unconstrained end of the air pouch to move in

a manner that minimizes the volume of self-intersection. However, the actuation of a single-block air pouch actuator involves both lateral and vertical movements, making it difficult to

precisely control the direction of desired inflation. This limitation necessitates the incorporation of multiple joints to effectively inhibit the lateral actuation of the air pouch. Our

devised FLEXER addresses this necessity through a device architecture that encompasses (i) a CE that serves as an electric contact point, (ii) an anchoring frame (AF) that maintains the

shape of the FLEXER and provides the necessary mechanical constraint for actuation, and (iii) multiple semicircular legs (SLs) strategically positioned in an equiangular arrangement to link

the AF and the CE (Supplementary Figs. 8 and 9). As depicted in the top photographs in Fig. 2b, a three-legged FLEXER with a 10 cm AF diameter was fabricated to illustrate the design

approach. The AF is securely affixed to the fabric, serving as an integral mechanical anchor for the entire structure. The dimensions of the CE can be flexibly adjusted by either being

enlarged to enhance signal detection or reduced to minimize the overall size of the FLEXER. The SLs are linked to both the CE and AF through two pivotal joints. The first joint, which is

situated at the AF, dictates the rotational direction of the SLs while functioning as a stabilizer at the CE level. Similarly, the second joint, which is located at the CE, serves as an

electrode-level stabilizer, ensuring the stability of the entire system. When pneumatic pressure was applied, both joints unfolded, directing the CE vertically. While expansion, FLEXER’s

Joint 1 raised the SLs and CE by deflecting it from 0° to 42.2° (Fig. 2b, bottom right graph), and Joint 2 shifted the angle from 0° to 31.5°, ensuring parallel alignment between the CE and

AF planes for stable skin contact. The FLEXER also achieved a rapid actuation speed of ~12 cm/s by deploying the CE in <0.4 s (Fig. 2b, bottom left graph). This rapid actuation proves

advantageous in situations30 where users require prompt analysis of vital signals (e.g., ECG and EMG signals) related to urgent medical conditions, such as coronary heart disease,

cardiovascular disease, and congestive heart failure31,32,33,34. Furthermore, we assessed the contact stability of the FLEXER during its spring-like motion. The three-legged FLEXER was

attached to a linear actuator, and a cyclic linear motion with a 20 mm travel length was applied to simulate dynamic movement while measuring the contact force of the CE. As a comparative

measure, a balloon with the same diameter as the AF of the FLEXER was also tested (Fig. 2c and Supplementary Movies 3 and 4). The measured force was then differentiated with respect to time

to quantify the change in force over time. The result revealed that the three-legged FLEXER exhibited a consistent time derivative of force during repetitive movement, highlighting its

effectiveness in reducing motion-related interference during biosensing35. Contrastingly, the balloon displayed a standard deviation of the time derivative of force of 0.212 N/s, which is 80

times higher than that of the FLEXER (0.0026 N/s). This difference underscores the enhanced contact stability of the FLEXER in managing movement-related challenges during sensing

operations. Moreover, we evaluated the deviation of the CE from its center after the activation of FLEXER because MXene was coated on only one SL of the FLEXER, extending from the SL to the

AF as a conductive trace. Supplementary Figure 10 presents top-view images comparing the activation of MXene-coated and non-coated FLEXER samples. The CE diameter of the FLEXER is 10 mm, and

the center of the CE remained aligned with the inner contact area after activation. This demonstrates the consistent movement of the FLEXER system along with the electrode materials. To

expand the FLEXER into a wider range of wearable bioelectrodes, the contact force of the electrodes must be adjustable. This can be achieved by selecting an appropriate shape and number of

SLs. To evaluate the relationship between the FLEXER design parameters and the resulting contact force, a set of 16 distinct samples with varying SL widths and numbers were fabricated (Fig. 

2d, e). Since the AF remained mechanically fixed and the movement of the CE depended on the behavior of the SLs, the design parameters for the FLEXER were confined to the shape and number of

the SLs. The AF and CE diameters were maintained at 130 and 15 mm, respectively, while the pneumatic pressure was maintained at 5 psi to eliminate any additional control variable. Figure 2f

presents the recorded contact forces of the different SL widths and numbers for the FLEXER. The data demonstrate that the contact force increased as the number and width of the SLs

increased. This trend can be explained by the PIA mechanism, which establishes a connection between the output force and the volume of joint overlap. Regarding the FLEXER, the increase in

the number and width of its SLs directly contributes to the enlargement of the overlapping areas. This increase in overlapping areas leads to a heightened contact force. Eq. (1) can be used

to determine the contact force based on the two design parameters at a pneumatic pressure of 5 psi: $$F=0.25+0.35 * w+0.24 * n \, ({{{R}}}^{2}=0.97),$$ (1) where _F_ represents the contact

force, and _w_ and _n_ represent the width and number of the SLs, respectively. This empirical relationship is graphically illustrated in Fig. 2f. The contact force is expressed as follows

at high pneumatic pressures of 10 psi (Eq. (2)) and 15 psi (Eq. (3)) (Supplementary Fig. 11): $$F=0.26+0.33 * w+0.30 * n \, ({{{R}}}^{2}=0.93),$$ (2) $$F=0.28+0.32 * w+0.34 * n \,

({{{R}}}^{2}=0.90)$$ (3) Additionally, the maximum contact distance of the FLEXER electrode depends on the FLEXER size, as shown in Supplementary Fig. 12. When the AF diameter of the FLEXER

varied from 8 to 13 cm, the contact distance increased from 1.7 to 3.2 cm, all at a constant pressure of 10 psi. Considering both the magnitude and uniformity of the contact force is

essential for the FLEXER to effectively function as a bioelectrode in accurately detecting biological signals. To assess the impact of contact force uniformity based on the number of SLs,

the contact force of the CE was measured at various points using a 3 × 3 grid, as depicted in the schematic at the top-left corner of Fig. 2g. The contact force distributions of FLEXER

models with two, three, four, and five SLs were analyzed, as shown in Fig. 2g and Supplementary Fig. 13. Calculating the standard deviation for FLEXER models with different numbers of SLs

revealed the following trend: An increase in the number of SLs resulted in a more uniform distribution of contact force, as illustrated in Fig. 2h. CHEMICAL ANALYSIS OF MX-CNF-PCE ELECTRODES

MXene was used as the electrode material of the FLEXER because of its exceptional electrical conductivity and compatibility with water-based solution methods. However, MXene has poor

mechanical strength and experiences a reduction in electrical conductivity under ambient oxidation. To address these challenges, we incorporated PCE and CNF into the MXene solution to

enhance the solution properties. When combined with MXene, PCE effectively envelops the MXene surface, providing a protective shield against oxygen exposure. Moreover, this combination

enhances the flexibility of MXene by widening the gaps between its platelets. Conversely, CNF significantly increases the mesoscopic mechanical strength of the composite. Since MXene has a

platelet-like structure, the interconnection of individual MXene platelets through covalent bonds can result in poor mechanical strength. CNF serve as a platform for MXene attachment because

their dimensions (diameter: 3–30 nm and length: several microns) differ significantly from those of MXene (diameter: several microns and thickness: 1.2–1.8 nm36), facilitating the release

of strain within the composite structure. Supplementary Figure 14 provides a schematic representation of this composite, which encompasses both CNF and PCE elements. To realize this

approach, a water-based solution containing MXene, CNF, and PCE (MX-CNF-PCE) was prepared. This MX-CNF-PCE solution was then spray-coated onto the contact side of the FLEXER structure using

a polyethylene terephthalate (PET) shadow mask (Fig. 3a and Supplementary Fig. 15). The hydrophilic nature of the cotton fabric, the hydrophilic functional groups present on the MXene

nanosheets, and the hydroxyl groups within the CNF and PCE all enabled the solution to be adsorbed onto the fabric, resulting in the formation of densely packed MX-CNF-PCE layers. We

confirmed the uniformity and integrity of the MX-CNF-PCE spray-coating using scanning electron microscopy (SEM) and energy-dispersive X-ray (EDX) analysis37, as illustrated in Fig. 3b. The

top-view SEM image reveals that the MXene nanosheets enveloped the cotton fibers and bridged the gaps between them, while the unmodified cotton fabric exhibited a clean surface characterized

by interwoven warp and weft yarns (Supplementary Fig. 16). Additionally, the uniform distribution of each element within the MXene-based solution was observed from the EDX mapping (Fig. 3b

(right side) and Supplementary Fig. 17). Generally, electrodes must have low sheet resistance to be able to measure biosignals with high reliability. Here, the MX-CNF-PCE and MX-CNF

electrodes were measured to have sheet resistances of 24.7 Ω/☐ and 20.5 Ω/☐, respectively, which were slightly higher than that of the MXene electrode (19.1 Ω/☐) (Fig. 3c). This is

attributed to the inclusion of electrically nonconductive CNF and PCE within the MXene interlayers. However, their sheet resistances are still significantly lower than those of previously

reported MXene-coated cotton electrodes (569–761 Ω/☐)37. In addition to the sheet resistance of electrodes, the skin-to-electrode impedance is also a crucial factor. Skin-to-electrode

impedance reflects the skin’s resistance in transmitting electrical signals from the user to the sensing element of the electrode. Low skin-to-electrode impedance is associated with high

biosignal quality, as it signifies reduced resistance at the contact point between the skin and conductive surfaces38. Fig. 3d illustrates the measured skin-to-electrode contact impedances

of the FLEXER electrodes and reference dry and gel-type Ag/AgCl electrodes. The inflated FLEXER electrode displayed skin-to-electrode impedance comparable to those of reference electrodes of

the same size (diameter = 3 cm). Notably, the skin-to-electrode impedance of the FLEXER electrode was similar to that of the dry-type electrode, particularly up to a frequency of 2.45 kHz.

At a frequency of 100 Hz, the FLEXER electrode exhibited an impedance of 191 kΩ, while the dry and gel Ag/AgCl electrodes exhibited impedances of 190 kΩ and 64 kΩ, respectively39. These

impedance values are sufficiently low for accurate biosignal measurements without significant noise interference40. Further, we investigated the electromechanical responses of the MX-CNF-PCE

bioelectrode under mechanical deformation. A 15% tensile strain was applied to the three electrodes (MXene, MX-CNF, and MX-CNF-PCE), and the normalized resistance (R/R0) was measured, as

depicted in Fig. 3e. MX-CNF-PCE showed the best electromechanical stability with the smallest R/R0 increase of 2.1 at a 15% tensile strain, whereas MXene and MX-CNF exhibited R/R0 values of

4.8 and 3.2, respectively. The enhanced stability of MX-CNF-PCE is attributed to its unique brick-and-mortar architecture. In this structure, the 2D MXene nanosheets function as bricks,

while the 1D CNF serves as the mortar41. This is due to the formation of hydrogen bonds between the terminal groups (–OH, –O, and –F) of MXene and the hydroxyl groups of the CNF. The

incorporation of PCE, a comb-type polymer, into MX-CNF-PCE introduces additional hydrogen bonds, which significantly enhance its mechanical stability. Owing to these improvements, MX-CNF-PCE

exhibits a decrease in R/R0 in stark contrast to MX-CNF. Furthermore, we conducted a cyclic bending stability test by subjecting the three MXene-based electrodes to a 15% strain repeatedly

for 1000 cycles while measuring the R/R0 values, as depicted in Fig. 3f. This test simulates situations where stress is frequently applied to the bioelectrode on the fabric overlying

specific areas, such as joints like knees or elbows42. A consistent trend was observed throughout the test: The inclusion of CNF and PCE enhanced electromechanical stability. MX-CNF-PCE,

MX-CNF, and MXene had R/R0 values of 1.4–1.6, 2.3–2.6, and 6.1–16.9, respectively. For the oxidation resistance test, the MXene-based electrodes were exposed to a sealed glass chamber with

100% relative humidity for 17 days, as illustrated in Supplementary Fig. 18. The results of this rigorous environmental test revealed the remarkable oxidation stability of MX-CNF-PCE, as

evidenced by a modest increase in its R/R0 value from 1 to 65 (Fig. 3g). This marginal increase in R/R0 became apparent when compared to those of the MXene and MX-CNF electrodes43, which

experienced substantial increases to 1231 and 548 (20 times and 9 times that of MX-CNF-PCE), respectively. As mentioned earlier, this is attributed to the protective barrier formed by the

incorporation of PCE, which effectively shields MXene from oxidation. Sweat excreted by the skin can also affect the performance of bioelectrodes, thereby affecting their R/R0 ratio. To

assess the stability of MX-CNF-PCE in response to perspiration, its electrical characteristics were observed in an artificial sweat44. After wetting the three MXene-based electrodes with the

artificial sweat (see Supplementary Fig. 19), we monitored their electrical response (R/R0) for 20 minutes (Fig. 3h). MX-CNF-PCE exhibited the most electrically stable response because of

the PCE coating on the MXene nanosheets. Additionally, experiments were conducted to determine the optimal mixing ratio of MX-CNF-PCE for enhanced electromechanical properties by doubling

and halving the CNF and PCE amounts, as shown in Supplementary Fig. 20. Since CNF and PCE act as insulators for the electrode, their proportion needs to be minimized in comparison to MXene.

Considering the spray-coating capability and the electrical conductivity of the bioelectrode, we determined the optimized mass ratio of MXene to be 82 wt% of the total electrode composition.

Maintaining this MXene weight ratio (82 wt%), we precisely adjusted the amounts of CNF and PCE in the electrode to further improve its environmental stability. By comparing the

environmental stability of bioelectrodes with different CNF and PCE ratios, we identified the weight ratio of 24:4:1 (MXene:CNF:PCE) as optimal for the FLEXER system. Consequently, the

MX-CNF-PCE electrode demonstrated enhanced electromechanical and environmental resistance properties under various mechanical deformations, including tensile strain and cyclic bending, 100%

humidity environment, and interference from sweat. Spectroscopic characterization was performed on the MX-CNF-PCE electrode to understand the chemical structure underlying its improved

electromechanical test results (Fig. 3i‒k). The X-ray diffraction (XRD) curves in Fig. 3i and Supplementary Fig. 21 reveal evidence of the intercalation and blending of the CNF and PCE

within the MXene nanosheets. Specifically, the (002) diffraction peak for MXene appeared at 2θ = 5.82°, which shifted to 5.70° in MX-CNF and 4.66° in MX-CNF-PCE. These shifts correspond to

an increase in the interlayer spacing from 3.04 nm to 3.10 nm and 3.78 nm, respectively22,45,46,47. Fig. 3j presents the X-ray photoelectron spectroscopy (XPS) spectra of the pristine MXene,

MX-CNF, and MX-CNF-PCE composite films. An analysis of the Ti 2_p_ and O 1 _s_ spectra reveals that the area ratio of Ti2+ to Ti3+ peaks increased from 3.52 (MXene) to 3.56 and 3.85 (MX-CNF

and MX-CNF-PCE, respectively). Simultaneously, the area ratio of the –COO– peak to the total chemical bonds decreased from 0.04 (MXene) to 0.02 (MX-CNF and MX-CNF-PCE). These observations

confirm the formation of covalent Ti–O bonds between the MXene nanosheets and the PAA anchor of PCE, as revealed by the Ti 2_p_ spectrum (i.e., –COOH). Furthermore, the F 1 _s_ spectra

reveal the presence of hydrogen bonds between the MXene nanosheets and the hydroxyl groups in the CNF or the partially hydrolyzed –COO– of PCE (i.e., –COOH). The area ratio of the hydrogen

bond peak (C–Ti–Fx –H) to the total area increased from 0 (MXene) to 0.2 and 0.32 (MX-CNF and MX-CNF-PCE, respectively). The appearance of a high binding energy peak in the F 1 _s_ region

for C–Ti–Fx–H demonstrates the formation of hydrogen bonds, which contributed to MX-CNF and MX-CNF-PCE exhibiting better mechanical stability than pristine MXene. These ratio increments are

depicted in Fig. 3k. WIRELESS ELECTROPHYSIOLOGICAL MONITORING USING FLEXER To showcase the capabilities of the FLEXER in wearable biosensing, we developed a wireless electrophysiological

monitoring system. Figure 4a provides an overview of the working concept and block diagram of the developed system (see Supplementary Figs. 22 and 23 for more details). The FLEXER and the

flexible printed circuit board (fPCB) were electrically connected through jumper wires, allowing electrophysiological signals detected by the FLEXER to be routed to the biopotential

amplifier on the fPCB. These signals were then amplified and filtered by the biopotential amplifier before undergoing analog-to-digital conversion (ADC). The converted signals were

transmitted wirelessly to the computing unit in real time via a Bluetooth Low-Energy (BLE) module for further analysis. An ECG measurement was conducted with the developed wireless

electrophysiological monitoring system (Fig. 4b, see Supplementary Fig. 24 left for details). As a control group, ECG signals were also measured using commercially available gel-type and dry

Ag/AgCl electrodes with the developed wireless system. To record the ECG signals, two electrodes were placed on the left and right sides of the chest, and a ground electrode was placed on

the lower abdomen48. During the ECG recording, the FLEXER was affixed to the clothing, while both gel-type and dry Ag/AgCl electrodes were securely attached to the skin. Despite the gap

between the clothing and the skin, the FLEXER exhibited a high signal-to-noise ratio (SNR) because of its unique pneumatic structure, which facilitated effective skin-electrode contact (Fig.

 4c). Conversely, the FLEXER with low air pressure displayed a low SNR owing to inadequate skin-electrode contact. Consequently, the PQRST waveforms in the ECG recorded with the FLEXER

closely resembled those obtained using commercial Ag/AgCl gel electrodes (Supplementary Fig. 24 right). Moreover, the FLEXER demonstrated its efficacy in monitoring changes in heart rate via

ECG measurements performed before (72 BPM) and after (125 BPM) exercise, as shown in Fig. 4d, e. Unlike commercial Ag/AgCl gel electrodes, which necessitate continuous skin contact for

long-term monitoring, FLEXERs only make contact with the skin during measurements. This minimizes discomfort even during extended periods of use, which is crucial for ensuring user comfort

and compliance in continuous health monitoring scenarios. Supplementary Movie 5 shows emergent status of single-FLEXER and multi-FLEXER when pneumatic force is occurred which can contact to

skin with facile hand pumping. Real-time measurement of ECG using multi-FLEXER in situations involving standing, walking, and driving, both in the inactive and active status has been also

proceeded in Fig. 4f. During real-time ECG monitoring, signals were dramatically got stabilized after the activation of FLEXER. (Supplementary Movie 6) The FLEXER is also highly suitable for

capturing EMG signals, which are foundational for hand gesture recognition, because of its enhanced electrical conductivity and stable skin contact due to its pneumatic-based design. This

capability has profound implications in areas such as human-machine interfaces and particularly prosthesis control in healthcare45,46,49. Gesture recognition via the EMG process entails the

placement of multichannel electrodes on various areas of the arm, with recognition being facilitated by extracting EMG signal features using various classifiers (Fig. 5a)47. To demonstrate

this, EMG signals corresponding to eight distinct gestures were measured using FLEXERs positioned on the forearm, as depicted in Fig. 5b. The recorded EMG signals, captured across five

channels for each gesture, displayed distinct patterns among the gestures. The signals were then subjected to the continuous wavelet transform (CWT), which transformed them into scalograms,

i.e., image-like time-frequency representations. These scalograms served as inputs for a multi-input convolutional neural network (CNN)-based gesture recognition system50. For each gesture,

the scalograms derived from the five channels underwent independent processing through three convolution layers and one fully connected layer to extract unique features. These processed

outputs were then concatenated to create a comprehensive feature set for each gesture. This concatenated layer was subsequently linked to three additional fully connected layers to classify

the eight gestures (Fig. 5c). Further details can be found in Supplementary Table 1 and Supplementary Figs. 25 and 26. To evaluate the generalizability of the system across independent

datasets, five-fold cross-validation tests were performed on randomly mixed datasets. The high-dimensional features extracted from the multi-input CNN model were visualized using

t-distributed stochastic neighbor embedding (t-SNE). This visualization displayed a distinct separation of features, contributing significantly to the achievement of an accuracy rate of

97.92% in Fold 5 (Fig. 5d and Supplementary Fig. 27). The recognition accuracy using CNN model for all eight gestures in each fold is presented as a confusion matrix (Fig. 5e and

Supplementary Fig. 28). The average accuracy across the five-fold cross-validation tests was 95.94%. This high accuracy is mainly due to the aforementioned SNR of the FLEXER. Generally, EMG

signals can be used to assess grip strength15,51. Thus, a grip strength test was conducted by performing gripping actions at various force levels (Fig. 5f). During this procedure, a

dynamometer quantified the force level, and the corresponding EMG signals were recorded using the FLEXER on the flexor carpi radialis of the forearm (Supplementary Fig. 29). The recorded EMG

signals were then segmented into two-second time windows, and the root mean square (RMS) of the signals were calculated. As depicted in Fig. 5g, the RMS of the EMG signals exhibited a

corresponding increase with grip strength. DISCUSSION In conclusion, the development of FLEXER, a lightweight and flexible wearable bioelectrode with a pneumatic structure, represents a

significant advancement in real-time healthcare signaling technology for wearable devices. The incorporation of MXene-based dry electrodes allows the FLEXER to achieve exceptional electrical

conductivity and significantly reduce skin-to-electrode contact impedance, thereby addressing key challenges in biosensing applications. Moreover, the innovative design of the FLEXER

ensures consistent skin contact, enabling stable signal recording and accurate monitoring of physiological parameters. Comprehensive evaluations demonstrated the impressive electromechanical

properties of the FLEXER, which include exceptional mechanical stability, strain resistance of up to 15%, and remarkable durability over 1000 bending cycles. Additionally, the real-time

wireless electrophysiological monitoring system developed using the FLEXER enables seamless recording and transmission of ECG and EMG signals. Furthermore, the FLEXER demonstrates

exceptional accuracy in monitoring curved regions, with a recognition accuracy of 95.94% for hand gesture recognition using EMG signals. These significant advancements highlight the

potential of FLEXERs for personalized healthcare applications, such as prosthesis control and rehabilitation, and underscore their transformative impact on the field of wearable

bioelectrodes. METHODS FABRICATION OF FLEXER The FLEXER design was simplified using the visual programming software Rhino 7 and Grasshopper 3D (Supplementary Fig. 9). Two pieces of

TPU-laminated cotton fabric were overlapped, ensuring that the TPU layers came into direct contact. Hot sealing with a pen-type soldering tip was conducted along the designed pathway using a

customized commercial XY plotter (Liyang equipment), and the fabric was cut to the desired size using Cameo 4 pro (Silhouette). After preparing the pneumatic structure of the FLEXER, the

MX-CNF-PCE solution was spray-coated on it through a PET shadow mask to create a conductive path on the FLEXER. Pneumatic force was applied to the FLEXER through an air blower connected to

an airline. SYNTHESIS OF TI3C2TX MXENE AND MXENE-BASED ELECTRODES The etchant solution was prepared in a 250 mL Teflon beaker as follows: 3.2 g of LiF (99.9%; Sigma-Aldrich) was dissolved in

40 mL of a 9 M HCl aqueous solution and cooled to <5 °C using an ice-water bath. The etchant was then deoxygenated with ultrahigh-purity N2. Subsequently, 2.0 g of MAX phase (Ti3AlC2

powder, 99%, 325 mesh; Forsman) was gradually added to the etchant under gentle stirring. The mixture was deoxygenated again and protected in an inert atmosphere. Etching was performed in an

oil bath at 25 °C for 48 h to remove most of the Al layer from the MAX phase. The resulting product was washed and delaminated in two 50 mL centrifuge tubes using deoxygenated water and

then subjected to five to six cycles of centrifuge-shaking (Labogene 416, ONE Commercial shaker Horizontal Single Head Shaking Machine 220 V LJS80-1). Finally, the delaminated MXene was

sonicated in an ice bath for 30 min and centrifuged at 2826×_g_ for 30 min to obtain a supernatant predominantly composed of single-layer MXene. The MXene dispersion was mixed with a CNF

polymer aqueous solution (1 wt%; CNNT) and a PCE polymer aqueous solution (MW = 50 k, 55.0 wt%; L’BESTE GAT) according to the mass ratio specified in the experimental design (MXene:CNF:PCE =

 24:4:1, 24:2:1, 24:4:2, and 24:2:2). The mixture of MXene and polymers was vigorously shaken for 30 min to obtain a homogeneous MXene–polymer composite material. CHARACTERIZATION All video

analysis of the pneumatic structure of the FLEXER was performed using the Kinovea program. The contact force of the FLEXER was measured using a digital force gauge (ZTA-5N; IMADA) under

various pressure and FLEXER design conditions. The surface morphologies and elemental distribution of the MXene-based electrodes were characterized using SEM (JSM-7610F-Plus) and EDX

analyses. The sheet resistance was measured using the four-point probe method (Keithley 2182A, 2634B, and 6221). The skin-to-electrode impedance was measured using an

inductance–capacitance–resistance (LCR) meter (E-4980AL; KEYSIGHT) in the frequency range of 20 Hz to 300 kHz. Contact stability and tensile strain stability tests were conducted to evaluate

the mechanical robustness of the MXene-based electrodes on the FLEXER using a stepper motor controller (ECOPIA, BM-111). All electromechanical resistance data of the MXene-based electrode

were gathered using a parameter analyzer (4200A-SCS; Keithley). XRD (SmartLab; Rigaku) was used to detect the differences in the interlayer spacing of the MXene-based electrodes. An X-ray

photoelectron spectrometer (K-alpha, Thermo U.K.) was operated using an aluminum anode as the source with a spot size of 400 μm. WIRELESS ELECTROPHYSIOLOGICAL MONITORING An electrophysiology

amplifier (RHD 2132, Intan Technologies) with a 16-bit ADC and a differential gain of 192 was used to amplify, filter, and digitize electrophysiological signals. The sampling frequency was

258 Hz, and the bandpass filter frequency was 0.5–100 Hz. A BLE system on chip (QN9080SIP; NXP Semiconductors) wirelessly transmitted the data to a recording laptop for further analysis. The

entire system on the fPCB was powered by a 3.7 V lithium polymer battery and electrically connected to the FLEXER via jumper wires (AWG 30). REAL-TIME HEART RATE MEASUREMENT USING ECG The

ECG was measured by two electrodes placed on the chest and a ground electrode placed on the lower abdomen. In addition to the FLEXER, gel-type (Vitrode L-150X; Nihon Kohden) and dry (Laxtha)

Ag/AgCl electrodes were used for noise comparison of the signals. The Ag/AgCl dry electrodes were attached to the skin using medical tape (2702; 3 M). The commercial electrodes were

connected to the developed fPCB via snap connectors (Laxtha). The recorded ECG signals were transmitted wirelessly to the laptop through the BLE system on chip of the developed wireless

monitoring system. A fourth-order Butterworth band-pass filter (0.5–35 Hz) was used to denoise artifacts such as motion or power line artifacts. Subsequently, the R peak was detected to

calculate the heart rate in beats per minute. The SNR of a single PQRST wave in the ECG signals was calculated as follows: $${{{{{{\rm{SNR}}}}}}}_{{dB}}=20 \,{\log

}_{10}\frac{{A}_{{PQRST}}}{{A}_{{noise}}},$$ (4) where APQRST and Anoise are the amplitudes of the PQRST and noise, respectively. Thereafter, the SNR was averaged over the PQRST waves in the

recorded ECG signals. The signal processing was performed using MATLAB 2022b (MathWorks). The real-time ECG was measured with the subject standing, walking, and driving, in both the

inactive and active statuses of multi-FLEXER. GESTURE RECOGNITION AND GRIP STRENGTH TEST USING EMG For gesture recognition, five FLEXERs were placed on the forearm muscle. In addition, a

FLEXER was placed on the flexor carpi radialis for grip strength test. Both the ground and reference electrodes were positioned proximally to the elbow. Thereafter, the recorded EMG signals

were transmitted wirelessly to the laptop using the aforementioned system. Power line interference in the EMG signals was removed via a 60 Hz notch filter, and the signals were subsequently

filtered using the fourth-order Butterworth band-pass filter (10–80 Hz). Gesture recognition was conducted on 120 EMG signal datasets for each eight distinct gestures. In these datasets, the

signals were z-normalized and then segmented using a 4.5 s time window. Subsequently, scalograms were extracted through the CWT using the Morlet wavelet to provide image representations

that could serve as input for a multi-input CNN-based classifier. The scalogram image was then resized to 64 × 64 and normalized. The input size was set at 64 × 64 × 3 to account for the RGB

layers within each image. The architecture of the model comprised three convolution layers and one fully connected layer per channel, which were subsequently concatenated by a concatenation

layer. This concatenated layer was connected to three additional fully connected layers and was ultimately followed by a Softmax layer for the recognition of the eight gestures. A rectified

linear unit (ReLU) was selected as the activation function for the model. Meanwhile, the Adam optimizer (learning rate = 0.0001) was used as an optimizer, and loss consumption was performed

using the cross-entropy loss function. Five-fold cross-validation was performed for generalized performance. After training for the multi-input CNN for 100 epochs, the accuracy of the

five-fold cross-validation was averaged. The grip strength test was conducted using a dynamometer, with the volunteer maintaining a fixed elbow position. The dynamometer measured the maximum

force level as the volunteer applied various grip strengths with the right hand. EMG signals were simultaneously recorded by the FLEXER on the flexor carpi radialis. These EMG signals were

segmented using a 2 s time window to ensure that all grip-related signal variations were included. The RMS value of the segmented EMG signals was computed to establish a correlation between

the maximum force level and the RMS value derived from the grip-induced EMG signals. All signal processing was performed using MATLAB 2022b (MathWorks), and deep learning for gesture

recognition was performed using TensorFlow (Google). ETHICS INFORMATION FOR HUMAN SUBJECT RESEARCH The authors confirmed that under Article 13, Paragraph (1) of the Enforcement Rule of

Bioethics and Safety Act of the Ministry of Health and Welfare, Korea, Institutional Review Board approval was not needed as volunteers used wearable sensors with simple contact measurement.

In total of 2 participants were male and average age was 27 years old. The authors affirm that human research participants provided informed consents for publication of the images in Fig. 

4f and Supplementary Figs. 4, 25, and 29. STATISTICS AND REPRODUCIBILITY The SEM images in Fig. 3b and Supplementary Figs. 16 and 17 were tested with each three samples and five times

repeated for each sample to get similar results. REPORTING SUMMARY Further information on research design is available in the Nature Portfolio Reporting Summary linked to this article. DATA

AVAILABILITY All data supporting the findings of this study are available within the article and its supplementary files. Any additional requests for information can be directed to, and will

be fulfilled by, the corresponding authors. Source data are provided with this paper. CODE AVAILABILITY The custom codes used in this study for wireless electrophysiology monitoring and

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ACKNOWLEDGEMENTS This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korean government (MSIT) (No. RS-2023-00234581 and No. RS-2024-00415347) and

the Korea Medical Device Development Fund grant funded by the Korean government (the Ministry of Science and ICT, the Ministry of Trade, Industry and Energy, the Ministry of Health &

Welfare, and the Ministry of Food and Drug Safety) (Project Number: 1711174497, RS-2020-KD000093). AUTHOR INFORMATION Author notes * These authors contributed equally: Sanghyun Lee, Dong Hae

Ho, Janghwan Jekal. AUTHORS AND AFFILIATIONS * Department of Chemical and Biomolecular Engineering, Yonsei University, Seoul, Republic of Korea Sanghyun Lee, Soo Young Cho, Young Jin Choi 

& Jeong Ho Cho * Department of Energy Science and Engineering, Daegu Gyeongbuk Institute of Science and Technology (DGIST), Daegu, Republic of Korea Dong Hae Ho * Department of Robotics

and Mechatronics Engineering, Daegu Gyeongbuk Institute of Science and Technology (DGIST), Daegu, Republic of Korea Janghwan Jekal, Saehyuck Oh & Kyung-In Jang * Department of Mechanical

Science and Engineering, University of Illinois at Urbana−Champaign, Urbana, IL, USA Yoon Young Choi * School of Electrical and Electronic Engineering, Yonsei University, Seoul, Republic of

Korea Taeyoon Lee * Department of Bio and Brain Engineering, Korea Institute of Science and Technology (KIST), Seoul, Republic of Korea Taeyoon Lee Authors * Sanghyun Lee View author

publications You can also search for this author inPubMed Google Scholar * Dong Hae Ho View author publications You can also search for this author inPubMed Google Scholar * Janghwan Jekal

View author publications You can also search for this author inPubMed Google Scholar * Soo Young Cho View author publications You can also search for this author inPubMed Google Scholar *

Young Jin Choi View author publications You can also search for this author inPubMed Google Scholar * Saehyuck Oh View author publications You can also search for this author inPubMed Google

Scholar * Yoon Young Choi View author publications You can also search for this author inPubMed Google Scholar * Taeyoon Lee View author publications You can also search for this author

inPubMed Google Scholar * Kyung-In Jang View author publications You can also search for this author inPubMed Google Scholar * Jeong Ho Cho View author publications You can also search for

this author inPubMed Google Scholar CONTRIBUTIONS Conceptualization: S.L. and D.H.H. Experiment: S.L., D.H.H., and J.J. Methodology: S.L., D.H.H., and J.J. Main data analysis and manuscript

writing: S.L., D.H.H., and J.J. Assisted data analysis and manuscript writing: S.Y.C., Y.J.C., S.O., and Y.Y.C. Visualization: S.L., D.H.H., and J.J. Supervision: T.L., K.-I.J., and J.H.C.

All authors contributed to the writing of the manuscript. All authors have approved the final version of the manuscript. CORRESPONDING AUTHORS Correspondence to Kyung-In Jang or Jeong Ho

Cho. ETHICS DECLARATIONS COMPETING INTERESTS The authors declare no competing interests. ADDITIONAL INFORMATION PUBLISHER’S NOTE Springer Nature remains neutral with regard to jurisdictional

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