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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mech. Eng</journal-id>
<journal-title>Frontiers in Mechanical Engineering</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mech. Eng</abbrev-journal-title>
<issn pub-type="epub">2297-3079</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">966335</article-id>
<article-id pub-id-type="doi">10.3389/fmech.2022.966335</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Mechanical Engineering</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Contact mechanics analysis of a soft robotic fingerpad</article-title>
<alt-title alt-title-type="left-running-head">Achilli et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fmech.2022.966335">10.3389/fmech.2022.966335</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Achilli</surname>
<given-names>Gabriele Maria</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1693791/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Logozzo</surname>
<given-names>Silvia</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1921771/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Malvezzi</surname>
<given-names>Monica</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/137533/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Valigi</surname>
<given-names>Maria Cristina</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1689357/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Department of Engineering</institution>, <institution>University of Perugia</institution>, <addr-line>Perugia</addr-line>, <country>Italy</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Department of Information Engineering and Mathematics</institution>, <institution>University of Siena</institution>, <addr-line>Siena</addr-line>, <country>Italy</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/601759/overview">Markus He&#xdf;</ext-link>, Technical University of Berlin, Germany</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/708477/overview">Lorenzo Scalera</ext-link>, University of Udine, Italy</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/280982/overview">Shaoting Lin</ext-link>, Massachusetts Institute of Technology, United States</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Maria Cristina Valigi, <email>mariacristina.valigi@unipg.it</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Tribology, a section of the journal Frontiers in Mechanical Engineering</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>24</day>
<month>08</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>8</volume>
<elocation-id>966335</elocation-id>
<history>
<date date-type="received">
<day>10</day>
<month>06</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>25</day>
<month>07</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Achilli, Logozzo, Malvezzi and Valigi.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Achilli, Logozzo, Malvezzi and Valigi</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>The precision grasping capabilities of robotic hands is a key feature which is more and more required in the manipulation of objects in several unstructured fields, as for instance industrial, medical, agriculture and food industry. For this purpose, the realization of soft robotic fingers is crucial to reproduce the human finger skills. From this point of view the fingerpad is the part which is mostly involved in the contact. Particular attention must be paid to the knowledge of the mechanical contact behavior of soft artificial fingerpads. In this paper, artificial silicone fingerpads are applied to the last phalanx of robotic fingers actuated by tendons. The mechanical interaction between the fingerpad and a flat surface is analyzed in terms of deformations, contact areas and indentations. A reliable model of fingertip deformation properties provides important information for understanding robotic hand performance, that can be useful both in the design phase and for defining control strategies. The approach is based on theoretical, experimental, and numerical methods. The results will be exploited for the design of more effective robotic fingers for precision grasping of soft or fragile objects avoiding damages.</p>
</abstract>
<kwd-group>
<kwd>grasping</kwd>
<kwd>robotic finger</kwd>
<kwd>manipulation</kwd>
<kwd>3D scanner</kwd>
<kwd>robotic gripper</kwd>
<kwd>contact mechanics</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>Manipulators are essential elements of robots which are constituted of a mechanical structure with a terminal element known as end-effector. The end-effector has the effective responsibility of interacting with the object to be manipulated (<xref ref-type="bibr" rid="B31">Melchiorri and Kaneko, 2008</xref>; <xref ref-type="bibr" rid="B8">Carbone, 2012</xref>; <xref ref-type="bibr" rid="B35">Pozzi et al., 2022</xref>).</p>
<p>Grasping is the function to pick up and hold an object. Grasping and manipulation are fundamental abilities for humans and in several applications robots are employed to replicate the operation of human hands. Research in this field is very active and aimed at conceiving new designs for manipulators and grippers to improve the manipulation capabilities. The main tasks performed by a gripper are grasping and manipulation of objects; for this reason, they are specialized structures with few sensors and characterized by simple kinematic structures. The most modern grippers are more and more similar to human hands (<xref ref-type="bibr" rid="B7">Bennett et al., 2015</xref>; <xref ref-type="bibr" rid="B41">Shintake et al., 2018</xref>; <xref ref-type="bibr" rid="B23">Ke et al., 2021</xref>), and their design varies from grippers with two parallel fingers, to those that replicate the anthropomorphism of the human hand with articulated fingers and palm (<xref ref-type="bibr" rid="B3">Achilli et al., 2020</xref>; <xref ref-type="bibr" rid="B1">Achilli et al., 2021</xref>; <xref ref-type="bibr" rid="B2">Achilli et al., 2022</xref>; <xref ref-type="bibr" rid="B42">Shorthose et al., 2022</xref>).</p>
<p>Being very significative for many operations in work and human life, human hands are the subject of a wide range of engineering and technology research topics: human hand serves as an inspiration for constructing successful robotic hands and grippers, as well as the starting point for developing upper limb prostheses and haptic technologies. Human hands are strong end-effectors that humans use to grasp and manipulate items and tools, as well as perceptive means (<xref ref-type="bibr" rid="B11">Clemente 1981</xref>; <xref ref-type="bibr" rid="B6">Balasubramanian and Santos, 2014</xref>; <xref ref-type="bibr" rid="B12">Controzzi et al., 2014</xref>). The grasping taxonomies reported in literature are more than 100 (<xref ref-type="bibr" rid="B16">Feix et al., 2014</xref>) and the action of grasping can be defined according to different characteristics as power grasping and precision grasping. In precision grasps the object is generally small, and sometimes fragile and it is grasped between the finger-pads. Precision grasping is required in the manipulation of components in the industrial, agricultural, and medical fields (<xref ref-type="bibr" rid="B34">Payne and Yang, 2014</xref>; <xref ref-type="bibr" rid="B29">Low et al., 2016</xref>; <xref ref-type="bibr" rid="B19">Gong et al., 2022</xref>).</p>
<p>
<xref ref-type="fig" rid="F1">Figure 1</xref> shows an example of both human and robotic fingers during precision grasp. As it possible to understand, the analysis of contact is an important issue to manage precision grasping with robotic fingers.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Human <bold>(A)</bold> and robotic <bold>(B)</bold> fingerpads during precision grasping.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g001.tif"/>
</fig>
<p>Since the contact between a hard gripper and a hard object can lead to shocks and consequent damages of the manipulated object, the compliance of grasping is a topic of great significance (<xref ref-type="bibr" rid="B25">Li et al., 2020</xref>). From this perspective, the use of advanced materials and soft components to make grippers is becoming an interesting practice (<xref ref-type="bibr" rid="B39">Salvietti et al., 2019</xref>).</p>
<p>3D printed materials such as PLA, ABS, TPU and silicone rubbers are becoming the most popular choice for grippers thanks to their ease of fabrication, low toxicity, and robustness (Elango and Faudzi, 2015; Malvezzi et al., 2019a; Malvezzi et al., 2019b; <xref ref-type="bibr" rid="B13">Dragusanu et al., 2022</xref>; Dragusanu et al., 2022b). Compliant materials are used for gripping components and pads with fingers made in PLA by 3D printing and soft components mold in silicone (&#x17b;ur et al., 2019). Furthermore, in recent papers anthropomorphic grippers with partly soft components have been described (Catalano et al., 2014; Deimel and Brock, 2016) reproducing human fingertips (Pinel, 1990; <xref ref-type="bibr" rid="B15">Dzidek et al., 2017</xref>).</p>
<p>The objective of this paper is the study of contact of a silicone fingertip for robotic fingers with partly soft components. The considered artificial finger of a robotic gripper studied in (<xref ref-type="bibr" rid="B13">Dragusanu et al., 2022</xref>) is equipped with a silicone fingertip with the aim of performing precision grasping of objects exploiting the softness of the pad.</p>
<p>The attention of the paper is focused on the mechanical interaction between the fingerpad and a flat surface in terms of contact deformations, contact areas and indentations (<xref ref-type="bibr" rid="B50">Wu et al., 2003</xref>). The analysis is performed by exploiting both 2D and 3D techniques, considering a tribological point of view and correlating forces, displacements, and deformations of fingers. A Finite Element Model is set, and experimental results are compared with simulated and theoretical ones, obtained by applying some contact theories. The systematic contact analysis allowed to determine the relationship between contact force and deformation in soft robotic fingertips both numerically and experimentally. In particular, the correlation between applied force, indentation, and contact patch area is investigated. The results obtained from experimental measures are compared with the results from theoretical contact analysis.</p>
<p>This kind of research generates information that can be useful for designing and predict the contact in precision grasping of robotic hands having that kind of fingerpad. The main contribution of the paper is the identification of the contact properties of silicone fingertips to be applied to robotic underactuated grippers, in terms of contact patch and contact pressure distribution. Differently from fully actuated hands, in which joints can be precisely and independently controlled to perform complex manipulation tasks, in underactuated and soft robotic hands finger closure motion and grasp stability and robustness properties are related to the structural overall compliance, that depends both on joint stiffness, or finger structure deformation, and on contact properties (<xref ref-type="bibr" rid="B37">Prattichizzo et al., 2013</xref>). Notwithstanding the amount of studies on modelling, simulation and control of soft robotic grippers is increasing (<xref ref-type="bibr" rid="B14">Duriez and Bieze, 2017</xref>; <xref ref-type="bibr" rid="B17">George Thuruthel et al., 2018</xref>; <xref ref-type="bibr" rid="B21">Hussain et al., 2021</xref>), to the best of the author&#x2019;s knowledge, fewer research is dedicated to contact properties. Contact patch extension, contact stiffness and pressure distribution have an important role in quantifying grasp robustness, stability, and stiffness (<xref ref-type="bibr" rid="B30">Malvezzi and Prattichizzo, 2013</xref>; <xref ref-type="bibr" rid="B38">Roa and Su&#xe1;rez, 2015</xref>).</p>
<p>The 2D analysis is carried out by taking ink fingerprints correlated with the applied forces, while the 3D analysis is performed by 3D deformation maps obtained by 3D optical scanners and a new experimental method inspired by (<xref ref-type="bibr" rid="B48">Valigi and Logozzo, 2019</xref>; <xref ref-type="bibr" rid="B28">Logozzo et al., 2022b</xref>; <xref ref-type="bibr" rid="B24">Landi et al., 2022</xref>) and using the 3D scanning technologies as in (<xref ref-type="bibr" rid="B26">Logozzo et al., 2018</xref>; <xref ref-type="bibr" rid="B46">Valigi et al., 2018</xref>; <xref ref-type="bibr" rid="B5">Affatato et al., 2020</xref>). The experiments were carried out using an instrumented plate and a reverse engineering method (<xref ref-type="bibr" rid="B49">Valigi et al., 2016</xref>; <xref ref-type="bibr" rid="B45">Valigi et al., 2019a</xref>; <xref ref-type="bibr" rid="B47">Valigi et al., 2019b</xref>). Theoretical contact models where applied and discussed (<xref ref-type="bibr" rid="B40">Schwarz, 2003</xref>; <xref ref-type="bibr" rid="B4">Adams et al., 2007</xref>; <xref ref-type="bibr" rid="B20">He&#xdf; and Popov, 2019</xref>). The main differences with the previously mentioned works are related to the fields of application of the methodology. Indeed, in this manuscript the methodology is used to analyze precision grasp of robotic fingers with silicone fingertips (<xref ref-type="bibr" rid="B28">Logozzo et al., 2022b</xref>). In addition, the applied methodology has been improved, as described in (<xref ref-type="bibr" rid="B27">Logozzo et al., 2022a</xref>).</p>
<p>The paper is structured as follows: in <xref ref-type="sec" rid="s2">Section 2</xref> the sample preparation is described together with the instruments and applied methodologies; <xref ref-type="sec" rid="s3">Section 3</xref> reports results of the experiments and numerical and theoretical analyses, discussing the comparison of results; <xref ref-type="sec" rid="s4">Section 4</xref> is dedicated to conclusions.</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<title>Materials and methods</title>
<sec id="s2-1">
<title>Sample preparation</title>
<p>Material stiffness and gripper morphology typically define the deformation and kinematic capabilities in soft robot grippers made of one single material. The combination of soft materials with different properties in a single gripper is the solution to engineer deformation behavior required by the specific task in which the gripper is employed.</p>
<p>Therefore, soft grippers designers aim at systematically taking advantage of multi-material 3D printing for creating dexterous soft robotic devices. The studied finger belongs to a new type of robotic grippers named WaveJoints grippers and composed of 3D-printed fingers, actuated by tendons, in which each finger is a monolithic element composed of stiff parts (the phalanges) connected by flexible wave-shaped parts (<xref ref-type="fig" rid="F2">Figure 2</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>The WaveJoints gripper.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g002.tif"/>
</fig>
<p>The fingers of the gripper were reproduced by 3D printing but a new element in silicone was added to simulate the human fingertip contact. The fingertip was made of EcoFlex 00&#x2013;30 (<xref ref-type="bibr" rid="B33">Noor and Mahmud, 2015</xref>; <xref ref-type="bibr" rid="B43">Steck et al., 2019</xref>; <xref ref-type="bibr" rid="B36">Pozzi et al., 2021</xref>) and crafted using a 3D printed mould realized according to a proper design. After casting, the silicone fingerpad was mounted on the last phalanx of the WaveJoint finger (<xref ref-type="fig" rid="F3">Figure 3</xref>).</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Design of the sample finger, equipped with the soft, silicone-based, fingerpad.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g003.tif"/>
</fig>
<p>The experimental contact analysis was carried out by means of both 2D and 3D techniques.</p>
</sec>
<sec id="s2-2">
<title>Experimental instruments and 3D contact analysis</title>
<p>The 3D study was based on the method used in (<xref ref-type="bibr" rid="B28">Logozzo et al., 2022b</xref>) with some variations, as reported in (<xref ref-type="bibr" rid="B27">Logozzo et al., 2022a</xref>). The applied method implies the use of 3D optical scanners and reverse engineering and inspection software but, with respect to (<xref ref-type="bibr" rid="B28">Logozzo et al., 2022b</xref>) in this work the indentation of the fingertip subjected to a certain force was measured by a digital force-displacement gauge. The materials and instruments used for the 3D contact analysis were:<list list-type="simple">
<list-item>
<p>&#x2022; A sensorized plate equipped with a force sensitive resistor (FSR) and controlled by Arduino</p>
</list-item>
<list-item>
<p>&#x2022; A dough material to impress the fingerprint of the deformed fingerpad</p>
</list-item>
<list-item>
<p>&#x2022; A digital force-displacement gauge</p>
</list-item>
<list-item>
<p>&#x2022; A desktop 3D optical scanner</p>
</list-item>
<list-item>
<p>&#x2022; A reverse engineering and inspection software</p>
</list-item>
<list-item>
<p>&#x2022; A FEA software</p>
</list-item>
</list>
</p>
<p>Six tests were performed with the silicone fingerpad. For each test a layer of dough material was put on the FSR on the sensorized plate and the silicone fingerpad was pressed against the plate measuring a compressive force while the deformation of the fingerpad was impressed on the dough layer (<xref ref-type="fig" rid="F4">Figure 4</xref>).</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>3D Compression tests.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g004.tif"/>
</fig>
<p>The 3D fingerprints on the dough material were left to harden to the open air. Given the values of the compressive forces measured by the FSR, the corresponding vertical displacement of the fingerpad (<italic>&#x3b4;</italic>) was measured by a force-displacement gauge (ZTA 50-N, Imada, Japan), as represented in <xref ref-type="fig" rid="F5">Figure 5</xref>. Then the 3D fingerprints were digitized by means of a desktop structured light 3D scanner (EinScan-SE, Shining 3D, China) with a scanning procedure comprising 12 turntable rotations and alignment based on feature recognition (<xref ref-type="fig" rid="F6">Figure 6</xref>). The 3D scanning procedure was performed after calibration of the instrument. From this procedure the 3D digital models of the fingerprints impressed on the dough material were obtained in the form of triangular meshes. The 3D models of the fingerprints were imported in the mesh editing and inspection software (Geomagic, 3D Systems,US) together with the CAD model of the silicone fingertip. Then the two models were superimposed considering the indentation measured by the force-displacement gauge (<xref ref-type="fig" rid="F7">Figure 7</xref>).</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Displacement measurements.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g005.tif"/>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>3D scanning procedure.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g006.tif"/>
</fig>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Reconstruction of the fingertip deformation.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g007.tif"/>
</fig>
<p>From this alignment the 3D indentation maps were reconstructed, which represented the deviation between the deformed and undeformed fingertip. Taking as a reference the undeformed fingertip, the indentation map displays the 3D distribution of deformations. The 3D alignment can also help to display the gross contact areas defined by the intersection curve between deformed and undeformed finger. This methodology can be applied until the indentation does not become higher than the equivalent radius of the indenter.</p>
<p>More insight about the 3D contact analysis proposed in this work can be found in (<xref ref-type="bibr" rid="B27">Logozzo et al., 2022a</xref>), where different experimental instruments are discussed with particular attention to 3D scanners and reverse engineering software. For instance, the accuracy of the 3D measurements depends on the performance parameters of the used 3D digitizers. In this paper an instrument with an accuracy grade of 0.1&#xa0;mm for single frame was used. Trueness and precision of the contact area measurements depends both on the accuracy of the 3D digitizer and also on the alignment between the undeformed fingerpad model and the fingerprint model. In this work this alignment was guided by the indentations measured by the digital force-displacement gauge, but the accuracy and repeatability can also be improved using a second portable 3D scanner to digitize the fingerpad while it is imprinting on the dough material, as reported in (<xref ref-type="bibr" rid="B27">Logozzo et al., 2022a</xref>). In this work, this second 3D scanner was not used but the experimental contact area was also measured by using an additional method based on 2D ink fingerprints.</p>
</sec>
<sec id="s2-3">
<title>Numerical analysis</title>
<p>The numerical contact analysis was also performed by Finite Element Method (FEM) software. For the study, a hyperelastic material was chosen for the silicone part, considering a geometric nonlinearity (<xref ref-type="bibr" rid="B22">Jindrich et al., 2003</xref>; <xref ref-type="bibr" rid="B52">Sergachev et al., 2019</xref>). The used hyperelastic model was the 2-parameter Mooney-Rivlin one which simulates the behavior of Ecoflex 00&#x2013;30 silicone (<xref ref-type="bibr" rid="B36">Pozzi et al., 2021</xref>). The material properties are described with the shear modulus &#x3bc; and two Mooney-Rivlin constants C<sub>1</sub> and C<sub>2</sub>, as reported in <xref ref-type="table" rid="T1">Table 1</xref>. The study applied a prescribed displacement to the fingerpad equal to the maximum displacement measured by the force-displacement gauge, as mentioned in <xref ref-type="sec" rid="s2-2">section 2.2</xref>, with a fixed constraint on the rigid plate, to evaluate the deformation map of the component.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Material properties.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left"/>
<th align="left">Shear modulus (&#x3bc;)</th>
<th align="left">C1</th>
<th align="left">C2</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">Mooney-Rivlin 2-parameters</td>
<td align="left">4.72&#xa0;kPa</td>
<td align="left" char=".">0.4375&#x3bc;</td>
<td align="left" char=".">0.0625&#x3bc;</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s2-4">
<title>Experimental instruments and 2D contact analysis</title>
<p>The experimental 2D contact analysis was carried out using the following materials and instruments:<list list-type="simple">
<list-item>
<p>&#x2022; A sensorized plate equipped with a force sensitive resistor (FSR) and controlled by Arduino</p>
</list-item>
<list-item>
<p>&#x2022; Ink to create a fingerprint on a white paper</p>
</list-item>
<list-item>
<p>&#x2022; A digital caliper</p>
</list-item>
</list>
</p>
<p>The tests were performed by wetting the silicone fingerpad with the ink and pressing it on a white paper laying on the FRS. The same compressive forces considered for the 3D tests were measured while the 2D fingerprint was impressed on the paper (<xref ref-type="fig" rid="F8">Figure 8</xref>).</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>2D Compression tests.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g008.tif"/>
</fig>
<p>The obtained fingerprints had an ellipsoidal shape whose maximum and minimum semiaxes were measured by a caliper. These values were used to calculate the area of the fingerprint to be compared with the gross contact area resulting from the 3D measurements.</p>
</sec>
<sec id="s2-5">
<title>Theoretical contact analysis</title>
<p>Gross contact areas were also calculated according to the most common theoretical mechanical contact models and in particular the Hertz theory and the Johnson, Kendall and Roberts (JKR) model, considering a radius of curvature of the silicone-based finger equal to 5&#xa0;mm.</p>
<p>The measured indentations and forces were used as inputs for the calculations of the theoretical radii of circular contact areas to be compared with the experimental ones (<xref ref-type="bibr" rid="B40">Schwarz, 2003</xref>; <xref ref-type="bibr" rid="B4">Adams et al., 2007</xref>; <xref ref-type="bibr" rid="B15">Dzidek et al., 2017</xref>; <xref ref-type="bibr" rid="B20">He&#xdf; and Popov, 2019</xref>; <xref ref-type="bibr" rid="B52">Sergachev et al., 2019</xref>). The Hertzian contact area was calculated based on the experimental indentation depth. The indentation was used to calculate the radius of the contact area which was in turn calculated as a circle area. Regarding the JKR model the analysis of the formation of the contact was considered, according to (<xref ref-type="bibr" rid="B9">Chokshi et al., 1993</xref>).</p>
</sec>
</sec>
<sec sec-type="results|discussion" id="s3">
<title>Results and discussion</title>
<p>Results concerning the 3D deformation of the silicone fingerpad are given in terms of indentation maps, as represented in <xref ref-type="fig" rid="F9">Figure 9</xref>. In <xref ref-type="fig" rid="F10">Figure 10</xref>, the resulting gross contact areas are highlighted with an orange ellipse. <xref ref-type="fig" rid="F11">Figure 11</xref> shows the 2D fingerprints.</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>3D Indentation maps.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g009.tif"/>
</fig>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>3D Gross contact areas.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g010.tif"/>
</fig>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>2D Fingerprints.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g011.tif"/>
</fig>
<p>All the experimental and theoretical results are summarized in <xref ref-type="table" rid="T2">Table 2</xref>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Results.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Sample</th>
<th align="left">Force (N)</th>
<th align="left">&#x3b4; (mm)</th>
<th align="left">3D gross contact area (mm<sup>2</sup>)</th>
<th align="left">2D gross contact area (mm<sup>2</sup>)</th>
<th align="left">Hertz gross contact area (mm<sup>2</sup>)</th>
<th align="left">JKR gross contact area (mm<sup>2</sup>)</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">B7</td>
<td align="left">1.09825</td>
<td align="left">1.62</td>
<td align="left">48.07</td>
<td align="left">39.39</td>
<td align="left">25.45</td>
<td align="left">44.08</td>
</tr>
<tr>
<td align="left">B6</td>
<td valign="top" align="left">2.19904</td>
<td align="left">2.42</td>
<td align="left">65.47</td>
<td align="left">50.28</td>
<td align="left">38.01</td>
<td align="left">65.84</td>
</tr>
<tr>
<td align="left">B1</td>
<td valign="top" align="left">3.10773</td>
<td align="left">2.49</td>
<td align="left">70.70</td>
<td align="left">67.39</td>
<td align="left">39.11</td>
<td align="left">67.75</td>
</tr>
<tr>
<td align="left">B5</td>
<td valign="top" align="left">4.97893</td>
<td align="left">3.18</td>
<td align="left">77.88</td>
<td align="left">75.35</td>
<td align="left">49.95</td>
<td align="left">86.52</td>
</tr>
<tr>
<td align="left">B2</td>
<td valign="top" align="left">7.72941</td>
<td align="left">3.75</td>
<td align="left">85.86</td>
<td align="left">90.80</td>
<td align="left">58.90</td>
<td align="left">102.03</td>
</tr>
<tr>
<td align="left">B3</td>
<td valign="top" align="left">11.7107</td>
<td align="left">4.29</td>
<td align="left">87.34</td>
<td align="left">91.89</td>
<td align="left">67.39</td>
<td align="left">116.72</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The 3D indentation map at the maximum displacement (4.29&#xa0;mm) was compared to the deformation map obtained by FEM analysis. Results are displayed in <xref ref-type="fig" rid="F12">Figure 12</xref>. As it can be observed, there is a slight difference between the experimental and simulated indentation maps. This difference is caused by the presence of the dough material in the experimental setup, which is necessary to take a plastic impression of the elastic deformation of the finger. Indeed, in the FEM simulation, the thickness, and the plastic deformation of the dough material, placed between the silicone fingertip and the rigid surface, are not considered.</p>
<fig id="F12" position="float">
<label>FIGURE 12</label>
<caption>
<p>Indentation maps comparison between experimental and numerical results.</p>
</caption>
<graphic xlink:href="fmech-08-966335-g012.tif"/>
</fig>
<p>From <xref ref-type="table" rid="T2">Table 2</xref> one can observe that both 2D and 3D experimental results are not comparable with the theoretical results obtained by applying the Hertz theory. This evidence can be explained considering that the Hertz model does not take into account adhesion, which is not negligible in the case of soft materials as silicone (<xref ref-type="bibr" rid="B32">Morales-Hurtado et al., 2017</xref>; <xref ref-type="bibr" rid="B10">Ciavarella et al., 2019</xref>).</p>
<p>On the contrary, the JKR model which considers adhesion gives results which can be validated by the experimental data obtained both by 2D and 3D analyses. Results demonstrate that the JKR theory approximates 3D contact areas better than 2D ones and this can be due to the fact that the 3D experimental analysis gives better result to adhesion.</p>
<p>When the value of the indentation <italic>&#x3b4;</italic> is close to the radius R of the indenter, the JKR model does not release reliable results, as this model is valid until <italic>&#x3b4;</italic> &#x3c;&#x3c; R. In this case, JKR overestimates the gross contact areas as demonstrated by samples B5, B2, B3.</p>
<p>For samples B7, B6, B1 and B5 the 2D gross contact area is lesser than the 3D one and this phenomenon can be explained considering that the 3D results also include the adhesion zone, due to the presence of the dough material.</p>
<p>For the samples B2 and B3, which are characterized by the deepest indentation, the presence of the dough material could have limited the lateral bulging of the silicone fingerpad, giving 3D gross contact areas lesser than the 2D ones.</p>
<p>The 3D contact analysis method has the capability to compute the distribution of the fingerpad 3D deformations and results allow to also display the lateral contact between a fingerpad and a soft object to be grasped.</p>
<p>Silicone has a hyperelastic behavior and also the dough material has an influence on the contact but considering the comparison between numerical results and the outcomes of the 3D contact analysis reported in <xref ref-type="fig" rid="F12">Figure 12</xref> one can conclude that the information about the 3D deformation distribution obtained by 3D contact analysis is reliable and gives fundamental insights to design partly soft grippers which have to grasp soft objects avoiding damages. Furthermore, the knowledge of the gross contact area can allow to better control the precision grasping operations.</p>
</sec>
<sec sec-type="conclusion" id="s4">
<title>Conclusion</title>
<p>Grasping and manipulating objects is one of the most prevalent activities in human everyday life, which is the reason why human hands and fingers have been taken as an inspiration to design several artificial grippers. This paper was focused on the contact analysis of soft fingerpads with the aim of evaluating the 3D distribution of deformations during the contact, indentations, and gross contact areas. Numerical, experimental, and theoretical analyses were performed, and results were compared and discussed.</p>
<p>Gross contact areas were evaluated by 3D and 2D experimental contact analyses and by theoretical contact models. 3D deformations of the fingerpad were detected by means of 3D indentation maps obtained by 3D scanning techniques and by FEM analysis.</p>
<p>Results demonstrated that the 3D contact analysis gave reliable information about contact deformations and areas, also considering the adhesive phenomenon typically affecting the contact of soft materials. This study put the basis for the study of contact of partly soft grippers for the design of compliant precision grasping. This work represents a first step in the characterization of soft robotic finger contact elements. As highlighted in the introductory part of the paper, the results of this study are useful in the design and control of soft robotic fingers, since contact properties are important elements in grasping and manipulation tasks. Another important field in which the results of this study could be exploited is the development of new tactile sensors (<xref ref-type="bibr" rid="B51">Yamaguchi and Atkeson, 2019</xref>; <xref ref-type="bibr" rid="B18">Gomes et al., 2020</xref>; <xref ref-type="bibr" rid="B44">Sun et al., 2022</xref>).</p>
<p>Future developments of this work will include a deeper investigation on material models including nonlinearities and anisotropy, an extension of the experimental test set with different sizes, shapes, and materials of the fingerpads.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s5">
<title>Data availability statement</title>
<p>The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec id="s6">
<title>Author contributions</title>
<p>All authors listed have made a substantial, direct, and intellectual contribution to the work and approved it for publication.</p>
</sec>
<sec sec-type="COI-statement" id="s7">
<title>Conflict of interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s8">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
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