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AI-Enabled Flexible Sensing Skin for Next-Generation Aircraft: Toward Embodied Intelligence
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JingJing Ji1, 2, 3, YuXuan Pan1, 2, 3, ZhiHan Zhang1, 2, 3, Tian Xia1, 2, 3, Fan Zhang1, 2, 3, YongAn Huang1, 2, 3, *
Research. Vol 9 Article ID 1305
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Research. Vol 9 Article ID 1305
• REVIEW ARTICLE •
AI-Enabled Flexible Sensing Skin for Next-Generation Aircraft: Toward Embodied Intelligence
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JingJing Ji1, 2, 3, YuXuan Pan1, 2, 3, ZhiHan Zhang1, 2, 3, Tian Xia1, 2, 3, Fan Zhang1, 2, 3, YongAn Huang1, 2, 3, *
Affiliations
  • 1State Key Laboratory of Intelligent Manufacturing Equipment and Technology, Huazhong University of Science and Technology, Wuhan 430074, China.
  • 2Research Center for Advanced Electronics Manufacturing, School of Mechanical Science and Engineering, Huazhong University of Science and Technology, Wuhan 430074, China.
  • 3Flexible Electronics Research Center, Huazhong University of Science and Technology, Wuhan 430074, China.
Published: 2026-06-20 doi: 10.34133/research.1305
Outline
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Aircraft serve as the intelligent extension of human capabilities into 3-dimensional space. Next-generation aircraft will transcend the limitations of traditional fixed aerodynamic configurations, evolving into embodied intelligent agents capable of sensing their environment, making autonomous decisions, acting collaboratively, and self-evolving—ultimately achieving Fly-by-Feel. Flexible sensing skins, with their unique advantages (ultrathin, lightweight, large-area conformal attachment to the aircraft surface, and adaptive regulation), are emerging as the key enabling technologies. Multi-aerodynamic parameters are acquired through in situ sensing, and artificial intelligence (AI)-enhanced decision-making is implemented via edge-deployed chips. Based on this sensing–algorithm collaborative bridge, closed-loop actuation is further realized to support functional implementation. This paper reviews the core composition of the “sensing–decision–regulation” closed-loop system, including aerodynamic disturbance-free in situ sensing and AI-enhanced super-resolution field perception, and demonstrates its applications in 3 key scenarios: anti-icing/deicing, electromagnetic stealth, and lift enhancement/drag reduction. Finally, it highlights the future prospects of programmable intelligent flexible skins, promoting the aircraft’s paradigm shift toward intelligence, efficiency, and safety.

JingJing Ji, YuXuan Pan, ZhiHan Zhang, Tian Xia, Fan Zhang, YongAn Huang. AI-Enabled Flexible Sensing Skin for Next-Generation Aircraft: Toward Embodied Intelligence[J]. Research, 2026 , 9 (6) : 1305 - . DOI: 10.34133/research.1305
Future aircraft will evolve into a new generation of embodied intelligent aerial agents, capable of real-time perception of complex flight environments, autonomous decision-making for performance adjustment, and environmental self-adaptation [1,2]. Such evolving intelligence demands that the self-perception system deliver accurate, real-time structural and environmental data to underpin its autonomous learning and decision-making processes. Intelligent flexible sensing skin (iFlexSense) represents a revolutionary technological paradigm. Its core principle lies in integrating multiple flexible sensing and actuation units into an ultrathin substrate film conformally attached to aircraft surfaces, endowing conventional load-bearing structures with integrated functionalities of self-perception, data processing, and autonomous actuation [3]. Unlike conventional micro-electro-mechanical system (MEMS) that focus on single-point measurement, the iFlexSense can be deployed over large areas, even attached to thin-walled regions or internal flow channel areas. Owing to its ultrathin and lightweight nature, it imposes negligible modifications to the original aerodynamic contour when affixed to aircraft surfaces, thereby fully preserving the aircraft’s aerodynamic performance [4,5]. By integrating strain, pressure, shear stress, and other sensors, it acquires critical data regarding the aircraft’s structural state and ambient flow field, which serve as the core operational indicators for aircraft flight [6].
As the core intelligent module, artificial intelligence (AI) furnishes algorithmic support for the precise decision-making of iFlexSense systems [7], on the basis of super-resolution field reconstruction perception. Reconstruction algorithms essentially rely on discrete measurement point data collected by flexible skins, enabling accurate perception of distributed physical field information. Integral calculation of the reconstructed full-surface pressure distribution allows for real-time extraction of the aircraft’s lift and drag, which, in turn, empowers the flight control system to autonomously adjust flight states and realize safer, more energy-efficient flight strategies; precise reconstruction of the ambient flow field enables accurate identification of key flow phenomena including shock waves and boundary layer transition, offering a reliable decision-making basis for the early warning of hazardous flight conditions such as aircraft flutter and stall.
iFlexSense empowers the aircraft to become intelligent agents integrating sensing, perception, and actuation. Closely linked to aircraft flight safety, survivability, and core energy efficiency, anti-icing/deicing [8], electromagnetic stealth [9], and lift enhancement/drag reduction [10] stand as the 3 primary application scenarios for aircraft flexible smart skins. For aircraft anti-icing and deicing, mainstream current approaches predominantly depend on ground preventive protection and in-flight hot-air deicing. Flexible skins integrated with sensing capabilities enable active anti-icing/deicing through hydrophobic surfaces and heating interlayers; when coupled with neural networks (NNs), they deliver predictive support for deicing strategies, markedly boosting deicing efficiency and operational safety. In the domain of electromagnetic stealth, conventional coating-based stealth technologies are constrained by severe frequency-selective limitations. By harnessing electromagnetic metasurfaces and AI-driven adaptive frequency tuning functionalities, the iFlexSense system can realize full-band stealth coverage by regulating the geometric parameters (e.g., array spacing and dimension) of metallic microstructures. In contrast to the fixed aerodynamic configurations of contemporary aircraft, the iFlexSense system permits dynamic control of surface protrusions and even morphing wing structures, thereby optimizing the aircraft’s aerodynamic profile in real time during flight and improving aerodynamic efficiency. Although remarkable progress has been made in this research field, comprehensive and systematic review literature remains scarce.
Adopting the perception–decision–actuation collaborative closed loop as its core framework, this review systematically elaborates on the technological evolution and key breakthroughs of aircraft flexible smart skins in recent years. It further predicts that future flexible smart skins will fully break the design constraints of conventional aircraft that passively conform to aerodynamic environments, driving a paradigm shift toward aircraft that proactively sense airflow conditions and dynamically regulate surface properties. This will provide core impetus for the advancement of aerospace technology toward greater intelligence, efficiency, and safety, establishing it as a revolutionary enabling technology for the development of next-generation intelligent aerial vehicles.
iFlexSense is an integrated system. Built on flexible substrate materials (e.g., polyimide [PI] films) as its carrier, it integrates sensitive units such as pressure, strain, and temperature sensors onto the substrate via micro-nano fabrication technologies including magnetron sputtering and photolithography, forming a distributed sensing network. Such flexible substrates typically have a thickness of less than 100 μm, while the sensing units are generally fabricated at the submicron scale.
This ultrathin characteristic causes no damage to aircraft structures, nor does it alter their aerodynamic profiles, ensuring exceptional aerodynamic compatibility. However, accurately identifying flight states using limited sensing data remains a considerable challenge due to the strong nonlinearity of the surrounding aerodynamic field. AI-empowered iFlexSense, which integrates AI algorithms with its hardware platform, is the sole technical route capable of simultaneously satisfying the requirements of field perception, rapid decision-making, and adaptive regulation. The key merit of this technology lies in breaking through the constraints of traditional passive sensing, constructing a complete perception–decision–actuation closed loop, and realizing a genuine leap from simple data collection to active intelligent functionality.
Flexible electronic skins were initially applied in human wearable devices for monitoring physiological signals such as heart rate and body temperature [11]. Subsequently, it found application in industrial robotics for human–machine interaction monitoring [12]. For aircrafts, however, key measurement parameters focus on structural status and aerodynamic parameters. To accurately capture key signals including strain, vibration, and sudden changes in airflow distribution, sensor arrays must achieve micrometer-level spatial resolution and millisecond-level response speed (under high-speed maneuvering conditions, the single-frame response latency must be strictly controlled to ≤10 ms [13], while under flutter conditions, the response latency must meet the requirement of ≤5 ms [14]). To achieve this rapid response requirement, lightweight design is indeed a key technical pathway—among which model quantization and network pruning are the most mainstream lightweight technologies. Specifically, INT8 quantization reduces model volume by 75% [15], and network pruning cuts computational load by 40% to 55% [16], enabling efficient reduction of model size and computational overhead with minimal performance loss. The demanding environmental conditions in aerospace applications impose higher adaptability requirements on flexible skins [17,18]—ensuring no degradation of device performance over a wide temperature range (from low temperatures of −60 to −70 °C at high altitudes [19] to high temperatures of 1,100 °C near engines [20]). Under these thermal gradients and extreme high-altitude ultraviolet irradiation, the environmental adaptability of flexible substrates represents a critical technical challenge. Conventional PI meets general service requirements, yet in ultrahigh-temperature environments, flexible substrates such as microscale mica sheets are typically adopted to prevent brittle fracture and deformation [21]. In harsh high-altitude environments with intense ultraviolet irradiation and high-energy radiation, fluorine/boron-doped PI or PI aerogels can serve as reinforced substrates. The overall complexity during flight dictates the need for large-area measurement. However, achieving high-precision measurements across large areas remains challenging. The core innovation of iFlexSense lies in employing transfer printing technology to batch-transfer high-precision micro-sensor arrays, previously fabricated using techniques such as photolithography, onto large-area aircraft surfaces without damage [22]. To address the challenges of wiring and data busing in large-area high-density sensing arrays, direct printing techniques such as electrohydrodynamic jet printing are employed to integrally fabricate micro-interconnects on flexible skin surfaces (typical line widths: 3 to 5 μm, submicron thickness). Inspired by high-density super-resolution displays [23], a row–column matrix addressing combined with multichannel signal multiplexing architecture is utilized, enabling efficient signal acquisition for M×N-scale (thousands of) sensing nodes with merely M+N micro-interconnects. This design effectively eliminates wiring congestion while retaining the ultrathin and lightweight characteristics of the flexible skin.
Through core technological innovations such as micro-nano transfer and ultrathin fabrication [24,25], flexible skins have successfully addressed the dual challenges of high-precision, large-area measurement and harsh environment adaptation in aerospace scenarios. The massive data collected by these distributed sensor arrays require both millisecond-level local rapid processing during flight to ensure emergency response and in-depth mining and global analysis in ground-based R&D and full-life cycle management to support decision optimization—imposing differentiated adaptation requirements on the computing architecture for data processing. As a localized decision-making unit, edge intelligence represented by field-programmable gate arrays (FPGAs) adopts an end-to-end deployment scheme, and its operating environment constitutes a typical resource-constrained hardware scenario. Accordingly, such intelligent units take embedded lightweight models (e.g., multilayer perceptron [MLP] and convolutional neural network [CNN]) as their core, with a data processing capability of 106 to 1011 operations per second, a bandwidth demand ranging from 0.1 kbps to 1 Gbps, and a hardware power consumption of merely 1 mW to 100 W. Based on the above adaptive performance indicators, it can meet the latency requirements of 1 to 100 ms for core real-time scenarios [26,27]. On the other hand, in aircraft ground tests—including scenarios such as wind tunnel testing and full-life cycle health management—complex tasks like aerodynamic iterative optimization, historical flight data analysis, and integrated fleet operation data analysis inevitably generate massive data processing demands. This necessitates cloud intelligence as a supplement to edge intelligence [28]. Cloud intelligence relies on complex AI models such as variational autoencoders (VAEs) and transformers. Its data pattern processing capacity reaches the order of 1012 to 1018 operations per second, with a latency range of 100 ms to 5 s, typically requiring a bandwidth of 10 Gbps to 10 Tbps, a power consumption of 1 kW per single server, and a total power consumption of MW level for large-scale cloud data centers [29,30]. With its advantages in high computing power and large-scale data processing, it can simultaneously integrate multisource global information, providing a macro decision-making basis for aircraft R&D optimization, maintenance strategy formulation, and overall performance iteration.
Flexible skins achieve full-domain precise perception through high-precision sensor arrays, while the implementation of core functions such as real-time anti-icing/deicing, electromagnetic stealth, lift enhancement/drag reduction, and structural health monitoring (SHM) requires in-depth integration and adaptation of software and hardware. In the airborne application mode, at the system hardware level, chips such as FPGA suitable for extreme aerospace environments are selected as core processing units. The sensing signal acquisition module and data transmission module of flexible skins are integrated into standardized airborne boards, which transmit collected real-time data (e.g., flow field, strain, and vibration) to the airborne data processing unit or flight control system. Core algorithms—including dynamic ice thickness identification algorithm [31], electromagnetic scattering regulation algorithm [32], structural damage feature extraction algorithm [33], and real-time flow field analysis algorithm [34]—are solidified into the hardware logic units of FPGA chips to realize end-to-end closed-loop processing. In contrast, wind tunnel testing focuses on high-precision aerodynamic detection, long-term structural life cycle monitoring, and design iteration optimization, typically relying on large-scale data acquisition systems and cloud server computing [35]. A multichannel synchronous data acquisition system is built to complete synchronous collection of multidimensional parameters (e.g., structure, airflow, and environment). Data are uploaded to distributed server clusters in real time via dedicated transmission protocols to meet the requirements of massive data storage and high-intensity computing. The software leverages the server’s computing power for the rapid retrieval of historical data and multi-aircraft fleet test data, enabling in-depth comprehensive analysis. Additionally, a digital visualization interface is created to support retrospective comparison and horizontal analysis, facilitating full-life cycle SHM and assisting in the iterative optimization of aircraft design [36]. At this point, a complete AI-enhanced iFlexSense system architecture takes shape (Fig. 1).
The concept of “intelligent skin” was first proposed by the U.S. Air Force in 1985. Its original vision was to directly integrate functional modules into the airframe skin, thereby enabling the aircraft surface to serve as part of a distributed sensing and electronic warfare system [37]. The evolution from basic perception to intelligent skin systems can be broadly understood as a progressive transition from sensing to cognitive capability, divided into 5 stages (Fig. 2). Among them, Stages 1.0 to 3.0 mainly reflect the continuous evolution of sensing, progressing from in situ discrete sensing in Stage 1.0, to embedded sensor arrays in Stage 2.0, and finally to large-area integration and multimodal sensing in Stage 3.0, giving rise to adhesive thin-film iFlexSense. Stage 4.0 marks the extension of iFlexSense toward cognitive, where AI-driven technologies enable iFlexSense to evolve into an integrated sensing–computing system for local decision-making by near-sensor and in-sensor intelligence. Ultimately, in Stage 5.0, intelligent skin is envisioned to evolve into an embodied intelligent agent with a closed-loop perception–decision–actuation architecture, thereby realizing the paradigm of Fly-by-Feel.
Stage 1.0 was characterized by in situ sensing based on MEMS devices. In the 1990s, MEMS began to be integrated onto flexible substrates such as PI to measure surface shear stress, shock motion, and flow separation. The first flexible MEMS skin, developed at Caltech, adopted a silicon-island/PI interconnect architecture, enabling curved-surface attachment and dense sensor integration [38]. Subsequent work improved compatibility with microfabrication processes and enabled 3-dimensional (3D) transient shear-stress measurements in wind-tunnel environments [39]. NASA flight tests further demonstrated that PI-based hot-film arrays could capture shock-position variations during flight, while hybrid AeroMEMS arrays were capable of identifying near-wall separated flow [40]. Although this stage enabled conformal sensing on high-curvature surfaces, it remained limited by small coverage areas, insufficient interfacial reliability, and poor conformability to complex surfaces, allowing only single-parameter measurements.
Stage 2.0 marked the transition of sensing technology from localized measurement points to embedded sensor arrays along structural pathways, achieving distributed sensing. The representative technology of this stage was the fiber Bragg grating (FBG) sensor. Owing to its advantages of high sensitivity, immunity to electromagnetic interference, light weight, and multiplexed networking capability, FBG was widely applied in aerospace SHM and flight testing. By being embedded within composite structures, it enabled the formation of meter-scale sensing networks over wings, fuselages, and other components [41,42]. By integrating multiple gratings within a single optical fiber, multipoint strain and temperature measurements could be achieved [43]. This stage substantially expanded the sensing range and improved signal stability, allowing intelligent skin to further evolve into a distributed monitoring network linking aerodynamic shape with the state of load-bearing structures.
With advances in flexible electronics and materials science, Stage 3.0 achieved large-area integration and multimodal sensing, giving rise to adhesive thin-film iFlexSense meeting the demands for full-surface, multiparameter, and high-resolution measurements over complex aerodynamic structures. The introduction of novel functional materials, including conductive polymers, liquid metals, and 2-dimensional (2D) materials, endowed sensors with bendability, stretchability, and self-healing capability while maintaining excellent electrical performance [44,45]. Meanwhile, structural designs based on serpentine or fractal interconnects, stretchable conductive composite networks, and programmable array layouts tightly integrated sensors, signal acquisition circuits, and flexible printed circuit boards into networked topologies. These not only ensured the local independence of individual sensing nodes but also enabled global information fusion, thereby supporting real-time aerodynamic state monitoring and structural health assessment [46,47]. Under wind-tunnel and flight conditions, such flexible electronic skins enabled high-resolution pressure and strain measurements on unmanned aerial vehicle (UAV) wings or other complex surfaces, and could reconstruct the global aerodynamic field through networked nodes, thus realizing the transition from single-point measurement to full-surface, multiparameter integrated sensing [48].
Entering the 2020s, as full-surface and multiparameter sensing architectures gradually matured, intelligent skin systems were increasingly required to extract flight-relevant key information from massive heterogeneous sensor data in real time. Constrained by bandwidth, latency, and power consumption, traditional approaches relying on external centralized processing became increasingly inadequate. This drove iFlexSense beyond enhanced sensing toward an AI-enabled stage of cognitive enhancement, namely, Stage 4.0, becoming an integrated sensing–computing system. At this stage, machine learning can be used to identify critical states such as flow separation, stall, and flutter [3], and can also reconstruct full-field pressure distributions from limited sensing points [49]. The coupling of AI and materials further shortened the conventional chain of “sensing–sampling–transmission–computation”. In this context, the 2 complementary pathways of intelligent metamaterials and metamaterials intelligence, corresponding respectively to AI for materials and materials for AI, embed part of the sensing and computing burden directly into the material and structural design itself [50]. Through such lightweight deployment, intelligent skin acquires perception–decision capability and evolves from a passive data acquisition unit into a distributed information node capable of anomaly identification, state estimation, and local decision support.
With continued advances in flexible multimodal sensing, embedded AI, and miniaturized actuation, intelligent skin is expected to evolve into Stage 5.0—an embodied intelligent agent. In this stage, materials, structures, sensing, computing, and actuation converge into a closed-loop “perception–decision–actuation” system. Under the Fly-by-Feel paradigm, the aircraft surface transforms from a passive sensing interface into an active participant in flight perception and adaptive regulation [51]. Existing studies have combined feather-piezoelectric mechanoreceptors and deep learning to achieve real-time perception of flight parameters [52], allowing AI to perceive physical fields through material responses. For sensor hardware design, AI can enhance the sensitivity, conformability, and environmental adaptability of flexible skin by optimizing the composition and proportion of tunable materials and regulating surface microstructural units [53]. For intelligent information processing, lightweight in situ deployment is also a critical step to realize the deep integration of AI at the material level and establish a fully embodied intelligent agent. Lightweight AI algorithms are directly deployed on flexible sensing hardware through model compression, hyperdimensional computing, and other technologies, enabling flexible electronic skin to act as an embodied intelligent terminal with real-time local intelligent response [54]. Ultimately, intelligent skin will become an embodied intelligent node featuring endogenous physical intelligence, networked collaboration, and continuous evolutionary potential [55].
The sensing requirements for aircraft flexible skins closely revolve around 2 core objectives: flight safety assurance and aerodynamic performance optimization. As the skin interacts directly with airflow, it is necessary to real-time acquire the aerodynamic loads generated by the surrounding flow field—including the normal pressure (which affects lift) and the shear force (which is associated with drag and control stability). In terms of structural safety, the skin endures airflow impact, vibration fatigue, and temperature changes over the long term, making it prone to micro-crack initiation, propagation, or material performance degradation. Therefore, it is essential to accurately capture parameters such as the structural strain distribution, vibration frequency, and amplitude. To meet these measurement requirements, functional sensors are deployed in a targeted manner: pressure sensors are used to obtain normal aerodynamic pressure for lift inversion; shear force sensors directly detect the tangential force of airflow; strain sensors monitor structural deformation; and vibration sensors capture dynamic mechanical responses. By integrating micro-sensor arrays with excellent independent detection capabilities onto the flexible skin substrate, and relying on the collaborative arrangement of multitype sensing units, the flexible sensing skin enables simultaneous detection of multiple physical quantities.
The measurement of pressure distribution on the aircraft wing surface is the basis for obtaining lift, which is the core factor for ensuring flight safety and optimizing aerodynamic performance. According to Bernoulli’s principle, lift is essentially the cumulative effect of the pressure difference between the upper and lower surfaces of the wing [56], and it can be obtained by integrating the pressure over the wing surface (Fig. 3A)—this is also the fundamental reason why large-area pressure measurement is required. Furthermore, abrupt pressure changes are also “direct signals” for capturing key aerodynamic phenomena such as shock wave positions and flow separation, which is highly related with stall risk [57]. Measuring the surface pressure of an aircraft wing requires balancing multiple metrics: the sensitivity must be sufficient to capture subtle pressure changes for identifying airflow anomalies; the measurement range should cover the positive–negative pressure difference range while ensuring rapid dynamic response to track transient pressure; additionally, it must meet the requirements of environmental stability and miniaturized installation.
Compared with traditional sensing technologies such as pressure scanning valves [58], MEMS chips [59], and fiber optic sensors, the ultrathin flexible intelligent skin with the advantages of surface fit and aerodynamic compatibility shows great application prospects, avoiding the interference of sensor installation on the airflow field from the root, and adapting to the limited installation space on the wing surface [48] (Fig. 3B). The core sensing mechanisms of pressure sensors are mainly divided into 2 categories: resistive and capacitive sensing. Resistive sensors are based on the piezoresistive effect. Pressure-induced deformation of the sensitive layer changes the connectivity of its internal conductive paths, thereby causing a substantial change in resistance [60] (Fig. 3C). Such sensors have simple manufacturing process and low cost. Capacitive sensors, on the other hand, center on a capacitive structure composed of flexible electrodes and a dielectric layer. External wind pressure causes telescopic deformation of the dielectric layer, leading to regular fluctuations in capacitance [61] (Fig. 3D). Their advantages include fast response speed and excellent temperature stability, making them suitable for real-time monitoring of dynamic aerodynamic pressure and thus more favored in wing surface pressure measurement.
Research on substrate membranes and sensitive cell materials constitutes a pathway toward achieving superior sensor performance [62,63]. PI has been widely used due to its excellent mechanical properties and thickness-tunable fabrication techniques [64] (Fig. 3E). To address the measurement of both positive and negative pressures, the cavity structure has emerged as an effective solution. The cavity structure allows pressure differences to induce changes in the distance between 2 electrodes, thereby leading to capacitance variations [65]. Breakthroughs in precision machining processes such as laser etching and lithography have promoted the rapid development of higher-density, finer-structured sensor array fabrication technologies [66]. Xiong et al. [48] pioneered a programmable capacitive pressure sensor based on a PI substrate and a microcavity structure, with a thickness of only 70 μm and a high sensitivity of 0.28 kPa−1 within the range of 0 to 3 kPa. To enhance sensitivity, researchers have fabricated sensors by combining flexible substrates with abundant surface functional groups and conductive materials [60]. Notably, improving the dielectric constant is also a crucial means to boost the sensitivity of capacitive sensors. By integrating graphene fibers into fabrics, Javed et al. [67] developed sensors with layered conductivity, substantially enhancing sensitivity. With the advent of the electric double-layer principle, ionic liquid-based capacitive sensors have garnered widespread attention from researchers [68,69]. These sensors can not only detect subtle changes in the pressure layer induced by airflow separation via a high-sensitivity sensing chip, but also cover both positive and negative pressure ranges. Wang et al. [61] reported an ionic gel-based capacitive pressure sensor with an ultrawide sensing range (–100 to 600 kPa) and a high-frequency response of 400 Hz (Fig. 3G). Nonnegligible interference from temperature variations affects the testing performance of most industrial wind tunnels. To solve this issue, Li et al. [70] proposed a differential cavity structure, which eliminates crosstalk caused by temperature changes (Fig. 3F). The performance metrics of flexible skins under normal pressure are summarized in Table 1.
At present, the key challenge to be addressed for capacitive pressure sensors is the sampling frequency to cope with high-frequency pulsating signals. Future flexible skins will develop toward the direction of “larger size, thinner thickness, and higher precision”, enabling the detection of airflow separation during high-angle-of-attack flight.
Normal pressure is directly related to aircraft lift, while tangential shear stress directly reflects the magnitude of wall friction drag on the wing surface, which is another core object of aircraft monitoring. The fundamental cause of aircraft wall friction drag is the interaction between air viscosity and the aircraft surface [71]. This adhesion effect makes the boundary layer form an obvious velocity layer, and the viscous shear between air molecules, air flow, and the fuselage surface produces shear stress (Fig. 4A). According to Kolmogorov’s turbulent statistical theory [72], in the aerodynamic turbulent boundary layer, the size of the smallest vortices is approximately 10 to 100 μm, and the formation and dissipation time of these small vortices is only 0.1 to 1 ms. It is enough to prove that the shear stress has the characteristics of small numerical value, high dynamics and small characteristic scale of the flow structure. Therefore, in recent years, the wall shear stress sensor has been improved in terms of ultrathinning, high sensitivity, and high reliability.
The wall shear stress measurement technology mainly uses the traditional floating MEMS shear stress sensor [73], oil film method [74], hot wire anemometer [75], etc. As a modern technology for wall shear stress measurement, the flexible hot-film sensor is essentially a flexible electronic sensing thin-film element that works based on the self-heating effect. It first attains a stable thermal state via self-heating, then establishes the correlation between wall shear stress and its temperature through forced convective heat transfer [76]. Featuring a typical thickness of less than 100 μm, the flexible thermal sensor is suitable for direct attachment to aircraft wings, enabling wall shear stress measurement [77] and adaptive performance characterization in extreme operating environments (e.g., subsonic flow fields) [78] (Fig. 4B and C).
Research in the field of flexible hot-film sensors in aerospace primarily focuses on the development of high-performance flexible substrate materials and the optimization of micro-nano structures. Song et al. [79] prepared a suspended ultrathin flexible hot-film sensor with a thickness of only 6 μm, a sensitivity of 1.99 V2/Pa1/3, and a fast response characteristic of 1.2 ms (Fig. 4D). Also focusing on suspended structures, Gong et al. [80] designed a flexible calorimetric flow sensor based on a high-sensitivity vanadium oxide thermistor with an unprecedented speed resolution of 0.11 mm/s (Fig. 4E). Pang et al. [81] developed a 2-layer hot-film sensor, which improved its sensitivity by approximately 150% through reducing heat conduction (Fig. 4G). To meet the multiparameter measurement requirements of complex scenarios, they further developed an integrated sensor for shear stress, flow direction, and dynamic pressure on this basis [82]. This integrated sensor can measure wall shear stress in the range of 0 to 17 Pa with a measurement error of less than 0.4 Pa and a directional error of less than 3°. In addition to structural optimization, the regulation of the key performance of the sensor by the fabrication process is also crucial (Fig. 4F). Sun et al. [83] investigated the effects of annealing temperature and duration on the temperature coefficient of resistance (TCR), fabricated a flexible hot-film sensor with a TCR of 5,100 ppm/°C, and further studied the flow transition and separation characteristics of the NACA 0012 airfoil under various operating conditions (Fig. 4H). The performance metrics of flexible skins under shear stress are summarized in Table 2.
The flexible hot-film sensor is developing rapidly, which has the characteristics of good surface conformality, high sensitivity, and fast response time. However, heat loss control and dynamic calibration remain 2 major challenges that need to be addressed. Future development will continue to focus on material innovation, structural optimization, and other directions, gradually realizing the leap from laboratory research to engineering applications.
Aircrafts inevitably face deformation, fatigue, corrosion, and other losses during long-term flight, and monitoring the structural safety of the aircraft itself is a “bottom line requirement” for aviation safety. If structural hazards such as stress concentration and stiffness reduction occur, catastrophic accidents such as wing breakage and fuselage disintegration may occur in severe cases. Strain sensing and vibration sensing are key monitoring tools for identifying health hazards in aircraft structures [84]. Strain refers to the micro-deformation of a structure after being loaded, and it has a linear relationship with stress. Strain sensors can directly and quantitatively reflect the stress state of the structure—determining the presence of stress concentrations or predicting the initiation of fatigue cracks [85]. Structural stiffness directly dictates natural vibration characteristics. By tracking the dynamic characteristics of the loaded structure in real time, vibration sensors can rapidly detect stiffness degradation signals [86]. These 2 technologies convert invisible structural problems into quantifiable monitoring data, thereby enabling early warning of potential hazards. As more advanced morphing wing technologies continue to develop [87], the dynamic deformation characteristics of structures will become more complex. Flexible sensors that can fit complex structures greatly enhance the comprehensiveness and adaptability of monitoring (Fig. 5A).
The identification of stress concentration relies on tiny strain differences, which imposes strict demands on the sensor’s thickness [88], accuracy [89], and sensitivity [90]. Various research and breakthroughs were conducted, as shown in Fig. 5 (lower left). Yu et al. [91] proposed a laser-induced interface ablation method to fabricate ultrathin graphene-polyimide strain sensors, which measure only 8 μm thick—6 times thinner than those fabricated via traditional surface ablation methods. Guo et al. [92] developed a double-sided flexible sensing skin integrated with in situ self-compensation. The sensor achieves a strain linearity of 99.98%, making it suitable for multimodal measurement of morphing aircraft wings (Fig. 5B). The S4 method proposed by Meng et al. [93] obviates the trade-off between spatial resolution and strain resolution, allowing for more accurate detection of regions with steep strain gradients, such as edges and sharp corners. When an aircraft operates from ground level to high altitudes and from tropical to frigid regions, strain sensors must additionally exhibit full environmental tolerance [94]. Wang et al. [95] fabricated MoxW1−xS2 alloy flexible strain sensors via direct pulsed laser. These sensors have a detection limit as low as 4.9 με and can operate stably at a high temperature of 500 °C (Fig. 5C). In contrast, the flexible strain sensor based on a MoWNb medium-entropy alloy coating, developed by Li’s et al. [21], boasts an even lower detection limit of 0.57 με and operates over a wide temperature range from −150 to 1,100 °C (Fig. 5D). The performance metrics of flexible skins under strain are summarized in Table 3.
In response to the needs of aircraft structural vibration measurement, several research teams have also made innovative attempts, as shown in Fig. 5 (lower right). Early structural hazards only induce subtle vibration signal changes. Sensors require high sensitivity and low noise to distinguish normal fluctuations from early anomalies. Langat et al. [96] adopted the lamination and curing molding process to fully embed piezoelectric sensors into composite laminates, which can effectively avoid the masking of damage characteristics by environmental noise and obtain structural monitoring data with distinct dynamic features. Chen et al. [97] created a suspended-film flexible vibration sensor based on channel crack design. It demonstrates high sensitivity, good reproducibility, and robust sensing stability, and can achieve an ultrawide frequency vibration response range of 0.1 to 20,000 Hz (Fig. 5E). In some special parts of aircraft (e.g., high-temperature areas like engines), sensors are required to have high-temperature stability [20]. Hu et al. [98] proposed a self-powered piezoelectric vibration sensor based on PVDF-PI nanofiber membrane, which only suffers 15% performance loss at 80 °C (Fig. 5F). It is worth mentioning that in terms of functional integration, Chao et al. [99] achieved performance upgrades through the integration of biomimetic structures and metamaterials, and designed a self-powered biomimetic twisted hyperbolic metamaterial-integrated triboelectric nanogenerator sensor [100]. Weighing merely 10 g and with a 36-ms response time, it can perform self-powered monitoring of impacts within 1,000 N and UAV localization, achieving a balance of light weight, multifunctionality, and self-sustainability (Fig. 5G). The performance metrics of flexible skins under vibration are summarized in Table 4.
As the aviation industry demands more refined and intelligent structural safety monitoring, large-scale application of flexible vibration and strain sensors in aircraft has become inevitable. This will provide core technical support for full-life cycle aircraft health management.
The Fly-by-Feel flexible intelligent aircraft relies on flexible sensors to achieve proximal sensing of its flight status. However, sensor hardware alone cannot directly identify the structural health status or flow field evolution laws behind the data. AI algorithms are required to enhance perception capabilities and realize the conversion of “data–information–decision”, so that the flexible intelligent skin is not just “sensing” but “perception”. This section will elaborate on the discussion from 2 aspects: the structure itself and the surrounding aerodynamic field. Regarding fatigue damage and crack propagation induced by the complex operating conditions of the aircraft structure during long-term operation, AI technology can filter out noise, identify early-stage weak damage features, and predict damage evolution trends to generate maintenance decisions. On the other hand, in the study of the aircraft surrounding flow field, flow field reconstruction technology is crucial for obtaining a complete flow field state—by integrating advanced algorithms, it can inversely calculate the full-field flow distribution from discrete iFlexSense measurement points, providing a solid basis for optimizing aircraft aerodynamic performance and controlling flight attitudes.
The essence of aircraft SHM is monitoring all damages that may affect structural integrity and service safety [101]. As mentioned in the previous section, sensors can only output raw physical signals such as strain and vibration, which cannot be directly mapped to core SHM requirements—including “whether the structure has damage, where the damage is located, and how severe the damage is”. Reliance on algorithms for signal interpretation and information processing is essential in the process from simple data collection to flight health assessment. Achieving the dual value of flight safety assurance and operation and maintenance (O&M) efficiency optimization is the core goal of aircraft SHM. Its implementation path is divided into 2 core directions: real-time damage state monitoring based on iFlexSense and systematic health management for the entire life cycle (Fig. 6A). These 2 directions form a collaborative closed loop of edge intelligence and cloud-based O&M, jointly constructing a full-chain health assurance system for aircraft.
Among them, real-time damage state monitoring takes the flexible intelligent skin as a carrier, capturing abnormal signals such as strain and vibration [102,103]. However, flexible sensors can only be deployed at limited discrete locations. For damage localization in uncovered areas, it is necessary to rely on algorithms to infer the global structural state from local sensing signals. This task falls under the supervised learning framework for classification tasks, focusing on rapid identification of equipment current states from distributed local sensing signals—addressed by lightweight node-based NNs. Zhu et al. [104] propose a large-area monitoring technology combining flexible micro piezoelectric sensor arrays and machine learning algorithms. It adopts the MUSIC-aided back propagation neural network (BPNN) algorithm to realize adaptive learning and prediction of impact location, and the accuracy rate of impact location reaches more than 90% (Fig. 6B). The MUSIC-aided BPNN is essentially a shallow feedforward NN based on MLP. It can efficiently establish the nonlinear mapping between multisensor inputs and state outputs, without relying on the complex automatic feature learning mechanism of deep NNs. The primary goal of the real-time health monitoring module is damage detection and localization. Del Priore and Lampani [105] designed 2 types of graph neural network (GNN) architectures that optimize feature processing logic for spatial structural damage localization, adapting to the spatial topological characteristics of aircraft structures (binary damage detection + spatial probability distribution localization), achieving a localization error of only 3% of the wingspan (Fig. 6C). Zheng et al. [106] used the improved Fisher Discriminative Dictionary Learning method, which can identify loads at 8 corrugated crests with only 2 FBG sensors, achieving 100% localization accuracy. After damage detection and localization, it is necessary to evaluate the severity of damage. Pagani et al. [107] proposed a damage detection method based on artificial neural networks (ANNs). Its core network employs a single-hidden-layer architecture to avoid redundant computations. Using modal parameters as inputs and leveraging the nonlinear mapping capability of MLPs, it efficiently establishes the mapping between feature inputs and structural damage location/severity, enabling accurate detection of damage in each structural component (Fig. 6D). It is worth noting that signals measured by sensors are the superposition of structural vibration, environmental interference, and operational noise. Among them, the amplitude of environmental interference and operational noise is often 10 to 100 times that of damage signals [108]. Thus, algorithms are essential for interference compensation and damage signal extraction. Furthermore, the power consumption in the airborne situation is always an important point. Wang et al. [109] have developed a miniature ultralow-power wireless multiparameter monitoring system suitable for aircraft smart skin, with an average power consumption of as low as 7.59 mW/m2 (1 to 3 orders of magnitude lower than traditional systems). In addition, spiking neural networks (SNNs), as the latest generation of AI, employ a unique event-driven mechanism based on the “wake-on-demand” principle rather than continuous monitoring. Specifically optimized for airborne ultralow-power consumption requirements [110], SNNs substantially lower the power consumption of flight systems, providing technology for the improvement of the endurance of mainstream aircraft and the landing of new energy aircraft.
Cloud-based intelligence compensates for a critical conflict in real-time damage monitoring—sacrificing computational scale for rapid response—providing a solution for scenarios requiring massive computing power such as long-term optimized O&M and life cycle management of aircraft [111]. Most life cycle health management tasks belong to regression tasks in supervised learning (e.g., remaining useful life [RUL] prediction), while semisupervised or unsupervised learning paradigms are adopted for extreme scenarios lacking prior data. Characterized by reliance on large-scale long-time series historical monitoring data, these tasks require network architectures with capabilities of long-term temporal dependency capture, deep feature mining, and global pattern fitting. Wang et al. [112] proposed a self-supervised learning foundation model (BasGPT). This model leverages deep feature extraction and multidimensional data fusion to perform full-life cycle diagnostics for cross-type bleed air systems. It addresses the challenges of data scarcity for new aircraft types (e.g., C919) and poor cross-type compatibility, enabling the transfer of diagnostic knowledge from mature aircraft types to new ones (Fig. 6E). Predicting the RUL of structural components using historical data is a critical module in long-term aircraft monitoring and predictive maintenance [113]. Leveraging large-scale server clusters and distributed computing architectures, flexible smart skins not only receive and transmit real-time data but also integrate historical flight parameters, maintenance records, and material fatigue test data. This breaks through the storage and computing power limitations of airborne embedded systems, avoiding problems such as low RUL prediction accuracy and simplistic O&M schemes caused by insufficient local computational scale. Dagal et al. [114] integrate ANN with failure mode and effects criticality analysis (FMECA). By combining the nonlinear fitting capability of ANNs and the systematic risk analysis framework of FMECA, they compensated for the poor interpretability of stand-alone NNs, while using engine sensor data (e.g., temperature, pressure, and vibration) to predict failure probability, maintenance duration, and costs (Fig. 6F). Li et al. [115] developed a probabilistic individual aircraft tracking model based on dynamic Bayesian networks, which captures the temporal evolution patterns of structural damage via probabilistic modeling. It is capable of predicting crack lengths over the next 10,000 cycles in the width of the 95% confidence interval, realizing crack evolution tracking and RUL prediction. Supported by the powerful computing power of the cloud, multitype aircraft data collaboration and algorithm iteration enable the construction of more universal and accurate health management models. For example, based on federated learning technology, while protecting the data privacy of each airline, damage data of smart skins from different aircraft types can be aggregated to optimize the generalization ability of RUL prediction algorithms [116]. This results in a 15% to 20% reduction in prediction errors compared to a single airborne model, while improving prediction stability by more than 25% under different operating conditions [117,118]. Raouf et al. [119] achieved landing gear fault diagnosis and RUL prediction based on multi-AI technologies, covering fault detection and isolation, RUL prediction, and maintenance decision-making, realizing full-life cycle health management (Fig. 6G). Basora et al. [120] proposed a semisupervised anomaly detection framework. Utilizing a semisupervised learning paradigm to extract implicit degradation features from unlabeled data, this method resolves the issue of anomaly identification in data-scarce scenarios. It addresses the key challenge of limited fault samples in the full-life cycle health monitoring of aircraft fleet cooling units, reducing the overall fleet maintenance cost by 15%. In addition, linking the health assessment results output by the model with the airline’s O&M system can generate globally optimal maintenance plans by integrating flight scheduling data, ensuring flight safety while minimizing O&M costs to the greatest extent [121]. A comparison of typical models for different detection tasks is presented in Table 5.
Aircraft operate in complex flow field environments, and the flow state of wing surrounding flow is a core factor determining aircraft flight safety and aerodynamic lift-drag characteristics. It is particularly crucial to accurately acquire the distribution of key physical parameters on the wing surface and the spatiotemporal evolution characteristics of the surrounding flow field. However, the flow field around the wing features highly nonlinear and strongly coupled complex evolution characteristics [122,123]. Constrained by the spatial resolution of existing measurement methods, full-scale, high-resolution direct observation is nearly unachievable in wing-related scenarios. Accordingly, the importance of flow field reconstruction technology has become increasingly prominent. This technology can recover global flow field information based on limited discrete measurement point data [124,125] (Fig. 7A), resolving the core contradiction between limited observation and full-field analysis requirements, and is an inevitable choice to connect experimental data, numerical simulation, and engineering applications.
The evolution of flow field reconstruction methods for wing surfaces is closely intertwined with the growing demand for “accuracy–efficiency” in aerospace engineering. Methods for reconstructing aircraft wing surface flow fields from sparse points are generally categorized into 2 types: data assimilation (DA) and data-driven methods. DA methods, centered on strong physical constraints, integrate sparse observations with aerodynamic control equations to ensure the physical consistency of flow field reconstruction [126]. They effectively avoid pronounced errors of early physics-unconstrained methods in high-gradient regions such as wing leading-edge shocks and trailing-edge separation vortices, thus becoming the core technical pathway for high-precision scenarios like airworthiness certification and hypersonic flight. These methods are based on aerodynamic control equations and integrate sparse observation data via DA techniques [127], with the Ensemble Kalman Filter and variational assimilation as typical representatives. Li et al. [128] proposed a sparse sensor-assisted fractional generative model that reliably reconstructs the spatiotemporal field in unobserved regions using only 1% sparse flow field data, even at high noise levels (Fig. 7B). To further balance the accuracy and efficiency of DA techniques, He and Liu [129] proposed the LSE (linear stochastic estimation) + continuous adjoint DA strategy, effectively expanding the application scenarios of DA. In addition, Buchta et al. [130] applied nonlinear variational DA at Mach 6 to estimate the unknown flow field over an elongated cone from discrete wall pressure measurements (Fig. 7C). Shu et al. [131] proposed a “Denoising Diffusion Probabilistic Model + Partial Differential Equation residual layer constraint” framework for high-fidelity data reconstruction, reinforcing DA’s core advantage in physical constraints. However, DA methods suffer from notable limitations: as they require solving large-scale linear or nonlinear equations derived from control equations, calculating a single flow field typically takes hours or even days, resulting in a substantial mismatch with scenarios demanding high real-time response speeds.
Data-driven approaches, with NNs as their core, can be mainly categorized into 2 types: pure data-driven models and physics-informed learning frameworks. When applied to flow field reconstruction, physics-informed neural networks (PINNs) exhibit distinct characteristics and performance compared with pure data-driven networks, and their respective advantages and limitations are complementary. PINNs exhibit superior generalization ability and robustness, with strong resistance to noisy data, while inherently featuring physical consistency and interpretability. Nevertheless, their fitting accuracy deteriorates notably in reconstructing flow fields with high Reynolds numbers and strong nonlinear turbulence. Especially in large spatiotemporal domain flow field reconstruction, the training procedure becomes complicated and computationally time-consuming. By constructing lightweight models or introducing a small number of physical priors, these methods learn the mapping between sparse measurement points and high-resolution flow fields and accomplish reconstruction in a matter of seconds. They substantially enhance the efficiency and robustness of flow field reconstruction, rendering this approach one of the most extensively applied technical directions at present [132,133]. The primary advantage of pure data-driven models lies in high-resolution reconstruction of complex turbulent flows. Trained on large-scale labeled datasets, these models can accurately capture the complex nonlinear characteristics and fine-scale structures of flow fields. Without solving intricate physical constraint equations, they enable high-resolution flow field reconstruction within seconds. Nevertheless, such models rely heavily on large-scale labeled data with high spatiotemporal resolution. Their reconstruction accuracy degrades drastically under sparse or noisy measurements, often leading to missing flow details and distorted structures. Generalization is constrained by the distribution of training data, with substantial performance degradation when flow conditions exceed the training range or the sensor layout is modified. Lacking inherent physical constraints, these models exhibit poor interpretability. Zuo et al. [134] achieved end-to-end flow field reconstruction based on the Transform encoder’s deep attention network (DAN). Its batch prediction takes only 23 s (115 s for a single CFD case), greatly reducing the iteration period of aerodynamic design (Fig. 7D). For the problem of high-dimensional and nonlinear characteristics of complex fluid flow fields such as turbulence, Solera-Rico et al. [135] propose an end-to-end AI framework of “β-VAE extraction of spatial features + transformer prediction of temporal dynamics”, which greatly reduces the computational complexity and adapts to the rapid simulation and prediction requirements of engineering scenarios (Fig. 7E). Additionally, the spatiotemporal super-resolution method based on supervised machine learning proposed by Fukami et al. [136] improves efficiency by 3 orders of magnitude compared with DNS (which takes several hours). Different deep learning models have been applied to flow field-related tasks: multiscale temporal-path UNet (MST-UNet) enhances spatiotemporal flow field accuracy [137], the unsupervised deep learning model based on CycleGAN enables super-resolution reconstruction of turbulent flow fields without unpaired data [138], and the combination of GNN and MST pruning optimizes hypersonic flow field reconstruction efficiency with only minimal physical priors [139]. In recent years, the integration of NNs with other technologies has further broken through performance bottlenecks. Zhao et al. [49] proposed a PMNN (POD + MLP) model, which can reconstruct the flow field at the same resolution as that of full CFD simulations (equivalent to 222 grid points) with only 5 measurement points, and the entire process takes merely 2 ms. To address the issues of sparse flow field data or regional data missing, Xu et al. [140] use the Navier–Stokes equations as a loss constraint function. Even when the data sparsity reaches 1% or the data in the core wake region is truncated, the proposed model can still quickly and accurately reconstruct the wake field.
In the future, it can be anticipated that with the in-depth coupling of physical prior information and data-driven models, the physical consistency of NN-based methods will be further enhanced, and the proportion of integrated applications of the 2 types of methods (NN-based and DA-based) will continue to increase. Together, they will promote the development of aircraft flow field reconstruction technology using sparse measurement points toward real-time, intelligent, and highly reliable directions.
The technical merit of iFlexSense extends far beyond its capability for perception–decision information processing. The technical merit of iFlexSense extends far beyond its capability for perception–decision information processing. As the core module for AI- enabled UAVs, it constructs a bridge between in situ flight-related data acquired via structural skin sensing (e.g., pressure, shear stress, and strain) and the signal reconstruction and situational awareness of onboard AI, thereby enabling the directed translation and synergistic coupling of raw sensory inputs into UAV-specific decision outputs. By further advancing its active actuation functionalities, iFlexSense forms an integrated closed-loop intelligent system characterized by perception–actuation–control synergy. On the one hand, leveraging morphing technology to realize active actuation such as dynamic regulation of wing configurations, and combining preacquired sensing data with AI decision-making, it accomplishes tasks like real-time optimization of aerodynamic characteristics. On the other hand, the microstructures themselves can directly endow the skin with specific functional properties—for instance, hydrophobic microstructures and electromagnetic metasurface—enabling the fulfillment of key application requirements without additional complex actuation units. In this way, the intelligent skin evolves from a mere information-sensing system into an intelligent microsystem with active regulation capabilities.
Aircraft icing is a long-standing severe challenge in the aviation field. When an aircraft flies in environments such as clouds and supercooled water mist, supercooled water droplets will rapidly condense and freeze on parts including the fuselage, wings, and engine air inlets [141]. Icing can seriously damage the aerodynamic configuration of an aircraft, leading to lift loss and increased drag within a very short period of time, and may even result in catastrophic incidents such as stall that could cause casualties [142]. Aircraft anti-icing and deicing can be divided into anti-icing systems and deicing systems. Anti-icing technology prevents ice formation or adhesion on aircraft surfaces through nonactive energy input [143]. Among various anti-icing technologies, superhydrophobic surfaces have attracted extensive attention due to their excellent ice-retarding performance, icephobicity, as well as no energy consumption and low cost [144]. Their working principles can be roughly categorized into 2 types: utilizing microstructural design [145] and leveraging inherent material properties [146]. However, superhydrophobic surfaces can only inhibit icing to a limited extent rather than completely prevent it; when the ice layer accumulates to a certain thickness, deicing systems take effect. The traditional deicing method involves the use of hot air and an electric heating system [147,148] (Fig. 8A and B). The hot air system relies on the engine air intake or independent heater to provide heat energy, which requires a large amount of fuel to be converted into heat energy, and there are multistage losses in the energy conversion process, and most of the energy is lost in the pipeline transmission and heat exchange process; the electric heating system starts up with high instantaneous power, which puts great pressure on the aircraft power supply system. In addition, the weight of the whole set of equipment usually reaches hundreds of kilograms, directly increasing the load of the aircraft.
Flexible intelligent skin provides a new possibility for aircraft anti-icing and deicing. The flexible smart skin has achieved considerable weight reduction in structure, reducing the weight by more than 60% compared with traditional electric heating systems [149], while reducing energy consumption by about 50% [150]; during maintenance, only faulty modules need to be replaced, which considerably reduces operating costs. It can be fitted on any complex curved surface to achieve full coverage, avoiding the risk of local icing resulting from uneven heating on the fuselage surface in traditional deicing methods, and can further integrate both an ice condition sensing unit and an anti-icing/deicing module. Xu et al. [151] prepared a superhydrophobic graphene @NiO/Ni surface with triple heat conversion capability. The internal nickel layer imparts magnetocaloric deicing capability, which can achieve high-efficiency deicing throughout the life cycle (Fig. 8C). Zhang et al. [152] reported a structured elastic surface integrated with spring-like columns. These columns can store the work from volume expansion of frozen droplets as elastic energy, then release it rapidly as kinetic energy within milliseconds to achieve spontaneous ejection of the droplets (Fig. 8D). In recent years, active/passive coupled deicing technology has exhibited greater adaptability and effectiveness in different scenarios. Li et al. [153] show a sandwich-structured composite coating integrating both electric heating and superhydrophobic functions: its top layer is composed of hydrophobically modified epoxy resin and carbon black, while the silver nanowires (AgNWs) in the middle layer are used to adjust resistance and enhance electrothermal performance (Fig. 8E). Lee et al. [154] present a multifunctional magnetically responsive photothermal composite cilia array (MRPA). The MRPA exhibits immediate and reversible structural bending motion while maintaining superhydrophobic properties, enabling effective prevention, delay, and removal of ice accumulation (Fig. 8F).
AI-enabled flexible intelligent skin enables intelligent predictive decision-making and active deicing. Via integrated multiparameter sensors and combined with flight conditions, it establishes an “icing risk prediction model” to activate low-power preheating before supercooled water droplets freeze, realizing the mode of “anti-icing first, deicing supplementary”. Jingxin et al. [155] tested an integral glass fiber composite airfoil with superhydrophobic coating and embedded electrothermal film (SHS-EET). Icing wind tunnel experiments showed that SHS-EET reduced ice shedding cycle by 64.6% and energy consumption by 72.3%. AI can also predict icing location and extent; leveraging real-time flight parameters from sensors, it dynamically identifies key icing characteristics such as location, thickness, and morphology. Compared with traditional machine learning methods, identification accuracy in complex icing scenarios improved by ~15% to 20% [156]. Løw-Hansen et al. [157] embedded electrothermal elements in UAV wings, monitoring ice shedding in real time via Kalman filter and continuous wavelet transform. AI algorithms predicted ice peeling time based on temperature changes and dynamically adjusted heating strategies to reduce energy consumption. Suo et al. [158] proposed a wing icing prediction model based on geometric constraint-enhanced NN. It enables rapid airfoil icing prediction (6 ms per case) and exhibits good generalization performance (Fig. 8G). Abdelghany et al. [159] adopted the Internet of Things (IoT) integrated with an ANN to predict the thermal performance of anti-icing systems. The proposed model is calibrated with experimental data to further optimize the heating power distribution, thereby improving the overall deicing efficiency (Fig. 8H). With “flexibility”, flexible intelligent skin breaks through structural adaptability limitations of traditional methods; with “intelligence”, it upgrades from “single deicing” to “multifunction integration and predictive regulation”, becoming one of the core development directions in future aircraft anti-icing and deicing.
Electromagnetic stealth is a crucial capability for aircraft to survive and operate in the modern complex electromagnetic countermeasure environment, which is directly related to the aircraft’s own safety and the success or failure of missions. Enemy electromagnetic detection devices such as radars can locate aircraft by emitting electromagnetic waves and receiving the reflected signals from targets [160]. There are numerous historical cases of aircraft damage caused by electromagnetic exposure. Initially, stealth technology was based on surface coatings for passive absorption/reflection, and later, metamaterials provide new possibilities for stealth technology by actively regulating the propagation path of electromagnetic waves [161]. The metamaterial stealth relied on complex 3D structures (thickness reaches centimeter level), which cannot meet the requirements of “lightweight and thin” in the aerospace field [162]. To address the limitations of 3D metamaterials, researchers compressed the meta-structure from a “3D bulk” to a “2D interface”—the thickness of metasurface is usually less than 1/20 of the wavelength [163]. Its main working mechanisms are divided into 2 types: light diffraction-based stealth and scattering cancellation-based stealth [164,165] (Fig. 9A and B). Integrating electromagnetic metasurface into the flexible intelligent skin of aircraft enables electromagnetic wave scattering reconstruction or phase modulation through the subwavelength microstructures on the metasurface, making this integrated system a new stealth paradigm based on wavefront engineering [166,167].
The involvement of AI technology provides core support for the dynamic stealth capability of aircraft flexible intelligent skins. Its value is concentrated on optimizing the real-time performance and precision of metasurface regulation. The system can dynamically adjust the bias voltage strategy of metasurface elements based on real-time analysis of parameters of incident electromagnetic waves such as reinforcement learning algorithms. This reduces the reflectivity regulation response time from milliseconds to even nanoseconds and expands the broadband stealth bandwidth by over 30% [168]. Qian et al. [169] took the lead internationally in developing a new generation of intelligent stealth devices based on deep learning. The devices can dynamically adapt and integrate with the characteristics of the background electromagnetic environment in only 15 ms (Fig. 9C). However, the experimental object is a perfect electrical conductor bump of a specific size, and the stealth effect can only be achieved for electromagnetic waves in a specific vibration direction. As research continues, stealth devices begin to develop into universal adaptations and achieve full polarization regulation (capable of responding to electromagnetic waves in all vibration directions) [170,171]. The active frequency selective surface (FSS) structure controlled by PIN diodes proposed by Cerveny et al. [172] can achieve full polarization reflectivity regulation in the 9 to 13 GHz band, but it is still difficult to solve the problem of multiband interference in complex electromagnetic environments. In recent years, NNs have been increasingly applied in complex electromagnetic/photonic systems. The pure NN-driven solution does not involve an iterative process during the prediction phase, which is crucial for on-site systems that require rapid responses. This characteristic has facilitated the development of an emerging concept—intelligent metasurface [173] (Fig. 9D). This intelligent metasurface can cancel the interference signal through NN in the electromagnetic environment where other scatterers exist, and without retraining, it can integrate the automatic regulation strategy of environmental sensing information, responding to design targets of multiple reflection modes with extremely low on-site computing capacity and time [174]. Next-generation stealth systems impose more stringent requirements on secure electromagnetic transmission, which demands reliable information delivery while avoiding electromagnetic radiation exposure. The radiation–stealth integrated metasurface provides a viable technical solution [175], enabling simultaneous high-efficiency dynamic radiation and low-observable full-polarization stealth within the same operating frequency band.
In addition to the exploration of general metasurface technology, research targeting radar detection, a typical application scenario, has also achieved new breakthroughs [176,177]. The core of radar detection is to achieve the maximum signal-to-noise ratio to improve the detection probability. The multiradar networking system proposed by Zheng et al. [178] has advanced metasurface technology from theoretical feasibility to engineering practicality (Fig. 9E). In addition, when an aircraft encounters wing deformation caused by airflow disturbance, it is also important to predict the attenuation trend of stealth performance in advance [179]. Xu et al. [180] proposed an intelligent reflecting surface that integrates integrated radiation and scattering control and integrated sensing and communication technologies. By conducting cross-dimensional fusion training on the sensed flow field pressure distribution data and metasurface electromagnetic scattering characteristic data, it can accurately modulate electromagnetic waves in real time according to dynamic variations of the external environment, thereby controlling the fluctuation of radar cross-section and achieving adaptive active stealth. Li et al. [181] demonstrated a flexible intelligent surface platform (FISP). This platform takes the metasurface’s own shape information as the core input, and the ANN-driven algorithm generates coding sequences by feeding data from the sensor array, with a response time of approximately 16.7 ms (Fig. 9F). Stochastic evolutionary learning (SEL)—a 2-stage mechanism that generates candidate solutions and selects optimal solutions—constitutes a core breakthrough at the algorithmic level (Fig. 9G). Qian et al. [182] innovatively adopted spatiotemporal modulation metasurface, breaking through the limitation that pure spatial-domain functional modulation can only be achieved by adjusting the spatial distribution or phase of metasurface elements, and completed outdoor flight tests across air–sea–land scenarios. This breakthrough is not only an upgrade of metasurface technology but also opens up a new paradigm of “flight autonomous stealth”, laying a foundation for the next generation of intelligent stealth equipment.
In the future, flexible intelligent skins in the electromagnetic stealth field must address core challenges such as high-density integration of metamaterials with skins and extreme environment adaptability, continue to advance toward multiband compatibility and AI-driven real-time adaptive electromagnetic regulation, and achieve dynamic stealth and synergistic adaptation with the environment.
The development of aircraft lift-enhancing and drag-reducing technology has always been confronted with the contradiction of balancing functional requirements and aerodynamic performance. Existing technologies often manifest themselves as “passive remediation” [183]. Taking the Boeing 737 MAX series as an example, to accommodate the LEAP-1B engines—with higher thrust and better fuel efficiency—the design team had to reposition the engines rearward and increase their size. This modification undermined the aircraft’s original pitch stability: under critical operating conditions such as low speed and high angle of attack, the aircraft nose tended to pitch up excessively, and there was even a risk of stall. To address this issue, Boeing developed the Maneuvering Characteristics Augmentation System (MCAS) [184]. Achieve “remedial control” by automatically pressing down the machine head under specific conditions (Fig. 10A). The shape of a traditional aircraft is fixed after the aircraft leaves the factory; it can only adapt to limited operating conditions through segmented adjustments of mechanical components such as flaps and slats. This highlights the bottleneck of current lift-increasing and drag-reducing technologies. The flexible smart skins can sense the airflow state in real time and dynamically adjust their curvature of the skin (macroscopic level) or local convex–concave structures (microscale surface), thus actively reducing drag and enhancing lift [185].
The flexible skins can achieve continuous bending of the wing along its full span and chord (Fig. 10B), and under AI enablement, the optimal airfoil profile for different operating conditions can be calculated to realize full-range airflow adaptation [186,187]. In addition, inspired by highly efficient aerodynamic organisms in nature, the flexible skin can achieve aerodynamic optimization by guiding airflow from surface protrusions and inhibiting separation from local oscillations [188,189]. The aerodynamic performance of the shark-skin-mimicking microgrooves is theoretically underpinned by the Reynolds-Averaged Navier–Stokes equations for incompressible turbulent boundary layers. Mimicking the microgroove structure of the shark skin—micrometer-scale rhombus-shaped protrusions and grooves—these microstructures constrain the spanwise near-wall flow, inhibit the development of streamwise vortices and hairpin vortices, and reduce turbulent Reynolds stresses, thereby stabilizing the near-wall flow into a low-fluctuation laminar-like state; the drag-reduction effect is optimal within the Reynolds number range corresponding to the laminar and laminar-turbulent transition regimes. The flexible skin uses the microstructure of protrusions and grooves to avoid airflow disturbance caused by lateral disturbances, delaying the transition of airflow from laminar to turbulent flow, thereby reducing frictional resistance [190], whereas the microstructure loses effectiveness or fails when the Reynolds number exceeds the upper bound of the optimal range (resulting in fully developed turbulence) or under high free-stream turbulence intensity and strong sudden disturbances, as intense turbulent mixing or an inherently unstable boundary layer negates the flow-guiding and disturbance-suppression effects. Furthermore, borrowing from dolphins to correct eddy and surface airflow disturbances in real time through microvibrations (Fig. 10C), by causing active disturbances such as micro-oscillations in specific areas of the skin, the external airflow is “sucked” into the separation zone and reattached to the wing surface, thereby suppressing the risk of stall [191].
The self-sensing capability and structural control function of flexible intelligent skins lay the foundation for aerodynamic optimization, while AI realizes the “perception–deformation–optimization” closed loop, enabling the system to evolve into active intelligent control. To address the challenge of limited aerodynamic datasets, it is crucial to enhance the model’s ability and efficiency in predicting aerodynamic parameters under unknown conditions. Studies such as cross-attention models incorporating physical information [192], denoising diffusion aerodynamic models [193], and generative design models based on conditional VAEs [194], among others, have been successively proposed. In the exploration of such generative models, the VAE framework, leveraging its advantage of flexible parameter regulation, has gradually been applied in airfoil design. Kang et al. [195] proposed a β-VAE-based airfoil parameterization method that can independently adjust physical parameters such as thickness and camber to generate smooth, nonself-intersecting airfoils (Fig. 10D). To meet more complex aerodynamic engineering requirements, Liu et al. [196] proposed a dual-module collaborative model: a deep neural network (DNN) rapidly outputting accurate flow field distributions; the deep reinforcement learning (DRL) optimization module continuously adjusts airfoil parameters via interactive learning with the DNN-predicted flow field, ultimately producing adaptive optimization strategies (Fig. 10E). Although there are relatively few studies in the literature on using flexible intelligent skins to actively alter surface protrusions or local oscillation states to intervene in airflow attachment and separation on wing surfaces, numerous studies have confirmed the drag reduction effect of transverse grooves [197,198]. Inspired by dolphin skin—whose dynamic microscale oscillations substantially affect the boundary layer near the skin—Wang and Liu’s research [199] demonstrated that this mechanism not only enables effective drag reduction through dynamic oscillations but also generates additional thrust.
It is foreseeable that morphing wings capable of intelligent adaptive deformation and real-time adaptation to multiple flight conditions will spearhead the development of future aircraft; meanwhile, research on the surface microstructures of flexible skins based on bionic design will also emerge as a core focus for advancing the aerodynamic performance of aircraft.
This review outlines the technical characteristics and development evolution of iFlexSense, and elaborates on its technical pathway to achieve full-scenario perception–decision–actuation by integrating multidimensional sensing/actuation units on ultrathin substrates and combining AI-enabled super-resolution field reconstruction algorithms. It conducts an in-depth analysis of the technology’s breakthrough applications in 3 core scenarios—anti-icing/deicing, electromagnetic stealth, and lift enhancement/drag reduction—as well as its substantial improvements to aircraft safety, survivability, and energy efficiency. This technology thoroughly breaks the inherent design limitations of traditional aircraft that passively adapt to aerodynamic environments, establishing a new paradigm featuring active airflow perception and dynamic adjustment of surface properties. Nevertheless, there remains room for further development and refinement of iFlexSense, and the following aspects are poised to become its core future development directions.
Unit cell modularization and high-density integration are the core future development directions of iFlexSense. Leveraging electronic row–column scanning and signal demodulation, multiphysical sensing modules are integrated into a single sensor unit cell, enabling synchronous acquisition and accurate resolution of multidimensional physical parameters at the same spatial position. This greatly improves the sensing system’s integration density and data integrity, while reducing redundant sensor deployment. However, the technology still needs further optimization in terms of large-scale mass production processes and cost control. Key breakthroughs are required in material costs and the stability of batch preparation, so as to promote its transformation from laboratory prototypes to large-scale commercial products.
Edge intelligence represents a major trend in future development. Moving forward, focus should be placed on the lightweight development of AI algorithms: computational complexity can be reduced through techniques such as model compression and quantization, while deployment of edge computing modules enables the migration of data processing to the local skin system. This will substantially enhance the real-time performance of data processing and the efficiency of autonomous decision-making. Practical engineering application needs to address the power consumption constraint of edge hardware under aircraft limited energy supply, and the compatibility issue between lightweight models and dynamic physical signal noise in complex flight environments.
In existing flexible intelligent skins, functions such as anti-icing/deicing, electromagnetic stealth, and lift enhancement/drag reduction are mostly designed independently. It is necessary to deepen the multifunctional collaborative design—for instance, integrating the electrothermal elements for anti-icing/deicing with the conductive network of stealth coatings in an integrated manner. This will effectively reduce system complexity and overall aircraft energy consumption, meeting the development requirements of next-generation energy-saving and multimission aircraft. Key engineering challenges include material interface peeling between integrated functional layers under cyclic mechanical stress (e.g., aircraft takeoff/landing), and uneven energy distribution in electrothermal–stealth integrated structures affecting both function efficiencies.
Embodied intelligence, as the latest research direction of iFlexSense, has demonstrated its core potential. Going forward, efforts should focus on advancing the evolution from the basic perception–decision–actuation closed loop to advanced autonomous learning, dynamic environmental adaptation, and multitask collaborative decision-making. This will fully unleash the core value of iFlexSense as an embodied intelligent agent for next-generation aircraft, and meet the higher-level requirements for autonomous and collaborative development of next-generation intelligent aircraft in complex mission scenarios. From a practical implementation perspective, the real-time response lag of autonomous learning algorithms under high-dynamics flight conditions and the difficulty in validating multitask collaborative decision robustness across extreme weather and mission switching scenarios need to be resolved.
1.
Natarajan G, Elango E, Sundaravadivazhagan B, Rethinam S. Artificial intelligence algorithms and models for embodied agents: Enhancing autonomy in drones and robots. In: Building embodied AI systems: The agents, the architecture principles, challenges, and application domains. Springer; 2025. p. 103–132.
2.
Sapkota R, Roumeliotis KI, Karkee M. UAVs meet agentic AI: A multidomain survey of autonomous aerial intelligence and agentic UAVs. arXiv. 2025. https://doi.org/10.48550/arXiv.2506.08045
3.
Xiong W, Zhu C, Guo D, Hou C, Yang Z, Xu Z, Qiu L, Yang H, Li K, Huang Y.Bio-inspired, intelligent flexible sensing skin for multifunctional flying perception. Nano Energy. 2021;90:Article 106550.
4.
Huang S, Liu Y, Zhao Y, Ren Z, Guo CF.Flexible electronics: Stretchable electrodes and their future. Adv Funct Mater. 2019;29(6):1805924.
5.
Shin HS, Ott Z, Beuken LG, Ranganathan BN, Humbert JS, Bergbreiter S.Bio-inspired large-area soft sensing skins to measure UAV wing deformation in flight. Adv Funct Mater. 2021;31(23):2100679.
6.
Hao M, Guo D, Zhang F, Huang Y. Yunteng G. Flexible intelligent skin multi-parameter measurement of aerodynamic loads on aircraft surfaces. In: Journal of Physics: Conference Series. IOP Publishing; 2025. p. 012004.
7.
Karbasian H, van Rees WM. A deep-learning surrogate model approach for optimization of morphing airfoils. In: Proceedings of the AIAA SCITECH. AIAA; 2023. p. 1619.
8.
Goraj Z. An overview of the deicing and anti-icing technologies with prospects for the future. In: Proceedings of the 24th International Congress of the Aeronautical Sciences. Edinburgh (UK): Optimage Ltd.; 2004.
9.
Rao GA, Mahulikar SP.Integrated review of stealth technology and its role in airpower. Aeronaut J. 2002;106(1066):629–642.
10.
Hosseini SS, van Dam C, Pandya SA. Surface-normal active flow control for lift enhancement and separation mitigation for high-lift common research model. In: Proceedings of the AIAA Scitech. AIAA; 2021. p. 1192.
11.
Li S, Kong C, Wu E, Yang C, Gao Z, Zhou X, Guo H, Jiang S, Liang JG.Advanced wearable biosensing and wireless integration technologies for next-generation healthcare monitoring. Soft Sci. 2026;6(1):17.
12.
Wang S, Chen X, Li S, Sun B, Chen X, Tian H, Wang C, Li X, Shao J.Advances in micro/nano-engineered flexible sensor arrays for intelligent human-machine interaction. Soft Sci. 2025;5(28):28.
13.
Casallas JS, Parra HG, Gaona EE.Wireless real-time data acquisition system for aerodynamic characterization of a wind turbine. Ingeniería. 2023;28:Article e18860.
14.
Wu Y, Dai Y, Yang C.Time-delayed active control of stall flutter for an airfoil via camber morphing. AIAA J. 2022;60(10):5723–5734.
15.
Jacob B, Kligys S, Chen B, Zhu M, Tang M, Howard A, Adam H, Kalenichenko D. Quantization and training of neural networks for efficient integer-arithmetic-only inference. IN: Proceedings of the IEEE Conference on Computer Vision and Pattern Recognition. IEEE; 2018. p. 2704–2713
16.
Li Y, Zheng X, Zheng J, Cheng N, Zheng B, Zhang C, Wang Y.AdaSP: Adaptive soft filter pruning with layer-wise ratios for model compression in low-altitude UAVs. IEEE Trans Cogn Commun Netw. 2017;12:3573–3585.
17.
Pang G, Yang G, Pang Z.Review of robot skin: A potential enabler for safe collaboration, immersive teleoperation, and affective interaction of future collaborative robots. IEEE Trans Med Robot Bionics. 2021;3(3):681–700.
18.
Arents J, Greitans M.Smart industrial robot control trends, challenges and opportunities within manufacturing. Appl Sci. 2022;12(2):937.
19.
Wang G, Hu C, Zheng D.Theoretical and simulation analysis of a thin film temperature sensor error model for in situ detection in near space. Appl Sci. 2023;13(10):5954.
20.
Guo K, Lu Y, Liu Z.High-temperature thin-film thermocouple for aero-engines. PLoS One. 2025;20(8):Article e0329462.
21.
Li W, Li Y, Xu M, Zhou Y, Miao R, Wang K, Cao Y, Song Y, Dang S, Zheng L, et al.Highly customizable, ultrawide-temperature free-form flexible sensing electronic systems based on medium-entropy alloy paintings. Nat Commun. 2025;16(1):7351.
22.
Guo D, Ling J, Huang Y, Xiong W, Xu Y, Bai Y, Li K, Zhang F, Huang Y.Recrystallization-induced laser lift-off strategy for flexible thermal sensors with near-limit sensitivity. Adv Mater Technol. 2024;9(2):2301444.
23.
Zhang F, Xu ZY, Hou C.Flexible, super-resolution skin with in-sensor hyperdimensional computing for real-time pressure field perception. Sci Adv. 2026.
24.
Fan F, Chen L, Wang Y, Wang P, Niu Y, Lv Y, Zhou Y, Shu Z, Liu P, Dong W, et al.Damage-free dry transfer printing of ultrathin films with on-demand interfacial adhesion: Principles and applications. Soft Sci. 2025;5(4):52.
25.
Lee DW, Park DH, Choi J-C, Chung S.Strain-engineered stretchable substrates for free-form display applications. Soft Sci. 2024;4(4):38.
26.
Qu Y, Sun H, Dong C, Kang J, Dai H, Wu Q, Guo S.Elastic collaborative edge intelligence for UAV swarm: Architecture, challenges, and opportunities. IEEE Commun Mag. 2023;62(1):62–68.
27.
Fu B, De Jong C, Guardado NG, Soriano AR, Reyes A.Event-driven predictive gaze analytics to enhance aviation safety. Proc ACM Hum Comput Interact. 2025;9(3):1–18.
28.
Tong C, Yin X, Wang S, Zheng Z.A novel deep learning method for aircraft landing speed prediction based on cloud-based sensor data. Futur Gener Comput Syst. 2018;88:552–558.
29.
Sadeghi A, Bellavista P, Song W, Yazdani-Asrami M.Digital twins for condition and fleet monitoring of aircraft: Toward more-intelligent electrified aviation systems. IEEE Access. 2024;12:99806–99832.
30.
Campbel N, Grauer J, Gregoryl I. Loss of control detection for commercial transports using conditional variational autoencoders. NASA Report. 2021.
31.
Dong Y, Ai J.Inflight parameter identification and icing location detection of the aircraft: The time-varying case. J Control Sci Eng. 2014;2014(1):Article 396532.
32.
Zhang N, Chen K, Hu Q, Zhao J, Zhao J, Jiang T, Feng Y.Spatiotemporal metasurface to control electromagnetic wave scattering. Phys Rev Appl. 2022;17(5):Article 054001.
33.
Ai L, Soltangharaei V, Bayat M, Van Tooren M, Ziehl P.Detection of impact on aircraft composite structure using machine learning techniques. Meas Sci Technol. 2021;32(8):Article 084013.
34.
Hasan M, Redonnet S, Zhongmin D.Aerodynamic optimization of aircraft wings using machine learning. Adv Eng Softw. 2025;200:Article 103801.
35.
Bouzidi Z, Terrissa LS, Zerhouni N, Ayad S.An efficient cloud prognostic approach for aircraft engines fleet trending. Int J Comput Appl. 2020;42(5):514–529.
36.
Shabbir A.Utilizing artificial intelligence for predictive maintenance in aircraft: Enhancing efficiency, safety, and operational reliability. Pak Advances in Engineering Research. 2024;1(02):73–83.
37.
Canan JW.USAF in the twenty-first century. Air Force Magazine. 1986;48.
38.
Jiang F, Tai Y C, Walsh K, Tsao T, Lee G-B, Ho C-M. A flexible MEMS technology and its first application to shear stress sensor skin. In: Proceedings IEEE The Tenth Annual International Workshop on Micro Electro Mechanical Systems An Investigation of Micro Structures, Sensors, Actuators, Machines and Robots. IEEE; 1997. p. 465–470
39.
Jiang F, Lee G-B, Tai Y-C, Ho C-M.A flexible micromachine-based shear-stress sensor array and its application to separation-point detection. Sensors Actuators A Phys. 2000;79(3):194–203.
40.
Moes TR, Sarma GR, Mangalam SM. Flight demonstration of a shock location sensor using constant voltage hot-film anemometry. NASA; 1997.
41.
Florance J, Fleming G, Burner A. Contributions of the NASA Langley Research Center to the DARPA/AFRL/NASA/Northrop Grumman smart wing program. In: 44th AIAA/ASME/ASCE/AHS/ASC Structures, Structural Dynamics, and Materials Conference. AIAA; 2003
42.
Sun G, Li H, Dong M.RETRACTED: Optical fiber shape sensing of polyimide skin for a flexible morphing wing. Appl Opt. 2017;56(33):9325–9332.
43.
Lawson NJ, Correia R, James SW, Partridge M, Staines SE, Gautrey JE, Garry KP, Holt JC, Tatam RP.Development and application of optical fibre strain and pressure sensors for in-flight measurements. Meas Sci Technol. 2016;27(10):Article 104001.
44.
Matsuhisa N, Kaltenbrunner M, Yokota T, Jinno H, Kuribara K, Sekitani T, Someya T.Printable elastic conductors with a high conductivity for electronic textile applications. Nat Commun. 2015;6(1):7461.
45.
Dickey MD.Stretchable and soft electronics using liquid metals. Adv Mater. 2017;29(27):1606425.
46.
Choi S, Han SI, Kim D, et al.High-performance stretchable conductive nanocomposites: Materials, processes, and device applications. Chem Soc Rev. 2019;48(6):1566–1595.
47.
Wang Y, Qiu L, Luo Y, Ding R.A stretchable and large-scale guided wave sensor network for aircraft smart skin of structural health monitoring. Struct Health Monit. 2021;20(3):861–876.
48.
Xiong WN, Guo DL, Yang ZX, et al.Conformable, programmable and step-linear sensor array for large-range wind pressure measurement on curved surface. SCIENCE CHINA Technol Sci. 2020;63(10):2073–2081.
49.
Zhao QY, Huang J, Guo YX, Ji J, Huang YA.Machine learning-assisted sparse observation assimilation for real-time aerodynamic field perception. Sci China Technol Sci. 2024;67(5):1458–1469.
50.
Qian CKI, Chen H.A guidance to intelligent metamaterials and metamaterials intelligence. Nat Commun. 2025;16(1):1154.
51.
Huang YA, Zhu C, Xiong WN, Wang Y, Jiang YG, Qiu L, Guo DL, Hou C, Jiang S, Yang Z, et al.Flexible smart sensing skin for “Fly-by-feel” morphing aircraft. Sci China Technol Sci. 2022;65(1):1–29.
52.
Li Q, Tan T, Wang B, Yan Z.Avian-inspired embodied perception in biohybrid flapping-wing robotics. Nat Commun. 2024;15(1):9099.
53.
Wang Y, Wang CQ, Pu W, Qui L.A large-scale sensing-monitoring integrated aircraft smart skin with ultralow weight and ultralow power consumption for structural health monitoring. IEEE Trans Ind Electron. 2024;72(2):2130–2139.
54.
Xu ZY, Xie EX, Hou C.AI-enabled flexible electronic systems via near-sensor and in-sensor computing. npj Flex Electron. 2026;10:52.
55.
Zhang C, Patras P, Haddadi H.Deep learning in mobile and wireless networking: A survey. IEEE Commun Surv Tutor. 2019;21(3):2224–2287.
56.
Russell J. Performance and stability of aircraft. Butterworth-Heinemann; 1996.
57.
Braud C, Podvin B, Deparday J.Study of the wall pressure variations on the stall inception of a thick cambered profile at high Reynolds number. Phys Rev Fluids. 2024;9(1):Article 014605.
58.
Wood KT, Araujo-Estrada S, Richardson T, et al.Distributed pressure sensing–based flight control for small fixed-wing unmanned aerial systems. J Aircr. 2019;56(5):1951–1960.
59.
Leitzke JP, Della Mea A, Faller LM, et al.Wireless differential pressure measurement for aircraft. Measurement. 2018;122:459–465.
60.
Xuan Y, Uchiyama T, Ura H, Hagiwara S, Kato H, Sarkar SK, Takei K.Flexible integrated air pressure sensors for monitoring positive and negative pressure distribution. ACS Appl Mater Interfaces. 2024;16(40):54215–54223.
61.
Wang J, Wei X, Shi J, Bai N, Wan X, Li B, Chen Y, Jiang Z, Guo CF.High-resolution flexible iontronic skins for both negative and positive pressure measurement in room temperature wind tunnel applications. Nat Commun. 2024;15(1):7094.
62.
Zhao D, Li F, Yu Y, Wu Y, Tang M, Wei K, Liu Y, Guo Y, Wang P, Wang H, et al.High-dielectric-constant polymer-based elastomeric dielectrics for soft electronic devices. Soft Sci. 2026;6:13.
63.
Zhang J, Tang C, Kong Q, He M, Lv P, Guo H, Guo Y, Shi X, Gu J.Strong and tough polyvinyl alcohol hydrogels with high intrinsic thermal conductivity. Soft Sci. 2025;5:9.
64.
Dong Z, Gong Z, Chen B, Sheng T, Cao Y, He Q, Zhao P, Jiang Y.Ultrathin flexible skin with all-polyimide pressure and airflow sensor array for estimation of flight parameters. IEEE Sensors J. 2023;23(23):29494–29501.
65.
Luo X, Gianchandani YB.A 100 μm diameter capacitive pressure sensor with 50 MPa dynamic range. J Micromech Microeng. 2016;26(4):Article 045009.
66.
Hu L, Zhang F, Luo L, Leng J.Advances in shape memory polymer porous materials: Fabrications, microstructures, and applications. Research. 2025;8:0989.
67.
Javed Y, Mansoor M, Shah IA.A review of principles of MEMS pressure sensing with its aerospace applications. Sens Rev. 2019;39(5):652–664.
68.
Yang X, Wang Y, Qing X.A flexible capacitive pressure sensor based on ionic liquid. Sensors. 2018;18(7):2395.
69.
Silvester DS, Jamil R, Doblinger S, Zhang Y, Atkin R, Li H.Electrical double layer structure in ionic liquids and its importance for supercapacitor, battery, sensing, and lubrication applications. J Phys Chem C. 2021;125(25):13707–13720.
70.
Li Y, Dong Z, Gong Z, Ma Z, Ke X, Sheng T, Yang X, Ding X, Jiang Y.An analytical pressure-velocity fusion algorithm-empowered flexible sensing patch for flight parameter detection. npj Flex Electron. 2025;9(1):75.
71.
Schlichting H, Gersten K. Boundary-layer theory. Springer; 2016.
72.
Tanner LH, Blows LG.A study of the motion of oil films on surfaces in air flow, with application to the measurement of skin friction. J Phys E Sci Instrum. 1976;9:194.
73.
Ghouila-Houri C, Arnoult T, Mazzamurro A, Kern S, Viard R, Teillet D, Palfi E, Garnier E, Talbil A, Pernod P. Flight-testing of a MEMS wall shear stress thermal sensor on a microlight aircraft. In: 2023 IEEE Sensors. IEEE; 2023.
74.
Driver DM, Drake A.Skin-friction measurements using oil-film interferometry in NASA’s 11-foot transonic wind tunnel. AIAA J. 2008;46(10).
75.
Yatskikh A, Kosinov A, Semionov N, Smorodsky B, Ermolaev Y, Kolosov G. Investigation of laminar-turbulent transition of supersonic boundary layer by scanning constant temperature hot-wire anemometer at Mach 2–4. In: Proceedings of the AIP Conference Proceedings, F. AIP Publishing LLC; 2021.
76.
Yan Y-C, Jiang C-Y, Chen R-B, Ma B-H, Deng J-J, Zheng S-J, Lou J.Highly sensitive flow sensor based on flexible dual-layer heating structures. Sensors. 2020;20(22):6657.
77.
Ghouila-Houri C, Gallas Q, Garnier E, Merlen A, Viard R, Talbi A, Pernod P.High temperature gradient calorimetric wall shear stress micro-sensor for flow separation detection. Sensors Actuators A Phys. 2017;266:232–241.
78.
Murakami K, Shiraishi D, Mizumi S, Oya Y, Omura N, Shibata T, Ichikawa Y, Motosuke M.Development of a flexible MEMS sensor for subsonic flow. Micromachines. 2022;13(8):1299.
79.
Song X, Xiao K, Xu W.An ultrathin and fast response flexible shear stress sensor with improved thermal efficiency. IEEE Sensors Letters. 2024;8(8):1–4.
80.
Gong Z, Di W, Jiang Y.Flexible calorimetric flow sensor with unprecedented sensitivity and directional resolution for multiple flight parameter detection. Nat Commun. 2024;15(1):3091.
81.
Pang P, Zhao K, Zhong S.Flexible skin for measurement of boundary layer state and flight attitude identification on UAV. Smart Mater Struct. 2023;32(4):Article 045008.
82.
Pang P, Zhang J, Luo C, Ma B, Zhang X, Luo J, Deng J. Flexible sensing skin for simultaneous measurement of wall shear stress, flow direction and dynamic pressure. In: 2024 IEEE Sensors. IEEE; 2024. p. 1–4.
83.
Sun B, Ma B, Wang P.High sensitive flexible hot-film sensor for measurement of unsteady boundary layer flow. Smart Mater Struct. 2020;29(3):Article 035023.
84.
Rahul V, Alokita S, Jayakrishna K. Structural health monitoring of aerospace composites. Woodhead Publishing; 2019.
85.
Sudhanshu S, Zunjarrao K.Piezoresistive strain monitoring sensors for structural health monitoring of fibre-reinforced composites. J Mater Sci. 2026;61:10715–10764.
86.
Gao Z, Zhu X, Fang Y, Zhang H.Active monitoring and vibration control of smart structure aircraft based on FBG sensors and PZT actuators. Aerosp Sci Technol. 2017;63:101–109.
87.
Liu T-W, Bai J-B, Li S-L, Fantuzzi N.Large deformation and failure analysis of the corrugated flexible composite skin for morphing wing. Eng Struct. 2023;278:Article 115463.
88.
Wang G, Zhao Y, Wang Z, Wang J, Wang S, Zhang Y, Zheng K, Han F, Wang C, Jiang Z.Island-shaped micro-cracks evolution in ultrathin film enables ultra-sensitive for strain sensors under high temperatures. Chem Eng J. 2025;512:Article 162321.
89.
Zhang Y, Anderson N, Bland S, Nutt S, Jursich G, Joshi S.All-printed strain sensors: Building blocks of the aircraft structural health monitoring system. Sensors Actuators A Phys. 2017;253:165–172.
90.
Raffaele L, Liberata G, Francesca A, Schiavo L, Oliviero M, Sorrentino A, Fiorentino M, Vertuccio L.Exploitation of the tunneling effect for the development of self-sensing nanocomposite materials. Appl Mater Today. 2025;46:Article 102882.
91.
Yu H, Bian J, Chen F, Ji J, Huang Y.Ultrathin, graphene-in-polyimide strain sensor via laser-induced interfacial ablation of polyimide. Adv Electron Mater. 2023;9(9):2201086.
92.
Guo D, Hao M, Zhang F, Lv X, Xu Z, Hou C, Ling J, Guo W, Ji J, Lai W.A bilateral, flexible sensing skin integrated in-situ self-compensation for multi-modal measurement of morphing wings. IEEE Sensors J. 2025;25(16):30455–30463.
93.
Meng W, Pal A, Bachilo SM, Weisman RB, Nagarajaiah S.Next-generation 2D optical strain mapping with strain-sensing smart skin compared to digital image correlation. Sci Rep. 2022;12:11226.
94.
Salmanpour MS, Sharif Khodaei Z, Aliabadi MH.Airborne transducer integrity under operational environment for structural health monitoring. Sensors. 2016;16(12):2110.
95.
Wang K, Wang H, Zhang X, Li Y, Zhou Y, Xu M, Li W, Zheng L, Wang X, Huang W.Pulsed laser-assisted direct fabrication of MoxW1-xS2 alloy-based flexible strain sensors with superior performance for high-temperature applications. Microsyst Nanoeng. 2025;11(1):161.
96.
Langat RK, Deng W, De Luycker E, Cantarel A, Rakotondrabe M.In-situ piezoelectric sensors for structural health monitoring with machine learning integration. Mechatronics. 2025;106:Article 103297.
97.
Chen X, Zeng Q, Shao J, Li S, Li X, Tian H, Liu G, Nie B, Lou Y.Channel-crack-designed suspended sensing membrane as a fully flexible vibration sensor with high sensitivity and dynamic range. ACS Appl Mater Interfaces. 2021;13(29):34637–34647.
98.
Hu Y, Guo R, Wang H, Zhao R, Ning R, Huang Z, Chu Z, Peng Y, Zhang Y, Zhang H.Gear-fault monitoring and digital twin demonstration of aircraft engine based on piezoelectric vibration sensor for engine health management. Nano Energy. 2025;133:Article 110448.
99.
Chao X, Hu H, Lin J, Ge X, Wang Y, Xie L, Hu B, Meng L, Yu S, Liang F, et al.Bioinspired twist-hyperbolic metamaterial for impact buffering and self-powered real-time sensing in UAVs. Sci Adv. 2025;11(36):eadw6179.
100.
Wang Y, Wang Y, Liu X, Wang X, Dai K, You Z.Self-powered microsystem for ultra-fast crash detection via Prestressed triboelectric sensing. Research. 2025;8:0753.
101.
Farrar CR, Worden K. Structural health monitoring: A machine learning perspective. John Wiley & Sons; 2012.
102.
Dey S, Bhattacharyya R, Sarma SE, Karmakar NC.A novel “smart skin” sensor for chipless RFID-based structural health monitoring applications. IEEE Internet Things J. 2020;8(5):3955–3971.
103.
Qiu L, Lin X, Wang Y, Yuan S, Shi W.A mechatronic smart skin of flight vehicle structures for impact monitoring of light weight and low-power consumption. Mech Syst Signal Process. 2020;144:Article 106829.
104.
Zhu C, Xu Z, Hou C, Lv X, Jiang S, Ye D, Huang Y.Flexible, monolithic piezoelectric sensors for large-area structural impact monitoring via MUSIC-assisted machine learning. Struct Health Monit. 2024;23(1):121–136.
105.
Del Priore E, Lampani L.Real-time damage detection and localization on aerospace structures using graph neural networks. J Sens Actuator Netw. 2025;14(5):89.
106.
Zheng Z, Lu J, Liang D.Load-identification method for flexible multiple corrugated skin using spectra features of FBGs. Aerospace. 2021;8(5):134.
107.
Pagani A, Enea M, Carrera E.Component-wise damage detection by neural networks and refined FEs training. J Sound Vib. 2021;509:Article 116255.
108.
Wang Z, Yang D-H, Yi T-H, Zhang G-H, Han J-G.Eliminating environmental and operational effects on structural modal frequency: A comprehensive review. Struct Control Health Monit. 2022;29(11): https://doi.org/10.1002/stc.3073
109.
Wang C, Wang Y, Pu W, Qiu L.A miniaturized and ultra-low-power wireless multi-parameter monitoring system with self-powered ability for aircraft smart Skin. Sensors. 2024;24(24):7993.
110.
Zhang A, Li X, Gao Y, Niu Y.Event-driven intrinsic plasticity for spiking convolutional neural networks. IEEE Trans Neural Networks Learn Syst. 2021;33(5):1986–1995.
111.
Dang HV, Tatipamula M, Nguyen HX.Cloud-based digital twinning for structural health monitoring using deep learning. IEEE Trans Industr Inform. 2021;18(6):3820–3830.
112.
Wang Y, Lei P, Wang X, Jiang L, Xuan L, Cheng W, Zhao H, Li Y.Leveraging large self-supervised time-series models for transferable diagnosis in cross-aircraft type bleed air system. Adv Eng Inform. 2025;65:Article 103275.
113.
Mylonas C, Chatzi E.Remaining useful life estimation for engineered systems operating under uncertainty with causal GraphNets. Sensors. 2021;21(19):6325.
114.
Dagal I, Erol B, Mbasso WF, Harrison A, Demirci A, Cali U.A data-driven approach to aircraft engine MRO using enhanced ANNs based on FMECA. IEEE Access. 2025;13:124710–124733.
115.
Li C, Mahadevan S, Ling Y.Dynamic Bayesian network for aircraft wing health monitoring digital twin. AIAA J. 2017;55(3):930–941.
116.
Cotorobai A, Silva JM, Oliveira JL. A federated random forest solution for secure distributed machine learning. In: 2025 IEEE 38th International Symposium on Computer-Based Medical Systems (CBMS). IEEE; 2025. p. 769–774.
117.
Rosero RHL, Silva C, Ribeiro B.Remaining useful life estimation in aircraft components with federated learning. PHM Society European Conference. 2020;9–9.
118.
Landau D, de Pater I, Mitici M, Saurabh N.Federated learning framework for collaborative remaining useful life prognostics: An aircraft engine case study. Futur Gener Comput Syst. 2025;174:107945.
119.
Raouf I, Kumar P, Cheon Y, Tanveer M, Jo S-H, Heung S.Advances in prognostics and health management for aircraft landing gear—Progress, challenges, and future possibilities. Int J Precis Eng Manuf-Green Technol. 2025;12(1):301–320.
120.
Basora L, Bry P, Olive X, Freeman F.Aircraft fleet health monitoring with anomaly detection techniques. Aerospace. 2021;8(4):103.
121.
Kabashkin I, Perekrestov V, Tyncherov T, Shoshin L, Susanin V.Framework for integration of health monitoring systems in life cycle management for aviation sustainability and cost efficiency. Sustainability. 2024;16(14):6154.
122.
Liu Q, Xu Y, Kurths J, Liu X.Complex nonlinear dynamics and vibration suppression of conceptual airfoil models: A state-of-the-art overview. Chaos. 2022;32(6):062101.
123.
Peng J-Z, Chen S, Aubry N, Chen Z-H, Wu W-T.Time-variant prediction of flow over an airfoil using deep neural network. Phys Fluids. 2020;32(12):123602.
124.
Luo Z, Wang L, Xu J, Chen M, Yuan J, Tan ACC.Flow reconstruction from sparse sensors based on reduced-order autoencoder state estimation. Phys Fluids. 2023;35(7):075127.
125.
Zhong Y, Fukami K, An B, Taira K. Sparse sensor reconstruction of vortex-impinged airfoil wake with machine learning. arXiv. 2023. https://doi.org/10.48550/arXiv.2305.05147
126.
Patel Y, Mons V, Marquet O, Rigas G.Turbulence model augmented physics-informed neural networks for mean-flow reconstruction. Phys Rev Fluids. 2024;9(3):Article 034605.
127.
Li S, He C, Liu Y.Unsteady flow enhancement on an airfoil using sliding window weak-constraint four-dimensional variational data assimilation. Phys Fluids. 2023;35(6):065122.
128.
Li Z, Han W, Zhang Y, Fu Q, Li J, Qin L, Dong R, Sun H, Deng Y, Yang L.Learning spatiotemporal dynamics with a pretrained generative model. Nat Mach Intell. 2024;6(12):1566–1579.
129.
He C, Liu Y.Time-resolved reconstruction of turbulent flows using linear stochastic estimation and sequential data assimilation. Phys Fluids. 2020;32(7):Article 075106.
130.
Buchta DA, Laurence SJ, Zaki TA.Assimilation of wall-pressure measurements in high-speed flow over a cone. J Fluid Mech. 2022;947:R2.
131.
Shu D, Li Z, Farimani AB.A physics-informed diffusion model for high-fidelity flow field reconstruction. J Comput Phys. 2023;478:Article 111972.
132.
Cai S, Mao Z, Wang Z, et al.Physics-informed neural networks (PINNs) for fluid mechanics: A review. Acta Mech Sinica. 2021;37(12):1727–1738.
133.
Erichson NB, Mathelin L, Yao Z, Brunton SL, Mahoney MW, Kutz JN.Shallow neural networks for fluid flow reconstruction with limited sensors. Proc A. 2020;476(2238):20200097.
134.
Zuo K, Ye Z, Zhang W, Yuan X, Zhu L.Fast aerodynamics prediction of laminar airfoils based on deep attention network. Phys Fluids. 2023;35(3):037127.
135.
Solera-Rico A, Sanmiguel Vila C, Gómez-López M, Wang Y, Almashjary A, Dawson ST, Vinuesa R.β-Variational autoencoders and transformers for reduced-order modelling of fluid flows. Nat Commun. 2024;15(1):1361.
136.
Fukami K, Fukagata K, Taira K.Machine-learning-based spatio-temporal super resolution reconstruction of turbulent flows. J Fluid Mech. 2021;909:A9.
137.
Bao K, Zhang X, Peng W, et al.Deep learning method for super-resolution reconstruction of the spatio-temporal flow field. Adv Aerodyn. 2023;5(1):19.
138.
Kim H, Kim J, Won S, Lee C.Unsupervised deep learning for super-resolution reconstruction of turbulence. J Fluid Mech. 2021;910:A29.
139.
Li Q, Li X, Chen X, Yao W.A novel graph modeling method for GNN-based hypersonic aircraft flow field reconstruction. Eng Appl Comput Fluid Mech. 2024;18(1):2394177.
140.
Xu S, Sun Z, Huang R, Dilong G, Yang G, Ju S.A practical approach to flow field reconstruction with sparse or incomplete data through physics informed neural network. Acta Mech Sinica. 2023;39(3):Article 322302.
141.
Kong W, Liu H.Unified icing theory based on phase transition of supercooled water on a substrate. Int J Heat Mass Transf. 2018;123:896–910.
142.
Cao Y, Tan W, Wu Z.Aircraft icing: An ongoing threat to aviation safety. Aerosp Sci Technol. 2018;75:353–385.
143.
Tian S, Li R, Liu X, Wang J, Yu J, Xu S, Tian Y, Yang J, Zhang L.Inhibition of defect-induced ice nucleation, propagation, and adhesion by bioinspired self-healing anti-icing coatings. Research. 2023;6:0140.
144.
Zeng D, Li Y, Huan D, Liu H, Luo H, Cui Y, Zhu C, Wang J.Robust epoxy-modified superhydrophobic coating for aircraft anti-icing systems. Colloids Surf A Physicochem Eng Asp. 2021;628:Article 127377.
145.
Haikun Z, Shinan C, Yuanyuan Z.Anti-icing & icephobic mechanism and applications of superhydrophobic/ultra slippery surface. Progress in Chemistry. 2017;29(1):102–118.
146.
Lo TNH, Lee J, Hwang HS, et al.Nanoscale coatings derived from fluoroalkyl and PDMS alkoxysilanes on rough aluminum surfaces for improved durability and anti-icing properties. ACS Appl Nano Mater. 2021;4(7):7493–7501.
147.
Domingos R, Papadakis M, Zamora A.Computational methodology for bleed air ice protection system parametric analysis. AIAA Atmos Space Environ Conf. 2010;7834.
148.
Esmaeilifar E, Raj LP, Myong RS.Computational simulation of aircraft electrothermal de-icing using an unsteady formulation of phase change and runback water in a unified framework. Aerosp Sci Technol. 2022;130:Article 107936.
149.
Vertuccio L, De Santis F, Pantani R, Lafdi K, Guadagno L.Effective de-icing skin using graphene-based flexible heater. Compos Part B. 2019;162:600–610.
150.
Ha JH, Hong SK, Kim DY, Park S-H.Flexible carbon nanotube/polydimethylsiloxane composite for the de-icing of airplane wings. J Nanosci Nanotechnol. 2021;21(3):1779–1783.
151.
Xu H, Lu H, Wang JX, Luo P, Yu F, Feng J, Zhou T.Full life cycle deicing and efficient anti-icing surface on polymers with triple thermal conversion capability. Adv Mater. 2025;38(5):Article e14989.
152.
Zhang H, Zhang W, Jin Y, Wu C, Xu Z, Yang S, Gao S, Liu F, Xu W, Wang S, et al.Freezing droplet ejection by spring-like elastic pillars. Nat Chem Eng. 2024;1(12):765–773.
153.
Li K, Wang Q, Zhou X, et al.Electrothermal/Superhydrophobic anti-deicing coating with a sandwich structure based on micro-nanomaterials. ACS Appl Nano Mater. 2024;7(21):24847–24856.
154.
Lee SH, Kim J, Seong M, Kim S, Jang H, Park HW, Jeong HE.Magneto-responsive photothermal composite cilia for active anti-icing and de-icing. Compos Sci Technol. 2022;217:Article 109086.
155.
Jingxin W, Dachuan YU, Zaili Y, Rongying G, Chunling Z.Experimental investigation of super-hydrophobic/electro-thermal synergistically anti-icing/de-icing strategy in ice wind tunnel. Trans Nanjing Univ Aeronaut Astronaut. 2023;40(2):193–204.
156.
Dong Y.An application of deep neural networks to the in-flight parameter identification for detection and characterization of aircraft icing. Aerosp Sci Technol. 2018;77:34–49.
157.
Løw-Hansen B, Hann R, Johansen TA. UAV icing: Ice shedding detection method for an electrothermal de-icing system. In: AIAA Aviation 2022 Forum. AIAA; 2022.
158.
Suo W, Sun X, Zhang W, Yi X.Aircraft ice accretion prediction based on geometrical constraints enhancement neural networks. Int J Numer Methods Heat Fluid Flow. 2024;34(9):3542–3568.
159.
Abdelghany ES, Farghaly MB, Almalki MM, Sarhan HH, Essa ME-SM.Machine learning and iot trends for intelligent prediction of aircraft wing anti-icing system temperature. Aerospace. 2023;10(8):676.
160.
Zohuri B. Radar energy warfare and the challenges of stealth technology. Berlin: Springer; 2020.
161.
Selvanayagam M, Eleftheriades GV.Experimental demonstration of active electromagnetic cloaking. Phys Rev X. 2013;3(4):Article 041011.
162.
Schurig D, Mock JJ, Justice BJ, Cummer SA, Pendry JB, Starr AF, Smith DR.Metamaterial electromagnetic cloak at microwave frequencies. Science. 2006;314(5801):977–980.
163.
Soric JC, Chen PY, Kerkhoff A, Rainwater D, Melin K, Alù A.Demonstration of an ultralow profile cloak for scattering suppression of a finite-length rod in free space. New J Phys. 2013;15(3):Article 033037.
164.
Pendry JB, Schurig D, Smith DR.Controlling electromagnetic fields. Science. 2006;312(5781):1780–1782.
165.
Ni X, Wong ZJ, Mrejen M, Wang Y, Zhang X.An ultrathin invisibility skin cloak for visible light. Science. 2015;349(6254):1310–1314.
166.
Bai Y, Zhu S, Liang J, Xing R, Kong J.4D printing of magnetically responsive materials and their applications. Research. 2025;8:0847.
167.
Zong H, Yang D, Qian J.Chemical-mechanical co-design for scalable flexible perovskite manufacturing. Soft Sci. 2026;6:21.
168.
Qian B, Zhao H, Zhu X, Li P, Hong H, Chu H, Guo Y-X.Nanosecond-level time-domain coding metasurface for radar signal generation. Nat Commun. 2025;16(1):10651.
169.
Qian C, Zheng B, Shen Y, Jing L, Li E, Shen L, Chen H.Deep-learning-enabled self-adaptive microwave cloak without human intervention. Nat Photonics. 2020;14(6):383–390.
170.
Zhang XG, Sun YL, Yu Q, Cheng Q, Jiang WX, Qiu C-W, Cui TJ.Smart Doppler cloak operating in broad band and full polarizations. Adv Mater. 2021;33(17):2007966.
171.
Liao J, Ji C, Yuan L, Huang C, Wang Y, Peng J, Luo X.Polarization-insensitive metasurface cloak for dynamic illusions with an electromagnetic transparent window. ACS Appl Mater Interfaces. 2023;15(13):16953–16962.
172.
Cerveny M, Ford KL, Tennant A.Reflective switchable polarization rotator based on metasurface with PIN diodes. IEEE Trans Antennas Propag. 2020;69(3):1483–1492.
173.
Wen E, Yang X, Sievenpiper DF.Real-data-driven real-time reconfigurable microwave reflective surface. Nat Commun. 2023;14(1):7736.
174.
Xia C, Lu Z, Zhang Y, Tan J.Broadband high optical transparent intelligent metasurface for adaptive electromagnetic wave manipulation. Research. 2024;7:0334.
175.
Wang Z, Song L, Zhang X, Jing L, Wang Z, Chen H, Li M, Liao D.Integrating dynamic chiral radiation with full-polarization invisibility via cooperative metasurface ensembles. Adv Mater. 2026;38:Article e23247.
176.
Liang L, Yang X, Li C, Yu R, Zhang B, Yang Y, Ji G.MXene-enabled pneumatic multiscale shape morphing for adaptive, programmable and multimodal radar-infrared compatible camouflage. Adv Mater. 2024;36(24):2313939.
177.
Wu Z, Huang J, Zeng X.Dual magnetic particles modified carbon nanosheets in CoFe/co@NC heterostructure for efficient electromagnetic synergy. Soft Sci. 2024;4:42.
178.
Zheng B, Xiong X, Tang J, Zhang R.Intelligent reflecting surface-aided electromagnetic stealth against radar detection. IEEE Trans Signal Process. 2024;72:3438–3452.
179.
Sen K, Aksimsek S, Kara A.Dynamic RCS modeling and aspect angle analysis for highly maneuverable UAVs. Aerospace. 2024;11(9):775.
180.
Xu HX, Wang ZJ, Wang YZ, Shao Y, Zhang W, Gao H, Zhang C, Feng W, Qiu C, Zhang H.Intelligent metasurface cloak reaches a new plateau: AI-assisted surface engineering for self-adaptive supportive invisibility. Research. 2026;9:1130.
181.
Li F, Pan T, Li W, Peng Z, Guo D, Jia X, Hu T, Wang L, Wang W, Gao M, et al.Flexible intelligent microwave metasurface with shape-guided adaptive programming. Nat Commun. 2025;16(1):3161.
182.
Qian C, Jia Y, Wang Z, Chen J, Lin P, Zhu X, Li E, Chen H.Autonomous aeroamphibious invisibility cloak with stochastic-evolution learning. Adv Photonics. 2024;6(1):016001–016001.
183.
Dal Monte A, Castelli MR, Benini E. A retrospective of high-lift device technology. In: Proceedings of the Proceedings of World Academy of Science, Engineering and Technology, F. World Academy of Science, Engineering and Technology (WASET); 2012.
184.
Naor M, Adler N, Pinto GD, Dumanis A.Psychological safety in aviation new product development teams: Case study of 737 MAX airplane. Sustainability. 2020;12(21):8994.
185.
Kota S, Martins J. Flexfloil shape adaptive control surfaces-flight test and numerical results. In: Proceedings of 31st Congress of the International Council of the Aeronautical Sciences (ICAS 2018), Belo Horizonte, Brazil, F. ICAS; 2018.
186.
Cramer NB, Cellucci DW, Formoso OB, Gregg CE, Jenett BE, Kim JH, Lendraitis M, Swei SS, Trinh GT, Trinh KV, et al.Elastic shape morphing of ultralight structures by programmable assembly. Smart Mater Struct. 2019;28(5):Article 055006.
187.
Woods BKS, Bilgen O, Friswell MI.Wind tunnel testing of the fish bone active camber morphing concept. J Intell Mater Syst Struct. 2014;25(7):772–785.
188.
Nair NJ, Goza A.Bio-inspired variable-stiffness flaps for hybrid flow control, tuned via reinforcement learning. J Fluid Mech. 2023;956:R4.
189.
Gehrke A, Mulleners K.Highly deformable flapping membrane wings suppress the leading edge vortex in hover to perform better. Proc Natl Acad Sci USA. 2025;122(6):Article e2410833121.
190.
Martin S, Bhushan B.Modeling and optimization of shark-inspired riblet geometries for low drag applications. J Colloid Interface Sci. 2016;474:206–215.
191.
Zheng T, Liu J, Qin L, Lu S, Mawignon FJ, Ma Z, Hao L, Wu Y, An D, Dong G.Effect of dolphin-inspired transverse wave microgrooves on drag reduction in turbulence. Phys Fluids. 2024;36:015157.
192.
Wang Y, Zhang P, Liu Y, Zhao J, Lin J, Chen Y. Aerodynamic coefficients prediction via cross-attention fusion and physical-informed training. In: Proceedings of the AAAI Conference on Artificial Intelligence. AAAI; 2025. p. 869–876.
193.
Cai Z, Fan Z, Liu T, et al.Neural network model for predicting aerodynamic parameters of airfoils. J Aircr. 2025;1–16.
194.
Wang X, Qian W, Zhao T, Chen H, He L, Sun H, Tian Y.A generative design method of airfoil based on conditional variational autoencoder. Eng Appl Artif Intell. 2025;139:Article 109461.
195.
Kang YE, Lee D, Yee K. Physically interpretable airfoil parameterization using variational autoencoder-based generative modeling. In: AIAA SCITECH 2024 Forum. AIAA; 2024. p. 0685
196.
Liu Z, Niu X, Jiang L, Li X, Chen G.An intelligent experience learning framework for aerodynamic shape optimization with direct embedding of flow field features. Aerosp Sci Technol. 2025;164:110407.
197.
Hijazi S, Tolouei E.Bio-inspired surface texture fluid drag reduction using large eddy simulation. J Appl Fluid Mech. 2023;16(6):1175–1192.
198.
Ricco P, Skote M, Leschziner MA.A review of turbulent skin-friction drag reduction by near-wall transverse forcing. Prog Aerosp Sci. 2021;123:Article 100713.
199.
Wang D, Liu H.Dolphin-inspired skin microvibrations offer a novel pressure-dominated drag reduction mechanism. Bioinspir Biomim. 2025;20(6): https://doi.org/10.1088/1748-3190/ae1397
Year 2026 volume 9 Issue 6
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doi: 10.34133/research.1305
  • Receive Date:2026-01-06
  • Online Date:2026-10-16
  • Published:2026-06-20
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  • Received:2026-01-06
  • Revised:2026-05-12
  • Accepted:2026-05-12
Affiliations
    1State Key Laboratory of Intelligent Manufacturing Equipment and Technology, Huazhong University of Science and Technology, Wuhan 430074, China.
    2Research Center for Advanced Electronics Manufacturing, School of Mechanical Science and Engineering, Huazhong University of Science and Technology, Wuhan 430074, China.
    3Flexible Electronics Research Center, Huazhong University of Science and Technology, Wuhan 430074, China.

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表12种不同金属材料的力学参数
科
Family
属数
Number of
genus
种数
Number of
species
占总种数比例
Percentage of
total species (%)
属
Genus
种数
Number of
species
占总种数比例
Percentage of total
species (%)
鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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