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  <front>
    <journal-meta><journal-id journal-id-type="publisher">MS</journal-id><journal-title-group>
    <journal-title>Mechanical Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">MS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Mech. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2191-916X</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/ms-17-313-2026</article-id><title-group><article-title>Review article: A review of control technologies for soft robots: from structural design to intelligent control</article-title><alt-title>A review of control technologies for soft robots</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Yu</surname><given-names>Huijun</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Lv</surname><given-names>Min</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Hu</surname><given-names>Bin</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zhang</surname><given-names>Yang</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-9889-2921</ext-link></contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Zhao</surname><given-names>Pengyuan</given-names></name>
          <email>zhaopengyuan@uestc.edu.cn</email>
        <ext-link>https://orcid.org/0000-0002-1645-191X</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>School of Mechanical and Electrical Engineering, University of Electronic Science and Technology of China, Chengdu 611731, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Thoracic Surgery Department, Sichuan Cancer Hospital and Institute, Chengdu, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Pengyuan Zhao (zhaopengyuan@uestc.edu.cn)</corresp></author-notes><pub-date><day>25</day><month>March</month><year>2026</year></pub-date>
      
      <volume>17</volume>
      <issue>1</issue>
      <fpage>313</fpage><lpage>332</lpage>
      <history>
        <date date-type="received"><day>29</day><month>October</month><year>2025</year></date>
           <date date-type="rev-recd"><day>8</day><month>January</month><year>2026</year></date>
           <date date-type="accepted"><day>24</day><month>January</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Huijun Yu et al.</copyright-statement>
        <copyright-year>2026</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://ms.copernicus.org/articles/ms-17-313-2026.html">This article is available from https://ms.copernicus.org/articles/ms-17-313-2026.html</self-uri><self-uri xlink:href="https://ms.copernicus.org/articles/ms-17-313-2026.pdf">The full text article is available as a PDF file from https://ms.copernicus.org/articles/ms-17-313-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e120">Soft robots, with flexible materials and biomimetic structures, show great potential in medical rehabilitation, the exploration of unstructured environments, and precision operations. However, their highly nonlinear, continuously deforming, and difficult-to-model characteristics pose significant challenges for control. This paper provides a systematic review of research progress in the field of soft robotics control: at the mechanical level, the combination of different biomimetic structures, materials, and actuation methods offers diverse motion patterns; kinematic and dynamic modeling methods encompass both classical physics-based theories and modern techniques; trajectory planning focuses on objectives such as obstacle avoidance and time optimization, as well as visual servoing; and control strategies summarize research progress in model-based control and model-free control. Despite significant achievements, soft robots still face challenges such as low drive efficiency and insufficient real-time performance. Future research should overcome these bottlenecks to advance the practical application of soft robots. This paper aims to provide technical references for researchers and promote further development in the field of soft robot control.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e132">Soft robots possess high levels of compliance, adaptability, and human–machine interaction safety, demonstrating significant application potential in fields such as medical rehabilitation, precision manipulation, disaster relief, and wearable devices. Compared to traditional rigid robots, soft robots are composed of flexible materials to adapt to complex environments through continuous deformation and achieve flexible movements similar to those of biological organisms. However, this compliance also poses significant challenges in modeling and control: highly nonlinear material properties, time-varying dynamic behavior, and continuous deformation across multiple degrees of freedom, making traditional robot control methods difficult to apply directly.</p>
      <p id="d2e135">With the rapid development of new materials, novel actuation methods, and intelligent control technologies, soft robots have transitioned from the laboratory to engineering applications, demonstrating unique value in fields such as healthcare, the exploration of unstructured environments, and industrial automation. Intuitive Surgical's Ion™ Robotic Endoluminal System received FDA approval in 2019. Its soft robotics catheter has an outer diameter of just 3.5 mm and is equipped with an imaging probe with an outer diameter of 1.7 mm for direct visualization (<xref ref-type="bibr" rid="bib1.bibx25" id="altparen.1"/>). The Marine Biological Laboratory in Woods Hole, USA, deployed a biomimetic jellyfish robot in the coastal waters off Massachusetts to monitor marine ecosystems (<xref ref-type="bibr" rid="bib1.bibx132" id="altparen.2"/>). During the COVID-19 pandemic, a team from Beihang University utilized a bare-hand, non-contact, interactive soft robotic arm for collecting throat swabs (<xref ref-type="bibr" rid="bib1.bibx61" id="altparen.3"/>).</p>
      <p id="d2e147">At the same time, the application of soft robots is also driving scientific and technological progress. Researchers at Harvard University proposed an inverse design framework to discover flexible mechanical metamaterials with target nonlinear dynamic responses (<xref ref-type="bibr" rid="bib1.bibx7" id="altparen.4"/>). Collaborating with the Max Planck Institute, Tongji University developed a pangolin-inspired robot featuring soft skin and hard scales, which can deform, roll, and deliver targeted heat inside the human body under magnetic actuation (<xref ref-type="bibr" rid="bib1.bibx103" id="altparen.5"/>). Researchers at the University of California, San Diego, created a lightweight quadruped soft robot that maintains system control and movement through pneumatic circuits and does not require any electronic devices for propulsion, marking an important step toward fully autonomous robots (<xref ref-type="bibr" rid="bib1.bibx20" id="altparen.6"/>).</p>
      <p id="d2e159">In recent years, soft robotics technology has gradually become a research hotspot, as evidenced by the number of published papers. Using the keyword “soft robotics”, a search in the Web of Science Core Collection yielded the number of papers related to soft robotics from 2000 to 2025, as shown in Fig. <xref ref-type="fig" rid="F1"/>. It can be seen that soft robotics began to enter the public eye only after 2013; since 2016, the number of related papers has increased approximately linearly with each passing year and has yet to reach its peak, demonstrating the vigorous development trend in the field of soft robotics.</p>

      <fig id="F1"><label>Figure 1</label><caption><p id="d2e167">The number of articles related to soft robotics from 2000 to 2025.</p></caption>
        <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f01.png"/>

      </fig>

      <p id="d2e176">A network analysis of 1237 papers was conducted using CiteSpace software, with the results shown in Fig. <xref ref-type="fig" rid="F2"/>. Based on the analysis of countries and institutions, the USA and China have the most extensive research content, followed by Japan, Switzerland, Italy, and England. Institutions such as the University of California System, the Chinese Academy of Sciences, ETH Domain, and Shanghai Jiao Tong University have made significant contributions to the field of soft robotics. Cluster analysis of keywords reflects the mainstream research directions in soft robotics: the design and manufacture of mechanisms and the selection of actuation methods, kinematic and dynamic modeling, control, and the application of data-driven methods in soft robotics.</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e183">Network analysis of soft robotics: <bold>(a)</bold> country analysis, <bold>(b)</bold> institution analysis, <bold>(c)</bold> keyword clustering analysis.</p></caption>
        <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f02.png"/>

      </fig>

      <p id="d2e201">This paper systematically reviews the research progress from mechanism design to advanced control methods around the core issues of soft robotics control. Section 2 reviews the structural design, materials, and actuators of robotic systems; Sect. 3 introduces kinematic and dynamic modeling techniques; Sect. 4 analyzes motion planning for soft robots; Sect. 5 compares the advantages and disadvantages of model-based and model-free control strategies; and Sect. 6 summarizes current challenges and outlines future development directions, aiming to provide guidance for further research in the field of soft robot control.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Mechanism</title>
      <p id="d2e212">The mechanism of soft robots includes structural design, materials, and actuators, which together determine the motion capability, environmental adaptability, and control strategies of robots. Typical mechanism cases are shown in Fig. <xref ref-type="fig" rid="F3"/>. The mechanism is not only the basis for modeling, planning, and control but also determines the upper limit of the robot's dynamic performance.</p>

      <fig id="F3" specific-use="star"><label>Figure 3</label><caption><p id="d2e219">Typical mechanism cases.</p></caption>
        <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f03.jpg"/>

      </fig>

<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Structural design</title>
      <p id="d2e235">The structural design of soft robots draws heavily on the morphology and movement mechanisms of biological organisms to achieve efficient, flexible, and environmentally adaptive movement. Typical biomimetic-inspired structures include octopus tentacles, earthworms/inchworms, vines, elephant trunks, and snakes. Table <xref ref-type="table" rid="T1"/> provides a comparative analysis of the motion characteristics, strengths, weaknesses, applicable scenarios, and control complexity of various soft robots with bio-inspired structures. Additionally, there are soft robots inspired by origami.</p>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e243">Comparison of soft robots with different bio-inspired structures.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:colspec colnum="7" colname="col7" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Bio-inspired</oasis:entry>
         <oasis:entry colname="col2">Structure</oasis:entry>
         <oasis:entry colname="col3">Motion</oasis:entry>
         <oasis:entry colname="col4">Strengths</oasis:entry>
         <oasis:entry colname="col5">Weaknesses</oasis:entry>
         <oasis:entry colname="col6">Applicable</oasis:entry>
         <oasis:entry colname="col7">Control</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">prototype</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">characteristics</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6">scenarios</oasis:entry>
         <oasis:entry colname="col7">complexity</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Octopus</oasis:entry>
         <oasis:entry colname="col2">Multi-layer</oasis:entry>
         <oasis:entry colname="col3">Bending, twisting,</oasis:entry>
         <oasis:entry colname="col4">High environmental</oasis:entry>
         <oasis:entry colname="col5">Weak load capacity,</oasis:entry>
         <oasis:entry colname="col6">Fine grasping,</oasis:entry>
         <oasis:entry colname="col7">High</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">tentacle</oasis:entry>
         <oasis:entry colname="col2">muscle tissue</oasis:entry>
         <oasis:entry colname="col3">elongation,</oasis:entry>
         <oasis:entry colname="col4">compliance, precise</oasis:entry>
         <oasis:entry colname="col5">complex modeling</oasis:entry>
         <oasis:entry colname="col6">operation in</oasis:entry>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">contraction</oasis:entry>
         <oasis:entry colname="col4">manipulation</oasis:entry>
         <oasis:entry colname="col5">control</oasis:entry>
         <oasis:entry colname="col6">confined spaces</oasis:entry>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Earthworm/</oasis:entry>
         <oasis:entry colname="col2">Segmented</oasis:entry>
         <oasis:entry colname="col3">Peristalsis,</oasis:entry>
         <oasis:entry colname="col4">Simple structure,</oasis:entry>
         <oasis:entry colname="col5">Slow movement</oasis:entry>
         <oasis:entry colname="col6">Pipeline/cavity</oasis:entry>
         <oasis:entry colname="col7">Medium</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">inchworm</oasis:entry>
         <oasis:entry colname="col2">soft-body</oasis:entry>
         <oasis:entry colname="col3">crawling</oasis:entry>
         <oasis:entry colname="col4">adaptable to narrow</oasis:entry>
         <oasis:entry colname="col5">speed, poor</oasis:entry>
         <oasis:entry colname="col6">inspection</oasis:entry>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">structure</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">environments</oasis:entry>
         <oasis:entry colname="col5">flexibility</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Vine</oasis:entry>
         <oasis:entry colname="col2">Extensible</oasis:entry>
         <oasis:entry colname="col3">Tip extension,</oasis:entry>
         <oasis:entry colname="col4">Strong extension</oasis:entry>
         <oasis:entry colname="col5">Path dependent,</oasis:entry>
         <oasis:entry colname="col6">Exploration,</oasis:entry>
         <oasis:entry colname="col7">Medium</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">soft-tube</oasis:entry>
         <oasis:entry colname="col3">climbing</oasis:entry>
         <oasis:entry colname="col4">capability, large</oasis:entry>
         <oasis:entry colname="col5">weak load-bearing</oasis:entry>
         <oasis:entry colname="col6">inspection</oasis:entry>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">structure</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">working range</oasis:entry>
         <oasis:entry colname="col5">capacity</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Elephant</oasis:entry>
         <oasis:entry colname="col2">Soft-rigid</oasis:entry>
         <oasis:entry colname="col3">Coiling, multi-</oasis:entry>
         <oasis:entry colname="col4">Strong load capacity,</oasis:entry>
         <oasis:entry colname="col5">Complex structure,</oasis:entry>
         <oasis:entry colname="col6">Industrial</oasis:entry>
         <oasis:entry colname="col7">High</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">trunk</oasis:entry>
         <oasis:entry colname="col2">hybrid</oasis:entry>
         <oasis:entry colname="col3">directional</oasis:entry>
         <oasis:entry colname="col4">high flexibility</oasis:entry>
         <oasis:entry colname="col5">large weight/volume</oasis:entry>
         <oasis:entry colname="col6">handling,</oasis:entry>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">structure</oasis:entry>
         <oasis:entry colname="col3">bending</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6">collaboration</oasis:entry>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Snake</oasis:entry>
         <oasis:entry colname="col2">Modular soft-</oasis:entry>
         <oasis:entry colname="col3">Undulation, lateral</oasis:entry>
         <oasis:entry colname="col4">Strong terrain</oasis:entry>
         <oasis:entry colname="col5">Limited movement</oasis:entry>
         <oasis:entry colname="col6">Inspection,</oasis:entry>
         <oasis:entry colname="col7">Medium-</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">body segments</oasis:entry>
         <oasis:entry colname="col3">motion, extension</oasis:entry>
         <oasis:entry colname="col4">adaptability, diverse</oasis:entry>
         <oasis:entry colname="col5">speed, weak dexterity</oasis:entry>
         <oasis:entry colname="col6">detection</oasis:entry>
         <oasis:entry colname="col7">high</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">movement modes</oasis:entry>
         <oasis:entry colname="col5"/>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e669">Octopus tentacles possess a unique muscle-connective tissue composite structure composed of longitudinal muscle, transverse muscle, and oblique connective tissue, enabling multi-degree-of-freedom motion without skeletal support, including bending, twisting, elongation, and contraction. Based on this principle, <xref ref-type="bibr" rid="bib1.bibx34" id="text.7"/> constructed a conical silicone continuum soft robot. <xref ref-type="bibr" rid="bib1.bibx79" id="text.8"/> achieved high-compliant multi-degree-of-freedom movement by simulating longitudinal muscles with linear chambers for bending and extension, spiral chambers for bidirectional twisting, and rigid rings to constrain radial deformation.</p>
      <p id="d2e679">Earthworms/inchworms achieve peristaltic movement through the periodic contraction and expansion of their segments. Their locomotion mechanism relies on the antagonistic action of circular muscles and longitudinal muscles, as well as friction regulation by body surface bristles.  <xref ref-type="bibr" rid="bib1.bibx102" id="text.9"/> designed an earthworm-like peristaltic structure composed of continuous silicone gel columns, with a uniform cylindrical cross-section that can undergo nonlinear axial stretching deformation, driven by segmented or continuous strain waves to achieve retrograde peristaltic propulsion. <xref ref-type="bibr" rid="bib1.bibx143" id="text.10"/> designed an inchworm-like soft structure composed of three segments of fiber-reinforced pneumatic muscles connected in series, with negative pressure suction cups integrated at both ends. Controlled bending and adhesion enable crawling, climbing, and transitional movements.</p>
      <p id="d2e688">Vine plants achieve climbing through apical growth and the spiral contraction of tendrils. Their movement relies on the synergistic regulation of tropism and phototropism. <xref ref-type="bibr" rid="bib1.bibx52" id="text.11"/> and <xref ref-type="bibr" rid="bib1.bibx43" id="text.12"/> both used thin-walled polyethylene tubes to construct vine-like soft robots, achieving tip extension and turning by releasing pre-stored segments via four sets of electromagnetic steering units.</p>
      <p id="d2e697">An elephant's trunk consists of approximately 150 000 muscle bundles, combining flexibility with load-bearing capacity. Its movement relies on hierarchical coordinated muscle contraction and the extensibility of skin folds. <xref ref-type="bibr" rid="bib1.bibx77" id="text.13"/> designed an elephant-trunk-like hybrid robot comprising a 6-degrees-of-freedom rigid skeleton and a 48-degrees-of-freedom soft hydrostatic segment in series, driven by an adjustable compliance matrix to achieve redundant degree-of-freedom coordination and end-effector interaction adjustment.</p>
      <p id="d2e703">Snakes leverage body bending and coordinated muscle contractions to demonstrate powerful locomotion capabilities, including serpentine, sidewinding, and concertina movements. <xref ref-type="bibr" rid="bib1.bibx112" id="text.14"/> proposed a modular 3D soft robotic snake, whose structure consists of three-segment, actively deformable pneumatic silicone modules connected in series. <xref ref-type="bibr" rid="bib1.bibx72" id="text.15"/> developed a modular soft robot that achieves a bidirectional crawling motion along the exterior of tubular structures through alternating grip and extension movements.</p>
      <p id="d2e712">Origami structures achieve programmable deformation through folding–unfolding mechanisms, with crease designs enabling various deformation modes, including unfolding, bending, and twisting. <xref ref-type="bibr" rid="bib1.bibx9" id="text.16"/> proposed a cable-free caterpillar-inspired biomimetic robot based on a triangular origami spring skeleton and coupled drive, with internal and external magnets, achieving adjustable structural stiffness and multi-modal motion through programmable crease patterns. <xref ref-type="bibr" rid="bib1.bibx60" id="text.17"/> were inspired by the Kresling origami structure and proposed an untethered soft robot capable of crawling in pipelines, with a high contraction ratio. <xref ref-type="bibr" rid="bib1.bibx23" id="text.18"/> proposed a vacuum-driven parallel continuum robot, utilizing soft–hard hybrid 3D-printed self-sensing origami linkages to achieve high load capacity, multi-modal motion, and precise closed-loop control.</p>
      <p id="d2e724">These structural designs fully leverage the flexible multi-joint characteristics of the biological world. Compared to rigid robotic arms, soft robots significantly increase degrees of freedom and flexibility in their structure. However, at the same time, this multi-joint design also introduces considerable challenges and uncertainties in motion and mechanical control.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Materials</title>
      <p id="d2e736">Soft robots primarily utilize elastic materials such as hydrogels, and dielectric elastomers or composite materials (<xref ref-type="bibr" rid="bib1.bibx114" id="altparen.19"/>), which exhibit high extensibility, low Young's modulus, and excellent energy absorption properties, making them well suited to soft robotics. Additionally, common materials include shape memory materials and magnetoresponsive materials.</p>
      <p id="d2e742">Hydrogels are soft hydrophilic materials composed of a network of hydrophilic polymers and a large amount of water. Their unique properties stem from the interactions between polymer chains and water molecules. Based on their stimulus response characteristics, hydrogels can be classified into various types, including temperature responsive (<xref ref-type="bibr" rid="bib1.bibx22" id="altparen.20"/>), light responsive (<xref ref-type="bibr" rid="bib1.bibx30" id="altparen.21"/>), and magnetically responsive (<xref ref-type="bibr" rid="bib1.bibx101 bib1.bibx119" id="altparen.22"/>). Hydrogels exhibit excellent biocompatibility and mechanical properties similar to those of the environment, but they have low mechanical strength and slow response speeds.</p>
      <p id="d2e754">Dielectric elastomers are a class of polymer materials with high dielectric constants and excellent elastic deformation capabilities, whose operational mechanism is based on the Maxwell stress effect. When an external electric field is applied to both sides of an electrically polarized dielectric elastomer film, the material compresses in the thickness direction and expands in the planar direction, resulting in significant electromechanical deformation. Dielectric elastomers have fast response speeds and high energy density, and can directly convert electrical energy into mechanical energy, making them widely used in soft robots (<xref ref-type="bibr" rid="bib1.bibx53 bib1.bibx37 bib1.bibx57" id="altparen.23"/>). However, they also face challenges such as high driving voltages and insufficient long-term cycling stability.</p>
      <p id="d2e760">Shape memory alloys are a class of metallic materials with unique shape memory effects and superelasticity, capable of restoring their preset shapes under external stimuli. The most commonly used shape memory alloy is nickel-titanium-based alloy, which exhibits excellent shape recovery rates, biocompatibility, and long cycle lifetimes. However, it suffers from slow response speeds and low driving efficiency (<xref ref-type="bibr" rid="bib1.bibx4 bib1.bibx82" id="altparen.24"/>).</p>
      <p id="d2e767">Magnetoresponsive materials are a class of functional materials that generate controllable mechanical responses under external magnetic fields. Common types include magnetorheological materials (including magnetorheological fluids and magnetorheological elastomers), magnetic composite materials (where magnetic particles are dispersed in polymers/hydrogels; <xref ref-type="bibr" rid="bib1.bibx129 bib1.bibx17 bib1.bibx101 bib1.bibx31" id="altparen.25"/>), and liquid magnetic materials (such as ferromagnetic fluids; <xref ref-type="bibr" rid="bib1.bibx46" id="altparen.26"/>). Magnetoresponsive materials possess wireless remote control and precise positioning control capabilities, demonstrating significant application potential in fields such as micro-robots and medical robots.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>Actuators</title>
      <p id="d2e784">The actuators of soft robots are closely related to their motion performance and modeling control. Common actuators include pneumatic drive, cable drive, and tendon drive.</p>
      <p id="d2e787">Pneumatic drive induces deformation of the elastomer by regulating the air pressure within a sealed cavity. When the internal air pressure increases, the elastic cavity expands and deforms; when the air pressure decreases, the material's elastic recovery force causes it to contract (<xref ref-type="bibr" rid="bib1.bibx94 bib1.bibx5" id="altparen.27"/>). Typical pneumatic actuators employ a multi-layer elastic material structure with a complex network of air channels embedded internally (<xref ref-type="bibr" rid="bib1.bibx78 bib1.bibx65" id="altparen.28"/>). Enhanced designs incorporate fiber reinforcement layers within the elastic matrix to control deformation direction and improve mechanical performance (<xref ref-type="bibr" rid="bib1.bibx118 bib1.bibx15" id="altparen.29"/>). Recent research has also developed vacuum-driven variants, which offer advantages such as energy efficiency, safety, and rapid response (<xref ref-type="bibr" rid="bib1.bibx63 bib1.bibx23 bib1.bibx105" id="altparen.30"/>).</p>
      <p id="d2e802">The cable drive system consists of a high-strength fiber cable core and a low-friction outer sheath. A servo motor winds the flexible cable, converting rotational motion into axial tensile force on the flexible skeleton, thereby generating bending/contraction (<xref ref-type="bibr" rid="bib1.bibx50" id="altparen.31"/>). Multiple cables working together can achieve complex movements (<xref ref-type="bibr" rid="bib1.bibx76 bib1.bibx120" id="altparen.32"/>). It features high force transmission efficiency and precise motion control (<xref ref-type="bibr" rid="bib1.bibx34" id="altparen.33"/>) but can only transmit tensile force, not compressive force, and suffers from friction losses and hysteresis effects (<xref ref-type="bibr" rid="bib1.bibx146" id="altparen.34"/>).</p>
      <p id="d2e817">Tendon-driven systems are based on biomimetic design, mimicking biological muscle-tendon systems. They achieve bidirectional motion through the synergistic action of opposing tendon pairs, with changes in tendon tension regulating joint stiffness (<xref ref-type="bibr" rid="bib1.bibx94" id="altparen.35"/>). Common tendon materials include high-strength fibers, steel wires (<xref ref-type="bibr" rid="bib1.bibx24" id="altparen.36"/>), and nylon threads (<xref ref-type="bibr" rid="bib1.bibx126" id="altparen.37"/>). By controlling the contraction length or tension of single or multiple tendons, the structure generates motions such as bending and deformation  (<xref ref-type="bibr" rid="bib1.bibx90 bib1.bibx91" id="altparen.38"/>). While tendon-driven systems exhibit highly biomimetic motion patterns and enable variable stiffness adjustment (<xref ref-type="bibr" rid="bib1.bibx122" id="altparen.39"/>), they suffer from slow dynamic response and complex control requirements.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Modeling of soft robots</title>
      <p id="d2e844">Soft robots are constructed from flexible materials, with mechanical designs enabling complex and supple movements. However, their ability to undergo continuous deformation and possess infinite degrees of freedom poses significant challenges for describing and predicting robotic behavior. Conventional modeling approaches for rigid robots cannot be directly applied. However, researchers have achieved the transition from discrete joints to continuum modeling by geometric mapping. This transforms rigid joints into deformable links, increasing the dimensionality to extend the limited joint degrees of freedom to the multiple degrees of freedom of a soft robot, along with other techniques. Soft robot modeling includes kinematic modeling and dynamic modeling. By establishing mathematical models to describe the motion characteristics and mechanical properties of soft robots, a foundation is provided for the design of robot planning and control strategies.</p>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Kinematic modeling</title>
      <p id="d2e854">Kinematic models are used to describe geometric relationships and the motion characteristics of robots, serving as the foundation for trajectory planning and position control. The continuous deformation characteristics of soft robots render traditional Denavit–Hartenberg (DH) parameter methods inapplicable, necessitating alternative methods such as the segment curvature assumption or Cosserat rod theory.</p>
<sec id="Ch1.S3.SS1.SSS1">
  <label>3.1.1</label><title>Segment curvature assumption</title>
      <p id="d2e864">The piecewise constant curvature (PCC) model divides the soft robot into multiple circular segments with constant curvature, to describe its configuration using curvature, arc length, and twist angle. Kinematic modeling divides the robot space into the actuator space, configuration space, and task space, establishing mappings between these spaces through the functions <inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:mi>g</mml:mi><mml:mo>(</mml:mo><mml:mo>⋅</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>(</mml:mo><mml:mo>⋅</mml:mo><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, as shown in Fig. <xref ref-type="fig" rid="F4"/>. The PCC method is highly efficient in computation, physically interpretable, and adaptable to multi-segment structures, making it widely adopted. For example, <xref ref-type="bibr" rid="bib1.bibx120" id="text.40"/> used the PCC method to solve the kinematic mapping relationship. <xref ref-type="bibr" rid="bib1.bibx130" id="text.41"/> used this method to establish forward and inverse kinematic models for particle-interference soft robots. <xref ref-type="bibr" rid="bib1.bibx35" id="text.42"/> further introduced Lagrange equations to model soft components, while also considering elastic deformation caused by gravitational loads. <xref ref-type="bibr" rid="bib1.bibx21" id="text.43"/> proposed a new procedure that relies on the PCC method to simplify highly complex hyper-redundant soft robotic arm models.</p>

      <fig id="F4"><label>Figure 4</label><caption><p id="d2e912">Kinematic mapping relationship (<xref ref-type="bibr" rid="bib1.bibx120" id="altparen.44"/>).</p></caption>
            <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f04.png"/>

          </fig>

      <p id="d2e924">The PCC model can only provide limited deformation modes because it simply divides the entire soft robotic arm into several segments, with the curvature of each segment treated as a constant. To address this issue, <xref ref-type="bibr" rid="bib1.bibx78" id="text.45"/> proposed a kinematic model based on the multi-curvature method; <xref ref-type="bibr" rid="bib1.bibx12" id="text.46"/> studied a new method for modeling the kinematics of variable-curvature soft robots based on the minimum energy method. They broke through the geometric limitations of PCC, significantly improving the accuracy and adaptability of soft robot motion description. Models established based on the segmented curvature assumption are intuitive, highly generalizable, and computationally efficient, making them suitable for scenarios requiring high real-time performance and where the robot's bending deformation is relatively smooth. However, their ability to describe complex deformations is limited, and the idealized assumptions inherently introduce model errors, resulting in finite precision.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS2">
  <label>3.1.2</label><title>Cosserat rod theory</title>
      <p id="d2e941">Cosserat rod theory provides a rigorous mechanical framework for the continuous deformation of soft robots. Its core idea is to treat soft structures as elastic rods capable of withstanding stretching, shearing, bending, and torsion, describing their kinematic and dynamic behavior using continuum mechanics methods. The Cosserat rod theory assumes that the length of the linear model is much greater than the cross-sectional radius, meaning that the soft robotic arm is treated as a spatial curve. As shown in Fig. <xref ref-type="fig" rid="F5"/>a, there are two coordinate systems: the global coordinate system <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> and the local coordinate system <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M5" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula> represents the position of a point on the curve. Among them, <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> constitutes the cross-section at that point, and <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the normal vector of that cross-section. It is important to note that <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">d</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is not necessarily in the same direction as the tangent to the curve; when they are different, it indicates that there is shear at <inline-formula><mml:math id="M9" display="inline"><mml:mi>s</mml:mi></mml:math></inline-formula>.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e1108">Geometric descriptions of the Cosserat rod theory and the pseudo-rigid body model: <bold>(a)</bold> Cosserat rod theory (<xref ref-type="bibr" rid="bib1.bibx48" id="altparen.47"/>), <bold>(b)</bold> pseudo-rigid body model (<xref ref-type="bibr" rid="bib1.bibx110" id="altparen.48"/>).</p></caption>
            <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f05.png"/>

          </fig>

      <p id="d2e1129">The configuration of a Cosserat rod is described by the position vector <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">p</mml:mi><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> and the rotation matrix <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mi mathvariant="bold">R</mml:mi><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, while deformation is described by the strain vector <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:mi mathvariant="bold-italic">ξ</mml:mi><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo>[</mml:mo><mml:mi mathvariant="bold-italic">v</mml:mi><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="bold-italic">u</mml:mi><mml:mo>(</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:msup><mml:mo>]</mml:mo><mml:mi>T</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M13" display="inline"><mml:mi mathvariant="bold-italic">v</mml:mi></mml:math></inline-formula> is the linear strain and <inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="bold-italic">u</mml:mi></mml:math></inline-formula> is the angular strain:

                  <disp-formula specific-use="gather" content-type="numbered"><mml:math id="M15" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E1"><mml:mtd><mml:mtext>1</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="bold-italic">v</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi mathvariant="bold">R</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="bold-italic">p</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">e</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd><mml:mtext>2</mml:mtext></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="bold-italic">u</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi mathvariant="bold">R</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="bold">R</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>s</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d2e1288">Based on Cosserat theory, <xref ref-type="bibr" rid="bib1.bibx24" id="text.49"/> described the kinematics of soft robotic hands, and <xref ref-type="bibr" rid="bib1.bibx126" id="text.50"/> developed a model to estimate the shape of soft robots, with accurate prediction results and support for 6 degrees of freedom strain and large deformations. However, the computational complexity is high, making it unsuitable for real-time control and difficult to widely adopt. Based on the Cosserat rod theory, the kinematic model for soft robots offers high accuracy, supports complex deformation modes, and features clear physical meaning of parameters along with strong generalizability. It is well suited to high-precision control and shape prediction under complex constraints. However, the equations are complex, resulting in high computational cost for numerical solutions, making it difficult to achieve real-time control.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS3">
  <label>3.1.3</label><title>Pseudo-rigid body model</title>
      <p id="d2e1305">The pseudo-rigid body model is a method of simplifying a flexible continuum into an equivalent mechanism consisting of rigid links and flexible joints, widely applied in the kinematic modeling of soft robots. Its core idea is to approximate continuous deformation using discrete rigid elements and virtual springs, balancing computational efficiency and accuracy. Figure <xref ref-type="fig" rid="F5"/>b illustrates a single-segment continuum robot with two sub-segments. The flexible main body of each sub-segment is decomposed into a series of pseudo-rigid links (B), connected via torsion springs (black circles), with flexible deformation simulated by virtual springs. The driving tendons are equivalent to a series of pseudo-rigid prismatic joints (C). Tendons are connected to disks (D) via passive rotational joints (red circles), and disks are connected to pseudo-rigid links via fixed joints (black dots).</p>
      <p id="d2e1310">Based on the above principles, <xref ref-type="bibr" rid="bib1.bibx138" id="text.51"/> proposed a parameter estimation paradigm coupling an analytical modeling method based on pseudo-rigid body modeling with the logarithmic decay method. <xref ref-type="bibr" rid="bib1.bibx110" id="text.52"/> introduced a new modeling method based on pseudo-rigid body modeling, constraint analysis of multi-body systems, and Lagrange multipliers. Similarly, <xref ref-type="bibr" rid="bib1.bibx140" id="text.53"/> proposed a method based on a unified rigid-flexible model, modeling kinematics, and dynamics by treating soft joints as flexible universal joints. The pseudo-rigid body model is computationally efficient, has simple parameter identification, and is highly compatible with traditional robot control algorithms, making it suitable for embedded control and the rapid development of soft robots. However, it has significant prediction errors in dynamic responses, difficulties in modeling environmental interactions, and insufficient accuracy for large deformations, making it unsuitable for high-precision control scenarios.</p>
</sec>
<sec id="Ch1.S3.SS1.SSS4">
  <label>3.1.4</label><title>Others</title>
      <p id="d2e1331">Neural networks represent a data-driven approach that bypasses complex physical modeling processes by establishing direct mapping from driving inputs to motion outputs. They are inherently suited to approximating high-dimensional nonlinear mappings and do not require the explicit formulation of geometric or mechanical equations, significantly lowering the barrier to modeling. This makes them well suited to soft robots, which exhibit large deformations, hysteresis, and nonlinearities. Using neural networks, <xref ref-type="bibr" rid="bib1.bibx76" id="text.54"/> derived an artificial learning rule to approximate the kinematic model of a soft robot. <xref ref-type="bibr" rid="bib1.bibx10" id="text.55"/> constructed a motion model for a soft robotic fish by training a neural network on data collected from visual sensors. Based on a multi-layer perceptron neural network, <xref ref-type="bibr" rid="bib1.bibx108" id="text.56"/> proposed a method for learning the inverse kinematics of a soft origami continuum robot. <xref ref-type="bibr" rid="bib1.bibx36" id="text.57"/> introduced an iterative self-improving learning strategy based on long short-term memory networks for end-to-end inverse kinematics modeling. However, neural networks are highly data dependent and incur high data acquisition costs. They also suffer from poor interpretability and reliability, and their generalizability is limited by the scope of the training data.</p>
      <p id="d2e1346">In addition, researchers have also developed kinematic models for soft robots based on various theoretical frameworks, including free Euler–Bernoulli beam theory (<xref ref-type="bibr" rid="bib1.bibx6" id="altparen.58"/>), discretized elastic beam theory (<xref ref-type="bibr" rid="bib1.bibx62" id="altparen.59"/>), continuum mechanics (<xref ref-type="bibr" rid="bib1.bibx65" id="altparen.60"/>), and Jacobian matrix theory (<xref ref-type="bibr" rid="bib1.bibx40" id="altparen.61"/>), and by employing methods such as the force density method (<xref ref-type="bibr" rid="bib1.bibx62" id="altparen.62"/>), Euler arc spline approximation (<xref ref-type="bibr" rid="bib1.bibx90" id="altparen.63"/>), transformation matrix method (<xref ref-type="bibr" rid="bib1.bibx134 bib1.bibx96" id="altparen.64"/>), absolute nodal coordinate formulation (<xref ref-type="bibr" rid="bib1.bibx38" id="altparen.65"/>), finite element analysis (<xref ref-type="bibr" rid="bib1.bibx3 bib1.bibx145 bib1.bibx66 bib1.bibx56" id="altparen.66"/>), and spatial curve integration (<xref ref-type="bibr" rid="bib1.bibx13" id="altparen.67"/>).</p>
</sec>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Dynamic modeling</title>
      <p id="d2e1389">Dynamic models study the relationship between force and motion, i.e., what kind of force needs to be applied to a physical object to achieve a certain motion. They reveal the dynamic relationship between driving inputs and motion responses, providing a theoretical framework for force/position hybrid control, impedance control, and other control methods.</p>
<sec id="Ch1.S3.SS2.SSS1">
  <label>3.2.1</label><title>Cosserat rod theory</title>
      <p id="d2e1399">In addition to kinematic models, Cosserat rods are widely used in the dynamic modeling of soft robots. For example, <xref ref-type="bibr" rid="bib1.bibx1" id="text.68"/> developed a dynamic Cosserat rod model for soft robots; <xref ref-type="bibr" rid="bib1.bibx94" id="text.69"/> used dynamic Cosserat rod theory to comprehensively address various aspects of deformation, including bending, torsion, shear, and stretching; and <xref ref-type="bibr" rid="bib1.bibx58" id="text.70"/> employed an optimized Cosserat rod model for the kinematic and dynamic analysis of multi-section magnetic soft robots. Furthermore, <xref ref-type="bibr" rid="bib1.bibx136" id="text.71"/> combined screw theory with Cosserat theory to establish a dynamic model for soft robotic arms; <xref ref-type="bibr" rid="bib1.bibx70" id="text.72"/> employed an accurate predictive model coupled with a large-deformation Cosserat rod model and low Reynolds number flow; and <xref ref-type="bibr" rid="bib1.bibx121" id="text.73"/> proposed and analyzed a method to incorporate contact modeling into the widely used shooting-based Cosserat rod implementation. Cosserat rod-based dynamic modeling provides a physically consistent and high-precision simulation and control foundation for soft robots, but it also faces challenges such as complex contact modeling and difficulties in real-time control.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS2">
  <label>3.2.2</label><title>Finite element method</title>
      <p id="d2e1430">The basic idea of the finite element method (FEM) is to discretize a continuum into a finite number of elements connected by nodes, approximate continuous field variables (including displacement, strain, and stress) using piecewise interpolation functions, and ultimately solve a system of algebraic equations to achieve high-precision simulation of soft robotics' nonlinear large deformations and dynamic behavior. The mapping from coordinate space to finite element space is shown in Fig. <xref ref-type="fig" rid="F6"/>. Here, <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">q</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the simplified coordinate of the rigid robot, <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">q</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the maximum coordinate of the rigid probe, <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">q</mml:mi><mml:mi mathvariant="normal">n</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the node coordinate of the non-rigid body, and <inline-formula><mml:math id="M19" display="inline"><mml:mi>M</mml:mi></mml:math></inline-formula> is the mapping function.</p>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e1477">From coordinate space (left) to FEM space (right) (<xref ref-type="bibr" rid="bib1.bibx16" id="altparen.74"/>).</p></caption>
            <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f06.png"/>

          </fig>

      <p id="d2e1489">Based on the FEM for modeling soft components, <xref ref-type="bibr" rid="bib1.bibx16" id="text.75"/> achieved the propagation of forces and displacements between soft and rigid models through a mapping mechanism. <xref ref-type="bibr" rid="bib1.bibx54" id="text.76"/> introduced an orthogonal decomposition algorithm to significantly reduce the size of large robot models obtained from the FEM, while preserving their structural and stability characteristics. Subsequently, they (<xref ref-type="bibr" rid="bib1.bibx55" id="altparen.77"/>) used the proper orthogonal decomposition algorithm to reduce the order of the model and proposed an iterative training method using radial basis function networks to construct the robot model. <xref ref-type="bibr" rid="bib1.bibx104" id="text.78"/> controlled the dynamic changes in vacuum pressure in each segment based on numerical simulations from the FEM. Similarly, <xref ref-type="bibr" rid="bib1.bibx17" id="text.79"/> proposed a magnetic soft robot simulation framework using the material point method, which inherently simulates self-collisions between model regions and can capture the effects of forces in non-uniform magnetic fields. The FEM possesses high-precision modeling capabilities and can accurately fit the nonlinear characteristics of materials (<xref ref-type="bibr" rid="bib1.bibx144" id="altparen.80"/>), but it is computationally expensive, lacks real-time performance, and faces inherent challenges such as mesh distortion under large deformations.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS3">
  <label>3.2.3</label><title>Lagrange method</title>
      <p id="d2e1519">As an important tool in analytical mechanics, the Lagrange method establishes the system's dynamical equations from an energy perspective, making it suitable for addressing dynamical problems in multi-degree-of-freedom, nonlinear systems such as soft robots. The Lagrange equations are:</p>
      <p id="d2e1522"><disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M20" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="normal">d</mml:mi><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mover accent="true"><mml:mi mathvariant="bold-italic">q</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi mathvariant="bold-italic">q</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">Q</mml:mi><mml:mi mathvariant="normal">ext</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M21" display="inline"><mml:mi>L</mml:mi></mml:math></inline-formula> is the Lagrange function given by <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:mi>L</mml:mi><mml:mo>=</mml:mo><mml:mi>T</mml:mi><mml:mo>-</mml:mo><mml:mi>V</mml:mi></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M23" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> is kinetic energy, <inline-formula><mml:math id="M24" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> is potential energy, <inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="bold-italic">q</mml:mi></mml:math></inline-formula> is the generalized coordinate, and <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">Q</mml:mi><mml:mi mathvariant="normal">ext</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the non-conservative force.</p>
      <p id="d2e1634">Using the Lagrange method, <xref ref-type="bibr" rid="bib1.bibx129" id="text.81"/> derived the dynamic motion equations for soft robots; and <xref ref-type="bibr" rid="bib1.bibx43" id="text.82"/> developed a dynamic model for plant-inspired growing robots and employed model predictive control to regulate task space position, orientation, and interaction forces. Building on this, <xref ref-type="bibr" rid="bib1.bibx127" id="text.83"/> introduced a PCC assumption to propose a simplified dynamic model for an underwater soft robotic arm, while accounting for the nonlinear viscoelasticity of soft materials; <xref ref-type="bibr" rid="bib1.bibx59" id="text.84"/> combined the Lagrangian equations, PCC method, and generalized coordinates to establish a nonlinear dynamic model for soft robots; and <xref ref-type="bibr" rid="bib1.bibx98" id="text.85"/> derived a singularity-free dynamic model based on the Lagrangian formula and the Taylor series expansion of a two-segment continuum robot. The Lagrangian method is widely used in the dynamic modeling of soft robots due to its energy consistency and nonlinear adaptability, but it also faces challenges such as high computational complexity and difficulties in online control and modeling non-conservative forces.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS4">
  <label>3.2.4</label><title>Koopman operator theory</title>
      <p id="d2e1661">Koopman operator theory (<xref ref-type="bibr" rid="bib1.bibx47" id="altparen.86"/>) provides a data-driven global linearization method for nonlinear soft robot systems, achieving the high-precision prediction of linear models by mapping nonlinear dynamics to an infinite-dimensional function space. Consider the following discrete nonlinear dynamic system with control inputs:

              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M27" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">u</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M28" display="inline"><mml:mi mathvariant="bold-italic">x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M29" display="inline"><mml:mi mathvariant="bold-italic">u</mml:mi></mml:math></inline-formula> represent the state and input of the system, respectively. The Koopman operator advances the evolution of observables through dynamic flows:

              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M30" display="block"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mi mathvariant="italic">ψ</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="italic">ψ</mml:mi><mml:mo>∘</mml:mo><mml:mi>f</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> denotes the discrete-time Koopman operator and <inline-formula><mml:math id="M32" display="inline"><mml:mo>∘</mml:mo></mml:math></inline-formula> denotes the composite operation of <inline-formula><mml:math id="M33" display="inline"><mml:mi mathvariant="italic">ψ</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M34" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>. <inline-formula><mml:math id="M35" display="inline"><mml:mi mathvariant="italic">ψ</mml:mi></mml:math></inline-formula> is referred to as an observable function in the elevated space. This equation can be further expressed as

              <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M36" display="block"><mml:mrow><mml:mo>(</mml:mo><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mi mathvariant="italic">ψ</mml:mi><mml:mo>)</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">u</mml:mi><mml:mi>k</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi mathvariant="italic">ψ</mml:mi><mml:mo>∘</mml:mo><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="italic">ψ</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">x</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="bold-italic">u</mml:mi><mml:mrow><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1855">The above equation indicates that the application of the infinite-dimensional Koopman operator transforms the system from a finite-dimensional nonlinear state space to an infinite-dimensional linear function space.</p>
      <p id="d2e1858">Based on the Koopman operator, <xref ref-type="bibr" rid="bib1.bibx115" id="text.87"/> proposed a modeling and control scheme for soft robots. <xref ref-type="bibr" rid="bib1.bibx32" id="text.88"/> utilized a data-driven learning method based on Koopman operator theory for modeling and introduced the concept of the static Koopman operator as a pre-gain term in optimal control. <xref ref-type="bibr" rid="bib1.bibx33" id="text.89"/> proposed a data-driven modeling framework for globally linearizing highly nonlinear dynamical systems in an elevated infinite-dimensional state space. <xref ref-type="bibr" rid="bib1.bibx135" id="text.90"/> proposed a data-driven mode decomposition algorithm using Koopman operator theory and finite-dimensional approximations of extended dynamics to estimate shape deformations of soft robots. Koopman operator theory offers a novel modeling perspective for nonlinear soft robot systems through global linearization and data-driven approaches, but it faces challenges such as difficulties in designing observation functions and high data requirements.</p>
</sec>
<sec id="Ch1.S3.SS2.SSS5">
  <label>3.2.5</label><title>Others</title>
      <p id="d2e1881">Neural networks, with their robust nonlinear fitting capability and data-driven nature, are not only applicable to the kinematic modeling of soft robots but are also frequently used for dynamic modeling. <xref ref-type="bibr" rid="bib1.bibx128" id="text.91"/> investigated dynamic analysis and response prediction of a hydraulic soft arm using long short-term memory neural networks. <xref ref-type="bibr" rid="bib1.bibx39" id="text.92"/> proposed a hybrid physics-learning modeling method based on the absolute nodal coordinate formulation and multi-layer neural networks. <xref ref-type="bibr" rid="bib1.bibx123" id="text.93"/> combined neural networks with a compact particle swarm optimization algorithm to predict the response of composite material booms. <xref ref-type="bibr" rid="bib1.bibx68" id="text.94"/>, inspired by the pseudo-rigid-body method, introduced a physics-informed neural ordinary differential equation to construct the model. <xref ref-type="bibr" rid="bib1.bibx26" id="text.95"/> utilized deep neural networks to capture the complexity of the dynamics, determining the input–output functional relationship between control inputs and robot trajectories. However, training neural networks requires a large amount of precise data support and demands that the data sufficiently cover the system's motion space. Otherwise, predictions may become distorted, and their black-box nature further leads to poor interpretability.</p>
      <p id="d2e1899">Numerous scholars have also achieved dynamic modeling of soft robots from other perspectives. <xref ref-type="bibr" rid="bib1.bibx111" id="text.96"/> adopted the passive motion paradigms, <xref ref-type="bibr" rid="bib1.bibx34" id="text.97"/> employed the extended Hamilton principle, <xref ref-type="bibr" rid="bib1.bibx19" id="text.98"/> established models based on equilibrium principles with prior deformation configurations, <xref ref-type="bibr" rid="bib1.bibx141" id="text.99"/> implemented an implicit integration methods based on curved beam models, <xref ref-type="bibr" rid="bib1.bibx117" id="text.100"/> combined virtual power principles and a spring-damper-fluid equivalent method, <xref ref-type="bibr" rid="bib1.bibx67" id="text.101"/> used the minimum norm method, <xref ref-type="bibr" rid="bib1.bibx124" id="text.102"/> utilized the absolute nodal coordinate formulation, <xref ref-type="bibr" rid="bib1.bibx51" id="text.103"/> and <xref ref-type="bibr" rid="bib1.bibx75" id="text.104"/> both used the reduced-order method, and <xref ref-type="bibr" rid="bib1.bibx41" id="text.105"/> extended the comprehensive dynamic gradient calculation method for rigid-linked systems to achieve the dynamic modeling of soft robots.</p>
</sec>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Planning</title>
      <p id="d2e1943">After establishing a model to predict the motion of soft robots, it is also necessary to determine which motions should be executed to accomplish the task and which leads to the problem of planning in complex environments. Planning enables robots to make autonomous decisions rather than simply executing preprogrammed fixed actions. Trajectory planning allows robots to adapt to complex and dynamic environments while ensuring safety and reliability; meanwhile, vision is commonly used to achieve trajectory tracking for soft robots.</p>
<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Trajectory planning</title>
      <p id="d2e1953">Trajectory planning determines the efficiency, safety, and stability of task execution. In addition to meeting movement constraints and obstacle avoidance requirements, its planning objectives typically include time optimization, shortest path, and minimum energy consumption.</p>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>Obstacle avoidance</title>
      <p id="d2e1963">Safely avoiding obstacles in dynamic or complex environments is a fundamental requirement of trajectory planning, making obstacle avoidance a research focus in soft robotics planning. <xref ref-type="bibr" rid="bib1.bibx109" id="text.106"/> developed an improved dynamic window algorithm based on fuzzy logic for intelligent obstacle avoidance, as shown in Fig. <xref ref-type="fig" rid="F7"/>a. <xref ref-type="bibr" rid="bib1.bibx50" id="text.107"/> investigated robot–obstacle collision avoidance under constrained conditions, as shown in Fig. <xref ref-type="fig" rid="F7"/>b. <xref ref-type="bibr" rid="bib1.bibx86" id="text.108"/> used a genetic algorithm to demonstrate trajectory planning for a manipulator in an environment with fixed obstacles. <xref ref-type="bibr" rid="bib1.bibx131" id="text.109"/> proposed a compliant obstacle avoidance algorithm that evaluates robot interaction states based on contact forces. <xref ref-type="bibr" rid="bib1.bibx98" id="text.110"/> achieved active obstacle avoidance for soft robots using an imitation learning framework and human demonstrations.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e1988">Implementation results of the trajectory planning algorithm: <bold>(a)</bold> automatic navigation in static and obstacle-laden virtual environments (<xref ref-type="bibr" rid="bib1.bibx109" id="altparen.111"/>), <bold>(b)</bold> principle of collision avoidance (<xref ref-type="bibr" rid="bib1.bibx50" id="altparen.112"/>), <bold>(c)</bold> trajectory planning in crowded environments (<xref ref-type="bibr" rid="bib1.bibx29" id="altparen.113"/>), <bold>(d)</bold> RRT<sup>∗</sup>-based trajectory planning, <bold>(e)</bold> RRT-based trajectory planning (<xref ref-type="bibr" rid="bib1.bibx95" id="altparen.114"/>).</p></caption>
            <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f07.jpg"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>Time optimal</title>
      <p id="d2e2042">The goal of time optimal is to minimize the time required for the robot to move from the start to the goal while satisfying constraints such as dynamics and joint velocity/acceleration/torque limits. This is particularly useful for tasks requiring rapid responses, such as dynamic interactions or emergency operations. <xref ref-type="bibr" rid="bib1.bibx84" id="text.115"/> solved for purely time-optimal trajectories under given constraints and compared them with trajectories optimized for joint angles and stiffness. The results showed that while the former reduced time, it sacrificed interaction safety and compliance.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <label>4.1.3</label><title>Shortest path</title>
      <p id="d2e2057">Shortest-path planning aims to compute the minimal geometric route from start to goal and is particularly useful in space-constrained or cluttered environments. Shortest-path planning methods are efficient and well suited to static environments but perform poorly in dynamic scenarios and often neglect robot dynamics. Common methods include the Dijkstra algorithm, A<sup>∗</sup> algorithm, and RRT<sup>∗</sup> algorithm.</p>
      <p id="d2e2078"><xref ref-type="bibr" rid="bib1.bibx29" id="text.116"/> proposed a path planning method for deformable soft robots in cluttered environments. Their approach used 3D Voronoi diagrams and the Dijkstra algorithm to compute optimal paths, balancing costs between robot size, shape variations, and path length, as shown in Fig. <xref ref-type="fig" rid="F7"/>c. <xref ref-type="bibr" rid="bib1.bibx133" id="text.117"/> and <xref ref-type="bibr" rid="bib1.bibx113" id="text.118"/> introduced an obstacle avoidance path planning algorithm based on the A<sup>∗</sup> algorithm and experimentally validated the effectiveness of the path planning algorithm and trajectory tracking control. <xref ref-type="bibr" rid="bib1.bibx95" id="text.119"/> proposed a novel path planning method with constant curvature constraints using the RRT<sup>∗</sup> algorithm. The implementation results are shown in Fig. <xref ref-type="fig" rid="F7"/>d and e: gray rectangles represent obstacles; pink and green nodes denote start and goal points; blue lines connect nodes; and orange and red paths represent the trajectories before and after the removal of unnecessary nodes, respectively. It can be seen that, compared with the standard RRT algorithm, the RRT<sup>∗</sup> algorithm has path optimality, can generate shorter paths, and has strong exploration capabilities, although its computation time and complexity are high.</p>
</sec>
<sec id="Ch1.S4.SS1.SSS4">
  <label>4.1.4</label><title>Minimum energy consumption</title>
      <p id="d2e2134">The objective of minimum energy consumption is to minimize power usage or actuator energy expenditure, making it particularly suitable for long-term operations or energy-constrained scenarios such as deep-sea exploration and inspection. <xref ref-type="bibr" rid="bib1.bibx6" id="text.120"/> treated electrical energy minimization as the primary optimization target, employing model-based predictive control strategies to compute actuator input signals. <xref ref-type="bibr" rid="bib1.bibx116" id="text.121"/> adopted a nonlinear constrained optimization approach to minimize total energy consumption during soft robot tasks. While energy-minimized planning enhances efficiency and reduces mechanical wear, it relies heavily on precise modeling and involves significant computational overhead.</p>
</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Visual sensing</title>
      <p id="d2e2152">To ensure precise motion along predefined trajectories, vision systems are frequently utilized for trajectory tracking in soft robots. The visual module primarily executes three functions: environmental perception, including target object recognition (<xref ref-type="bibr" rid="bib1.bibx105" id="altparen.122"/>), obstacle detection, and map reconstruction; pose estimation, which uses visual information to reconstruct the soft robot's shape and pose in real time (<xref ref-type="bibr" rid="bib1.bibx76 bib1.bibx79 bib1.bibx57" id="altparen.123"/>); and motion correction, which adjusts control signals with visual feedback to prevent path deviation and improve accuracy (<xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx131 bib1.bibx49" id="altparen.124"/>). Notably, <xref ref-type="bibr" rid="bib1.bibx98" id="text.125"/> developed a novel vision-based force sensor to achieve closed-loop grasping force control for soft grippers.</p>
      <p id="d2e2167">Data-driven methods are widely used in visual perception for soft robots. <xref ref-type="bibr" rid="bib1.bibx142" id="text.126"/> proposed a bending-sensing algorithm based on image preprocessing and deep learning, training a convolutional neural network with multi-task learning to obtain the bending state of a soft robotic finger. <xref ref-type="bibr" rid="bib1.bibx137" id="text.127"/> trained a convolutional neural network to map visual feedback to the tip pose of the actuator. <xref ref-type="bibr" rid="bib1.bibx93" id="text.128"/> combined a traditional neural network with B-spline curves, capturing external visual images and mapping them to the robot's shape. Additionally, <xref ref-type="bibr" rid="bib1.bibx106" id="text.129"/> used a recurrent neural network to estimate the pose of a proprioceptive bending sensor. <xref ref-type="bibr" rid="bib1.bibx69" id="text.130"/> also implemented multi-modal tactile sensing for a soft robotic finger based on a neural network model. <xref ref-type="bibr" rid="bib1.bibx97" id="text.131"/> employed machine learning to convert signals captured by low-cost sensors into shape parameters of a soft robot.</p>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>Control</title>
      <p id="d2e2200">Building upon the previously discussed mechanism, modeling, and planning of soft robots, control should unify and coordinate all elements to enable the robot to execute its intended motions with precision and robustness in real-world environments while compensating for uncertainties and disturbances. Soft robots, characterized by compliant materials, extremely high degrees of freedom, and strong nonlinearities, are difficult to model. Although researchers have achieved the kinematic and dynamic modeling of soft robots using various methods to facilitate the design of model-based controllers, factors such as simplifying assumptions, model simplifications, parametric uncertainties, and external disturbances lead to unmodeled dynamics within the system, posing challenges for control system design. Consequently, control methods that do not rely on models are increasingly being introduced for soft robot control. Some relevant research on both model-based and model-free control are summarized in Fig. <xref ref-type="fig" rid="F8"/>. It lists specific soft robot control methods from the past 5 years, arranged chronologically. This reveals a growing trend of embedding data-driven approaches into traditional feedback frameworks to form hybrid controllers. Model-based control and model-free control coexist, each with its own advantages and limitations. In terms of application outcomes, enhancing stability and improving tracking accuracy are the two most common performance objectives, reflecting the key challenges in soft robot control.</p>

      <fig id="F8" specific-use="star"><label>Figure 8</label><caption><p id="d2e2207">Relevant research on soft robot control.</p></caption>
        <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f08.png"/>

      </fig>

<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Model-based control</title>
      <p id="d2e2223">Model-based control utilizes internal models to predict robot behavior, thereby computing the control commands needed to achieve desired objectives. This approach offers high control efficiency and eliminates the need for a large number of sample data. Although soft robots present significant modeling challenges and exhibit unmodeled dynamics, researchers have made dedicated efforts and improvements within the model-based control framework. Through technical approaches such as robust control that accounts for uncertainties, adaptive control with online parameter adjustment, and control strategies that integrate data-driven methods, controllers capable of resisting, adapting to, and learning from unmodeled dynamics have been designed, thereby optimizing control performance.</p>

      <fig id="F9" specific-use="star"><label>Figure 9</label><caption><p id="d2e2228">System block diagrams of relevant research on soft robot control: <bold>(a)</bold> multi-rate hierarchical controller (<xref ref-type="bibr" rid="bib1.bibx45" id="altparen.132"/>), <bold>(b)</bold> PID controller with a saturated integral action (<xref ref-type="bibr" rid="bib1.bibx87" id="altparen.133"/>), <bold>(c)</bold> adaptive neural network controller (<xref ref-type="bibr" rid="bib1.bibx136" id="altparen.134"/>), <bold>(d)</bold> PID and iterative learning controller (<xref ref-type="bibr" rid="bib1.bibx133" id="altparen.135"/>).</p></caption>
          <graphic xlink:href="https://ms.copernicus.org/articles/17/313/2026/ms-17-313-2026-f09.png"/>

        </fig>

      <p id="d2e2262"><xref ref-type="bibr" rid="bib1.bibx99" id="text.136"/> established the dynamic model of the soft robot based on the absolute nodal coordinate formulation and solved the driving force through inverse dynamics. <xref ref-type="bibr" rid="bib1.bibx54" id="text.137"/> combined the reduced-order finite element model with the equivalent input disturbance method to achieve coordinated feedforward-feedback-disturbance compensation control, suppressing modeling uncertainties and disturbances. <xref ref-type="bibr" rid="bib1.bibx125" id="text.138"/> proposed a control strategy based on finite element dynamics models, combining feedforward with PID feedback to enhance the system's disturbance rejection capability and tracking accuracy. <xref ref-type="bibr" rid="bib1.bibx87" id="text.139"/> established the dynamic model of the underactuated soft robot and used the P-satI-D shape regulation control law with saturated integral term, which did not require precise stiffness parameters and could suppress constant disturbances. The block diagram of the control structure is shown in Fig. <xref ref-type="fig" rid="F9"/>b. They (<xref ref-type="bibr" rid="bib1.bibx88" id="altparen.140"/>) also proposed a PD+ feedback control method with gravity compensation to improve control performance. <xref ref-type="bibr" rid="bib1.bibx111" id="text.141"/> combined the pseudo-rigid-body model of the soft robot with elastic statics to achieve compensation for the connecting rod deformation. By implementing feedforward compensation based on the model and combining it with methods such as PID to suppress disturbances, relatively high control accuracy can be achieved in slow-tracking tasks. However, such methods require an accurate model. Otherwise, control precision may be difficult to guarantee. Additionally, their robustness to unmodeled dynamics and sudden external disturbances is limited.</p>
      <p id="d2e2286"><xref ref-type="bibr" rid="bib1.bibx44" id="text.142"/> established an articulated joint dynamic model for the soft robot and proposed an impedance control scheme, effectively reducing actuator torque requirements during impact. <xref ref-type="bibr" rid="bib1.bibx64" id="text.143"/> compared the torque estimation performance of musculoskeletal models and inverse dynamic models, and computed control commands through an admittance controller. <xref ref-type="bibr" rid="bib1.bibx40" id="text.144"/> utilized a pseudo-rigid-body model and employed an admittance force control strategy to achieve safe, compliant, and low-energy-consumption control performance. <xref ref-type="bibr" rid="bib1.bibx45" id="text.145"/> combined the developed nonlinear finite element model with admittance control to execute robot sensing and control at high rates. The control block diagram is shown in Fig. <xref ref-type="fig" rid="F9"/>a. Impedance/admittance control adjusts the dynamic interaction between the robot and the environment to achieve compliant operation, enhancing system compatibility and safety. It is well suited to tasks involving human-robot interaction or contact with uncertain environments. However, its performance relies on the tuning of impedance/admittance parameters, and its control accuracy is relatively low.</p>
      <p id="d2e2302"><xref ref-type="bibr" rid="bib1.bibx81" id="text.146"/> proposed a robust control method based on a linear time-invariant system model, integrating singular value decomposition decoupling, PI control, and anti-windup compensation. <xref ref-type="bibr" rid="bib1.bibx100" id="text.147"/> addressed robots with system uncertainties and input saturation, achieving constrained shape control through a dynamic model and a sliding-mode controller. <xref ref-type="bibr" rid="bib1.bibx80" id="text.148"/> utilized the dynamic model of the soft robot, employing super-twisting sliding-mode control and an input estimator to achieve position control of the end effector. <xref ref-type="bibr" rid="bib1.bibx14" id="text.149"/> proposed a sliding-mode controller based on a super-twisting extended state observer to robustly control the robot's attitude within a finite time, building upon the dynamic model. Robust control is capable of addressing model uncertainties, parameter variations, and external disturbances, ensuring convergence within a finite time frame while maintaining the stability and precision of the control system. It is suitable for tasks with strong environmental disturbances and high demands on control accuracy and stability. However, its controller design typically requires prior knowledge of the uncertainty bounds, and to guarantee robustness, the controller gains are often set relatively high, which may lead to potential control input chattering.</p>
      <p id="d2e2316"><xref ref-type="bibr" rid="bib1.bibx71" id="text.150"/> established a pseudo-rigid-body dynamic model for the modular soft robot and employed an adaptive backstepping sliding-mode controller to mitigate the effects of model uncertainties and external disturbances. <xref ref-type="bibr" rid="bib1.bibx2" id="text.151"/> developed a dynamic model based on the constant curvature assumption and proposed an adaptive sliding-mode controller to achieve robust curvature tracking control against external disturbances and parametric uncertainties. <xref ref-type="bibr" rid="bib1.bibx75" id="text.152"/> combined a decoupled reduced-order dynamic model with a robust fractional-order controller to realize adaptive motion control of the soft robot under model uncertainties. <xref ref-type="bibr" rid="bib1.bibx98" id="text.153"/> proposed a virtual reference adaptive control strategy based on visuo-tactile sensing to achieve closed-loop adaptive force control. Adaptive control enables the online estimation and compensation of unknown or slowly time-varying system parameters, thereby reducing reliance on the accuracy of the initial model. It performs particularly well in scenarios where system parameters are uncertain or difficult to identify precisely offline. However, the proofs of stability and convergence for adaptive control are complex. Furthermore, its convergence speed may be slow, making it difficult to track abrupt parameter changes, and its effectiveness in handling unmodeled dynamics remains limited.</p>
      <p id="d2e2330"><xref ref-type="bibr" rid="bib1.bibx8" id="text.154"/> constructed data-driven linear and nonlinear dynamic models based on Koopman operator theory and accomplished trajectory tracking control for the soft robot through a model predictive controller. <xref ref-type="bibr" rid="bib1.bibx85" id="text.155"/> established an RNN-based forward dynamic model and proposed a continual learning control method incorporating elastic weight consolidation to accurately control the soft manipulator under varying load conditions. <xref ref-type="bibr" rid="bib1.bibx27" id="text.156"/> established a soft-arm kinematic model based on the segmented constant curvature assumption. By employing the <inline-formula><mml:math id="M43" display="inline"><mml:mi>Q</mml:mi></mml:math></inline-formula>-learning reinforcement learning method, they achieved motion control with attitude constraints, satisfying task requirements without the need for motion planning. <xref ref-type="bibr" rid="bib1.bibx42" id="text.157"/> established a closed-loop control framework based on reinforcement learning and proprioceptive self-sensing, training the control policy through a physical simulation model to achieve coordinated movement of a multi-segment soft robot. <xref ref-type="bibr" rid="bib1.bibx35" id="text.158"/> proposed a data-driven model predictive control method with input mapping based on a system state-space model, reducing the impact of model inaccuracies. <xref ref-type="bibr" rid="bib1.bibx136" id="text.159"/> established a piecewise discrete dynamic model, designed an adaptive controller based on a radial basis function neural network, and combined it with a Lyapunov function to achieve precise trajectory tracking under motion constraints. The system block diagram is shown in Fig. <xref ref-type="fig" rid="F9"/>c. <xref ref-type="bibr" rid="bib1.bibx139" id="text.160"/> also designed an adaptive learning control method based on a radial basis function neural network on the basis of a reduced-order dynamic model of a soft trunk robot, achieving accurate trajectory tracking of the end effector. <xref ref-type="bibr" rid="bib1.bibx74" id="text.161"/> proposed a control algorithm combining a fractional-order sliding surface and deep reinforcement learning based on a nonlinear dynamic model to achieve trajectory tracking and suppress oscillations. <xref ref-type="bibr" rid="bib1.bibx135" id="text.162"/> compared analytical models and Koopman data-driven models, and realized trajectory tracking using a linear quadratic regulator combined with an unscented Kalman filter. Experiments showed that the system incorporating the Koopman model exhibited superior tracking accuracy and robustness. <xref ref-type="bibr" rid="bib1.bibx73" id="text.163"/> adopted an improved particle swarm optimization algorithm to optimize PID parameters for high-precision control, based on a data-driven control model for a pneumatic soft robot. <xref ref-type="bibr" rid="bib1.bibx28" id="text.164"/> improved the disturbance rejection capability and control accuracy of the soft robot based on a dynamic model and a particle swarm optimization algorithm. <xref ref-type="bibr" rid="bib1.bibx83" id="text.165"/> used iterative learning control to compensate for model uncertainties and correct errors online based on a flexible rod dynamic model, achieving high-precision control. Combining kinematic or dynamic models with data-driven methods for control can effectively balance tracking accuracy and generalization capabilities, offering flexible performance suitable for tasks requiring high precision, robustness, and adaptive capability. However, this approach involves higher design complexity and still requires a certain number of data for training and learning.</p>
      <p id="d2e2379">Model-based control features clear theoretical foundations and strong interpretability. Under ideal conditions – accurate models, known environments, and sufficient computational resources – it can achieve high-performance control of soft robots. However, due to its heavy reliance on models and the difficulty in obtaining accurate ones, this approach exhibits limited robustness against model uncertainties and unmodeled dynamics. Additionally, since most models are developed for specific soft robots and are influenced by factors such as structure and materials, and the controllers are designed based on these models, the generality and transferability of such controllers are often poor.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Model-free control</title>
      <p id="d2e2391">Model-free control does not rely on prior models. Its core principle involves directly learning the mapping relationship between states and actions from data, enabling it to handle complex tasks. Such controllers inherently avoid the series of issues caused by modeling difficulties, meaning they are insensitive to model uncertainties and exhibit strong adaptability and robustness.</p>
      <p id="d2e2394"><xref ref-type="bibr" rid="bib1.bibx18" id="text.166"/> proposed a data-driven control method based on Bayesian optimization and Gaussian processes, which online learned gait controller parameters and combined transfer learning to achieve adaptive control across different task spaces, improving data efficiency. and generalization. <xref ref-type="bibr" rid="bib1.bibx133" id="text.167"/> proposed a model-free closed-loop control system combining PID and iterative learning to achieve end-effector position tracking and improve the response speed for repetitive tasks. The control system block diagram is shown in Fig. <xref ref-type="fig" rid="F9"/>d. <xref ref-type="bibr" rid="bib1.bibx92" id="text.168"/> proposed a model-agnostic deep reinforcement learning control method, achieving rapid adaptation and generalization through Sim2Real transfer learning, significantly outperforming traditional PID control. <xref ref-type="bibr" rid="bib1.bibx107" id="text.169"/> combined feedforward control based on probabilistic model predictive control and feedback control based on a non-parametric learning method, realizing hybrid force/position tracking for the robot. It adapted to unknown environments without requiring precise modeling. <xref ref-type="bibr" rid="bib1.bibx89" id="text.170"/> proposed a self-tuning PID control method based on online identification using a discrete wavelet neural network, achieving gain adaptive adjustment and trajectory tracking relying only on position measurements.</p>
      <p id="d2e2413">Model-free control circumvents the challenges of modeling but introduces its own set of issues, including low sample efficiency, lengthy training times, difficulties in debugging, and poor interpretability. Therefore, in practical applications, the choice between model-based and model-free control often involves trade-offs among factors such as stability, accuracy, and safety.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d2e2425">This paper provides a detailed review of recent research progress in soft robotics regarding structure and actuation, kinematics, and dynamics modeling, as well as control and algorithms. It is observed that current research still faces several challenges. On the one hand, there is a trade-off between modeling accuracy and real-time control capability. High-precision modeling methods, such as the Cosserat rod theory, are computationally complex and often struggle to meet real-time control requirements, while methods like the pseudo-rigid body model improve computational efficiency at the cost of reduced accuracy. On the other hand, kinematics or dynamics models based on data-driven approaches often suffer from poor generalizability and interpretability. Moreover, most data-driven and learning-based control methods tend to focus on demonstrating the effectiveness of intelligent algorithms, while lacking rigorous proofs of convergence and stability. Future research should prioritize the development of lightweight, physics-informed modeling methods that integrate data and physical principles, ensuring both accuracy and real-time control feasibility. Additionally, efforts should be directed toward constructing data-driven control frameworks with theoretical guarantees, thereby enhancing the interpretability and reliability of such algorithms.</p>
      <p id="d2e2428">With the deepening of interdisciplinary research and technological innovation, soft robot control technology will continue to break new ground, driving its practical application in fields such as medical rehabilitation and precision manipulation. Future research should emphasize the integration of theoretical innovation and engineering practice to achieve the comprehensive development and widespread application of soft robot technology.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d2e2435">The data used in this work are available from the corresponding author upon reasonable request.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e2441">Huijun Yu: conceptualization and supervision. Min Lv: investigation and writing (original draft). Bin Hu: investigation. Yang Zhang: investigation. Pengyuan Zhao: writing (review and editing) and visualization.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e2447">At least one of the (co-)authors is a member of the editorial board of <italic>Mechanical Sciences</italic>. The peer-review process was guided by an independent editor, and the authors also have no other competing interests to declare.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e2456">Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e2462">This work was supported by the Shenzhen Science and Technology Program (KCXFZ20240903094011015) and the 2024 “Hundred Doctors-Hundred Enterprises” Initiative (2024H-100171).</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e2467">This research has been supported by the Shenzhen Science and Technology Program (grant no. KCXFZ20240903094011015) and the 2024 “Hundred Doctors-Hundred Enterprises” Initiative (grant no. 2024H-100171).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e2473">This paper was edited by Fulei Ma and reviewed by two anonymous referees.</p>
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