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	<title>semi-active control &#8211; Science</title>
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	<title>semi-active control &#8211; Science</title>
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		<title>Neural Network Meets Sliding Mode Control to Tame Smart Vibration Isolators</title>
		<link>https://scienmag.com/neural-network-meets-sliding-mode-control-to-tame-smart-vibration-isolators/</link>
		
		<dc:creator><![CDATA[Blake Davidson]]></dc:creator>
		<pubDate>Sat, 10 Oct 2026 00:41:40 +0000</pubDate>
				<category><![CDATA[Science News]]></category>
		<category><![CDATA[adaptive control]]></category>
		<category><![CDATA[adaptive control of vibration isolators]]></category>
		<category><![CDATA[composite materials for vibration damping]]></category>
		<category><![CDATA[hybrid control systems for vibration damping]]></category>
		<category><![CDATA[hysteresis]]></category>
		<category><![CDATA[intelligent vibration mitigation in engineering]]></category>
		<category><![CDATA[machine learning in vibration control]]></category>
		<category><![CDATA[magnetic field]]></category>
		<category><![CDATA[magnetorheological elastomer]]></category>
		<category><![CDATA[magnetorheological elastomer vibration isolators]]></category>
		<category><![CDATA[neural network control for vibration suppression]]></category>
		<category><![CDATA[nonlinear dynamics]]></category>
		<category><![CDATA[PLOS One]]></category>
		<category><![CDATA[radial basis function neural network]]></category>
		<category><![CDATA[real-time adjustable elastomer isolators]]></category>
		<category><![CDATA[resonance]]></category>
		<category><![CDATA[resonance region vibration reduction]]></category>
		<category><![CDATA[semi-active control]]></category>
		<category><![CDATA[semi-active vibration isolation techniques]]></category>
		<category><![CDATA[sliding mode control]]></category>
		<category><![CDATA[sliding mode control in smart vibration isolators]]></category>
		<category><![CDATA[smart materials]]></category>
		<category><![CDATA[smart materials for vibration isolation]]></category>
		<category><![CDATA[vibration isolation]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=256718</guid>

					<description><![CDATA[Researchers combined a radial basis function neural network with sliding mode control to achieve up to 55.8 percent vibration reduction in a magnetorheological elastomer isolator across varying excitation frequencies and amplitudes.]]></description>
										<content:encoded><![CDATA[<p>Vibration is one of the quietest enemies of modern engineering. It rattles sensitive instruments in laboratories, fatigues aircraft components, degrades the ride quality of vehicles, and can push precision manufacturing equipment out of tolerance within moments. Engineers have long sought materials and control strategies that can absorb unwanted motion before it propagates through a structure. A study published in PLOS One by Kiran Katari, Umanath R. Poojary, Ananda Hegde, and Gangadharan K. V. reports a meaningful step forward in this field: a hybrid control scheme that couples a radial basis function neural network with a sliding mode controller to command a magnetorheological elastomer isolator, achieving a maximum vibration reduction of 55.8 percent near the resonance region under the investigated operating conditions.</p>
<p>The material at the heart of the work is the magnetorheological elastomer, or MRE, a class of smart composite in which micrometer-scale magnetic particles are suspended in an elastic polymer matrix. When an external magnetic field is applied, the particles align and interact, stiffening the material and shifting its effective stiffness and damping properties within milliseconds. This reversible, field-controlled behavior makes MREs attractive for semi-active vibration isolation, in which the isolator adjusts its own mechanical properties in real time rather than relying on a fixed spring-damper design or consuming large amounts of power like a fully active actuator. Because the device modifies an inherent property of its material rather than injecting energy into a structure, semi-active systems also carry inherent stability advantages that have made them popular in automotive suspensions, seismic protection, and machinery mounting.</p>
<p>Yet MREs bring a notorious complication: their behavior is strongly nonlinear and hysteretic. The relationship between the applied magnetic field, the deformation of the elastomer, and the resulting force does not follow a simple algebraic rule. Instead, the material&#8217;s response depends on its deformation history, and its stiffness changes with both field strength and the amplitude and frequency of vibration. A controller designed under one set of assumptions can perform poorly, or even destabilize the system, when excitation conditions change. This is precisely the challenge the research team set out to address, focusing on excitations whose frequency and amplitude vary over a realistic operating envelope.</p>
<p>The experimental platform described in the study is a purpose-built MRE isolator with an orthogonal magnetic flux configuration. In this arrangement, the magnetic field is directed perpendicular to the plane in which the elastomer is sheared or compressed, maximizing the interaction between the field and the embedded particles while making efficient use of the magnetic circuit. The team fabricated the isolator and then systematically characterized its dynamic behavior under harmonic excitation across a frequency range of 15 to 80 hertz. This range is significant for practical isolation problems, because it spans many resonant frequencies of machinery mounts, vehicle subframes, and structural components where vibration damage and comfort problems concentrate. Mapping the isolator&#8217;s response across this band revealed the frequency-dependent shifts in stiffness and damping that any controller would need to handle.</p>
<p>To exploit the material&#8217;s adaptability without falling victim to its unpredictability, the researchers designed a hybrid controller built from two complementary elements. The first is a radial basis function neural network, or RBF network, a machine learning architecture whose output is a weighted sum of responses from localized, bell-shaped basis functions distributed across the input space. Because each basis function responds strongly only to inputs near its center, RBF networks can approximate nonlinear, spatially varying relationships efficiently and can be trained or updated online. In this application, the network&#8217;s job is to learn and adaptively estimate the isolator&#8217;s nonlinearities and hysteresis as they manifest under changing vibration conditions, providing a continuously refined model of the plant that a fixed mathematical model could never supply.</p>
<p>The second element is the sliding mode controller, a robust control technique with a long pedigree in engineering practice. Sliding mode control drives the system&#8217;s state trajectory onto a deliberately chosen sliding surface, along which the desired dynamic behavior is guaranteed, and then holds it there using a discontinuous control action that is insensitive to matched uncertainties. Its strength is robustness: once on the sliding surface, the closed-loop system tolerates a defined class of modeling errors and disturbances. Its weakness is that aggressive switching can amplify noise and induce chattering, and it traditionally requires a reasonably accurate bound on system uncertainties. The hybrid design resolves this tension elegantly, with the neural network absorbing the burden of representing the nonlinear, hysteretic dynamics while the sliding mode framework guarantees stability and rejects residual disturbances.</p>
<p>The division of labor matters because vibration isolation is a moving target. As excitation frequency sweeps through the resonance region, the isolator&#8217;s transmissibility changes rapidly; as amplitude grows, hysteresis loops widen and effective damping shifts. A purely neural approach risks drifting toward inaccurate estimates when conditions move outside its training experience, while a purely sliding mode approach would demand conservative margins that sacrifice performance. By integrating the two, the controller adapts its internal estimate of the system in real time while the sliding mode law enforces stable tracking of the isolation objective. The researchers evaluated this architecture both in simulation and experimentally, providing converging lines of evidence that the scheme works not only on paper but on a physical device subjected to real harmonic excitation.</p>
<p>The headline result is the maximum vibration reduction of 55.8 percent achieved near the resonance region under the tested conditions, the operating point where conventional passive isolators typically struggle most. Near resonance, even modest input forces can produce large transmitted vibrations, so effective attenuation there is the gold standard for isolator performance. Equally important, the study reports that the semi-active MRE isolator maintained stable performance across the full range of investigated excitation frequencies, indicating that the hybrid controller did not merely optimize for one narrow condition but adapted gracefully as the excitation environment changed. Stable adaptive performance under varying frequency and amplitude is the property that distinguishes an engineering solution from a laboratory demonstration tuned to a single test case.</p>
<p>The implications extend across several industries. Automotive engineers could apply such isolators to engine mounts and suspension elements, where excitation frequency changes constantly with driving conditions. Aerospace and marine systems, which encounter broadband vibration from rotating machinery and fluid-structure interaction, could benefit from isolators that retune themselves without mechanical adjustment. Precision manufacturing and semiconductor fabrication equipment, which must sit motionless on floors that are never truly still, represent another natural application. In earthquake engineering, semi-active devices built on similar principles have already been explored for structural protection, and a controller that handles nonlinear material behavior robustly could strengthen the case for MRE-based seismic isolators. Because semi-active systems require only modest power to drive the magnetic field rather than to generate control forces, they remain practical for battery-backed or low-power installations.</p>
<p>The work also speaks to a broader trend in control engineering: the marriage of learning-based models with provably robust control laws. Purely data-driven controllers often struggle to offer formal guarantees, while classical robust controllers can be overly conservative when systems are too nonlinear for simple models. Hybrid architectures such as the one demonstrated here let each approach cover the other&#8217;s weaknesses, a pattern that is spreading through robotics, energy systems, and aerospace. For magnetorheological elastomers specifically, the study suggests that the material&#8217;s most daunting property, its hysteresis, can be converted from an obstacle into a managed characteristic. The authors position the framework as an effective solution for handling nonlinear dynamics and a route toward greater adaptability in smart vibration isolation systems. As smart materials mature and machine learning hardware becomes inexpensive enough to embed in everyday devices, the vision of structures that sense, decide, and quiet themselves in milliseconds moves closer to routine engineering practice, and this research offers a concrete, experimentally validated blueprint for how that quieting can be achieved.</p>
<p><strong>Subject of Research:</strong> Hybrid neural network and sliding mode control of a magnetorheological elastomer vibration isolator under variable excitation conditions</p>
<p><strong>Article Title:</strong> Hybrid RBF neural network–based sliding mode control for a magnetorheological elastomer isolator under variable frequency and amplitude excitations</p>
<p><strong>Article References:</strong> Katari, K., Poojary, U. R., Hegde, A., &amp; K. V., G. (2026). Hybrid RBF neural network–based sliding mode control for a magnetorheological elastomer isolator under variable frequency and amplitude excitations. <em>PLOS One, 21</em>(10), e0360069. <a href="https://doi.org/10.1371/journal.pone.0360069" rel="noopener noreferrer">https://doi.org/10.1371/journal.pone.0360069</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1371/journal.pone.0360069" rel="noopener noreferrer">10.1371/journal.pone.0360069</a></p>
<p><strong>Keywords:</strong> magnetorheological elastomer, vibration isolation, sliding mode control, radial basis function neural network, semi-active control, smart materials, hysteresis, nonlinear dynamics, adaptive control, resonance, magnetic field, PLOS One</p>
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		<post-id xmlns="com-wordpress:feed-additions:1">256718</post-id>	</item>
		<item>
		<title>Semi-Active Damper With Negative Stiffness Tames Earthquake Shaking Without Adding Peak Forces</title>
		<link>https://scienmag.com/semi-active-damper-with-negative-stiffness-tames-earthquake-shaking-without-adding-peak-forces/</link>
		
		<dc:creator><![CDATA[Violet Maxwell]]></dc:creator>
		<pubDate>Sat, 03 Oct 2026 19:19:05 +0000</pubDate>
				<category><![CDATA[Earth Science]]></category>
		<category><![CDATA[advanced seismic mitigation technologies]]></category>
		<category><![CDATA[base isolation]]></category>
		<category><![CDATA[base-isolated building protection]]></category>
		<category><![CDATA[bidirectional damping effects]]></category>
		<category><![CDATA[Earthquake damping systems]]></category>
		<category><![CDATA[Earthquake engineering]]></category>
		<category><![CDATA[energy dissipation]]></category>
		<category><![CDATA[energy dissipation during specific motion cycles]]></category>
		<category><![CDATA[equivalent linearization]]></category>
		<category><![CDATA[friction damper]]></category>
		<category><![CDATA[hysteresis]]></category>
		<category><![CDATA[innovative earthquake engineering devices]]></category>
		<category><![CDATA[laboratory testing of seismic dampers]]></category>
		<category><![CDATA[low-cycle loading]]></category>
		<category><![CDATA[microcontroller-based damper control]]></category>
		<category><![CDATA[negative stiffness]]></category>
		<category><![CDATA[negative stiffness dampers]]></category>
		<category><![CDATA[optimizing damping to prevent force amplification]]></category>
		<category><![CDATA[seismic energy dissipation]]></category>
		<category><![CDATA[seismic protection]]></category>
		<category><![CDATA[semi-active control]]></category>
		<category><![CDATA[STM32 microcontroller]]></category>
		<category><![CDATA[structural demand reduction during earthquakes]]></category>
		<category><![CDATA[Structural dynamics]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=231598</guid>

					<description><![CDATA[Researchers in China have built and tested a semi-active friction damper that dissipates seismic energy only during unloading, extending structural period without increasing peak damping forces.]]></description>
										<content:encoded><![CDATA[<p>Earthquake engineers have long faced an uncomfortable trade-off. The most straightforward way to protect a building from violent shaking is to add damping, converting seismic energy into heat before it can accumulate in the structure. Yet conventional dampers, whether viscous, friction-based, or metallic, resist motion in both directions of every cycle, and that bidirectional resistance can raise the peak forces the structure must carry. In base-isolated buildings especially, researchers have documented that excessive supplemental damping can amplify floor accelerations and structural demands rather than reduce them. A team at Beijing University of Technology, working with a colleague at Kunming University of Science and Technology, now reports a device designed to escape this dilemma: an Equivalent Negative Stiffness Friction Damper, or ENSFD, that dissipates energy only during half of each motion cycle. The work, published in the Bulletin of Earthquake Engineering, combines analytical modeling, microcontroller-based control, and laboratory testing into a single experimental validation of the concept.</p>
<p>The central idea is deceptively simple. In a force-displacement plot, one complete cycle of motion traces a loop through four quadrants: two where displacement and force share the same sign, and two where they oppose each other. The ENSFD is engineered to deliver substantial damping force only in the second and fourth quadrants, the unloading phases of the cycle, while remaining nearly passive during loading. Because the device never pushes back hard against the structure as it moves in the direction of the driving force, it does not increase the maximum damping force transmitted to the building. At the same time, the asymmetric resistance mimics the effect of negative stiffness, a property that, in structural dynamics, effectively lengthens the period of a structure and softens its response to ground motion. The result is a damper that reshapes the hysteresis loop rather than simply enlarging it, concentrating energy absorption where it does the most good and least harm.</p>
<p>To make this concept usable in engineering practice, the researchers needed a way to represent the nonlinear, half-cycle behavior of the damper with parameters that standard analysis tools can handle. They built a nonlinear single-degree-of-freedom model of the ENSFD and applied the method of slowly varying parameters, an analytical technique for deriving the steady-state response of systems whose properties change gradually over a cycle of motion. From this treatment they extracted equivalent linearization parameters, essentially a stiffness and a damping coefficient that capture the averaged effect of the device over a full oscillation. These equivalent parameters were then checked against direct time-history analysis, in which the full nonlinear equations are integrated step by step under recorded ground motions. The comparison confirmed that the simplified parameters reproduce the response accurately enough for design-level seismic analysis, giving engineers a practical bridge between an exotic nonlinear device and the linearized calculation methods embedded in building codes.</p>
<p>Turning the mathematics into hardware required a control system capable of recognizing, in real time, which phase of the motion cycle the structure is in. The team designed a semi-active ENSFD built around an STM32 microprocessor, a widely used embedded controller with enough speed and reliability for structural applications. The complete system has three cooperating subsystems: a signal acquisition system that measures the structural response, a control system that processes those signals and decides the operating state, and a variable friction execution system that adjusts the friction force accordingly. The controller must distinguish among loading, unloading, and the transitional moments when the direction of motion reverses, because the damper&#8217;s behavior differs fundamentally in each state. Getting this logic right is the difference between a device that dissipates energy selectively and one that degenerates into an ordinary friction damper.</p>
<p>The experimental program consisted of low-cycle reciprocating tests, the standard laboratory protocol for seismic devices, in which the damper is pushed back and forth through many cycles at controlled displacement amplitudes and frequencies. The measured hysteresis curves matched the theoretical expectations: the device provided substantial damping force during unloading while contributing little resistance during loading, producing the characteristic asymmetric loop that defines equivalent negative stiffness behavior. The three subsystems worked together effectively, with the controller making accurate judgments during loading, unloading, and the transitions between them. This is a notable achievement for a semi-active device, since misclassification of the motion state would corrupt the force profile and undermine the entire design rationale.</p>
<p>Beyond confirming the basic behavior, the tests revealed how the damper&#8217;s energy dissipation capacity depends on its operating conditions and internal parameters. The researchers found that energy dissipation is positively correlated with the loading displacement amplitude, which is intuitive, since larger strokes sweep out larger hysteresis loops, and positively correlated with the spring stiffness of the device&#8217;s internal components. It is negatively correlated with the loading frequency, meaning the damper absorbs somewhat less energy per cycle when driven faster. When the team ranked the influencing factors by their impact, the ordering was clear: loading amplitude mattered most, spring stiffness came second, and loading frequency had the least effect. For designers, this hierarchy is valuable because it indicates that the device&#8217;s performance is governed primarily by the seismic demand itself, with the tunable mechanical properties offering a secondary but meaningful degree of control.</p>
<p>The equivalent negative stiffness damping characteristics of the ENSFD serve two complementary functions. First, by effectively extending the structural period, the device shifts the building&#8217;s response away from the frequency content of the earthquake, reducing the accelerations transmitted into the superstructure. This is the same principle that underlies base isolation, but achieved here through a supplementary damping device rather than by modifying the isolation system itself. Second, the concentrated unloading-phase dissipation controls seismic responses without the penalty of increased maximum damping force that accompanies conventional dampers. The authors report that the equivalent parameters derived from their analytical treatment are suitable for engineering analysis, which means the device can be incorporated into standard response-spectrum and time-history workflows without requiring bespoke nonlinear modeling of every installation.</p>
<p>The study situates itself within a growing body of research on negative stiffness and semi-active seismic protection. Negative stiffness devices, including the well-known device developed by Sarlis, Pasala, Constantinou, Reinhorn, Nagarajaiah, and Taylor, and various quasi-zero-stiffness and magnetic spring concepts, aim to reduce apparent structural stiffness and amplify damping effectiveness. Semi-active resettable devices, explored by Chase, Mulligan, and colleagues and by Bobrow, Jabbari, and Thai, demonstrated that reshaping hysteretic behavior with controllable hardware can outperform passive damping. Earlier work by members of the present team, including half-cycle friction damping devices and double triangular damping devices with equivalent negative stiffness for base-isolated buildings, laid the groundwork for the current ENSFD. The new study advances this lineage by closing the loop: a full analytical model, an equivalent linearization scheme validated by time-history analysis, a working electronic control system, and experimental verification in a single coherent program.</p>
<p>The practical significance of the frequency and amplitude findings deserves emphasis. Real earthquakes are broadband, nonstationary signals, and a damper whose output varies strongly with excitation frequency could behave unpredictably across different ground motions. The ENSFD&#8217;s weakest sensitivity being to frequency suggests a degree of robustness that bodes well for real-world deployment, while the strong dependence on displacement amplitude means the device naturally scales its energy absorption with the severity of the response, dissipating more when the structure moves more and less when the motion is mild. That self-scaling behavior is characteristic of well-behaved seismic protective systems and simplifies the task of designing the device for a target performance objective.</p>
<p>Challenges remain before such devices appear in buildings. The laboratory tests were conducted under controlled low-cycle reciprocating loading rather than full-scale shaking table conditions, and long-term reliability of the variable friction mechanism, along with the durability of the sensing and control electronics during years of dormancy punctuated by rare earthquakes, will need further study. Nevertheless, the demonstration that an STM32-based control system can reliably identify loading states in real time, and that the resulting hysteresis behaves as theory predicts, moves the equivalent negative stiffness friction damper from concept toward practice. For a field searching for ways to add damping without adding force, a device that works only half the cycle, and works best when the shaking is worst, is an idea whose time may have come.</p>
<p><strong>Subject of Research:</strong> Semi-active negative stiffness friction dampers for seismic response control of structures</p>
<p><strong>Article Title:</strong> Experimental study and equivalent parameter analysis of a semi-active negative stiffness friction damper</p>
<p><strong>Article References:</strong> Li, W., Peng, L., &amp; Lai, Z. (2026). Experimental study and equivalent parameter analysis of a semi-active negative stiffness friction damper. <em>Bulletin of Earthquake Engineering</em>. <a href="https://doi.org/10.1007/s10518-026-02647-x" rel="noopener noreferrer">https://doi.org/10.1007/s10518-026-02647-x</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10518-026-02647-x" rel="noopener noreferrer">10.1007/s10518-026-02647-x</a></p>
<p><strong>Keywords:</strong> negative stiffness, friction damper, semi-active control, seismic protection, equivalent linearization, hysteresis, STM32 microcontroller, energy dissipation, base isolation, earthquake engineering, structural dynamics, low-cycle loading</p>
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