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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0"><?xmltex \hack{\allowdisplaybreaks}?>
  <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-11-357-2020</article-id><title-group><article-title>A new hand rehabilitation system based on the cable-driven mechanism and dielectric<?xmltex \hack{\break}?> elastomer actuator</article-title><alt-title>A new hand rehabilitation system based on the cable-driven
mechanism</alt-title>
      </title-group><?xmltex \runningtitle{A new hand rehabilitation system based on the cable-driven
mechanism}?><?xmltex \runningauthor{H.~Amin et~al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff3">
          <name><surname>Amin</surname><given-names>Heba</given-names></name>
          <email>eng.hebaamin@hotmail.com</email><email>heba.saleh@ejust.edu.eg</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff3">
          <name><surname>Assal</surname><given-names>Samy F. M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Iwata</surname><given-names>Hiroyasu</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Department of Mechatronics and Robotics Engineering, School of Innovative Design Engineering, Egypt-Japan University of Science and Technology, 21934 Alexandria, Egypt</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Modern Mechanical Engineering, Graduate School of Creative Science and Engineering, Waseda University, 27 Waseda-cho, Shinjuku-ku, 162-0042 Tokyo, Japan</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Production Engineering and Mechanical Design, Faculty of Engineering,<?xmltex \hack{\break}?> Tanta University, 31511 Tanta, Egypt</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Heba Amin (eng.hebaamin@hotmail.com, heba.saleh@ejust.edu.eg)</corresp></author-notes><pub-date><day>20</day><month>October</month><year>2020</year></pub-date>
      
      <volume>11</volume>
      <issue>2</issue>
      <fpage>357</fpage><lpage>369</lpage>
      <history>
        <date date-type="received"><day>6</day><month>November</month><year>2019</year></date>
           <date date-type="accepted"><day>24</day><month>August</month><year>2020</year></date>
           <date date-type="rev-recd"><day>17</day><month>July</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2020 Heba Amin et al.</copyright-statement>
        <copyright-year>2020</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/11/357/2020/ms-11-357-2020.html">This article is available from https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020.html</self-uri><self-uri xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020.pdf">The full text article is available as a PDF file from https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e113">The increasing number of patients with hand disabilities after strokes or peripheral nerve injuries necessitates the continuous development of rehabilitation system devices to accelerate muscle recovery and to help patients regain the motor functions of their hands. This paper introduces the design of a hand rehabilitation system for patients who have a solitary impairment of their hand extension. The system was designed to be portable, simple, and cheap. Using a system based on a cable-driven mechanism instead of traditional rigid links reduces the degrees of freedom of the finger to one. The dielectric elastomer actuator was designed and fabricated as a smart actuator for the system, which supports the low cost of the system. A kinematic analysis of the cable-driven mechanism has been done. Parameters of the actuator were optimized to reach the required output. In order to characterize the performance of the actuator, a uniaxial tension test, isotonic test, and isometric test have been implemented.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e125">The hand is a vital, multifunctional organ for humans that plays an
important role in physical activities and in the development of fine and
gross motor skills. Any disease disrupting the hand function will lead
to disability and, consequently, worsen the quality of human life. The
need to develop hand rehabilitation strategies became a vital
issue with an increase in the number of patients (and old people in particular) who
suffer from impairments in their hand motor function after
strokes and injuries. The strategies for hand rehabilitation depend on maintaining the muscles' ability and preventing their atrophy by doing repetitive hand exercises <xref ref-type="bibr" rid="bib1.bibx6" id="paren.1"/>. As traditional,
human-assisted therapy is challenging and expensive, many hand
rehabilitation devices or robot-assisted therapies were recently introduced  and achieved excellent results by enhancing the motor
function of the muscles.  Those devices offer a new kind of
physiotherapy; in this way, patients practice moving their muscles by
following or withstanding the robot's force. Recently, there have been
significant developments with the advances in robotic technology, such
as the exoskeleton and bioengineering, that have become a significant
addition to physiotherapy methods.</p>
      <p id="d1e131">As a result of the variety of hand rehabilitation protocols, different
robots have been designed to run alternative therapies. The
rehabilitation clinics have different types of stationary hand
rehabilitation devices which are set up in the clinics and have acquired
good results, especially with the computer interface assistance that
increases the patients' motivation <xref ref-type="bibr" rid="bib1.bibx9 bib1.bibx22" id="paren.2"/>. The availability of
these devices is still insufficient for the majority of patients, due to the long time required for motor recovery training and the expensive fees for using the equipment.<?pagebreak page358?> Also, these devices do not help them directly in their daily life activities.</p>
      <p id="d1e137">Portable devices introduce an alternative to avoid some of these
issues as the patients can train themselves at home. The bulky
exoskeleton device is the most common type of portable assistive system
which supplies highly accurate motion. It is a mechanism of rigid
links fixed onto the palm side of the hand and controls the hand–finger
motion <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx11 bib1.bibx2 bib1.bibx12 bib1.bibx13 bib1.bibx4 bib1.bibx14" id="paren.3"/>. Despite its excellent results, the
bulky size and complicated structure present a burden for the
patient and limit its workspace area. Also, the rigid structures of
some of these devices are impeding the therapeutic potential of
robotics by reducing their biomimetic qualities, and the motion in
non-actuated directions, such as finger abduction, could include having
rigid axes of rotation that become misaligned with the finger's
anatomic axis during motion <xref ref-type="bibr" rid="bib1.bibx8" id="paren.4"/>.</p>
      <p id="d1e146">In contrast, soft rehabilitation devices, which are simple and lightweight, solve this problem by using the natural exoskeleton of
the hand and wearable gloves to control hand motion. These devices have been
fabricated from easily deformable materials such as fluids, gels, and
soft polymers that have better biomimetic qualities, due to their
increased compliance and inconstancy, while complying with the contours
of the human body. The lack of rigid components removes constraints on
non-actuated degrees of freedom and reduces joint alignment issues,
which could prevent joint damage. The main problem of this type of device is its
actuation system, as most of them are actuated by the pneumatic system,
which has a large complex volume and low
accuracy <xref ref-type="bibr" rid="bib1.bibx20 bib1.bibx24 bib1.bibx18 bib1.bibx13 bib1.bibx8" id="paren.5"/>. Recently, a soft glove for hand
rehabilitation with a cable-driven mechanism was introduced
<xref ref-type="bibr" rid="bib1.bibx23" id="paren.6"/>. Another trial was made by <xref ref-type="bibr" rid="bib1.bibx19" id="paren.7"/>, who proposed a
cable-driven structure of the hand exoskeleton system for virtual reality
purposes. Cherian et al. (2018) introduced the Exo-Glove, the most
popular one, which is suitable for the extension and flexion of the
finger. However, tendon-driven systems have a major limitation in
that they induce significant joint reaction forces. In and Cho (2013)
indicated that, since the tendons are attached further away with a
larger moment arm compared to the actual human tendons, these forces
should not be a problem unless the spasticity of the patient's fingers
is very high.</p>
      <p id="d1e159">Several types of actuators are used in hand rehabilitation
systems. The electric motors are the standard type due to their
availability, reliability, and easy torque control with high
precision, but the rigid structure may affect safety. Although the
pneumatic actuator has fewer requirements for maintenance and might be
stopped under a load without causing damages, the difficulty in
controlling it and the air storage bulk size limits its use. Also, the
hydraulic actuator has the same problem as the size of its parts;
however, it may supply higher actuated torque and can be controlled
with high precision, as reported by Yue et al. (2017). There are some
trials for using smart actuators in hand rehabilitation systems to
decrease the disadvantage of the previous actuators; for example, Tang
et al. (2013) designed an exoskeleton system to assist hand
rehabilitation exercises based on a shape memory alloy
actuator. While it offered a light and straightforward structure,
its temperature-dependent nature makes precise control difficult.</p>
      <p id="d1e162">Using dielectric elastomer materials (DEMs) as a smart actuator for
the system might be a remedy for the common defects of actuation
methods. The dielectric elastomer material has the closest material
properties for natural muscles, particularly in the stress and strain
levels. As mentioned by Pelrine et al. (2002) and Madden (2008), its
strain is between 10 % and 100 %, which is similar to or higher
than in muscle. Also, the stress is 0.1–8 <inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">MPa</mml:mi></mml:mrow></mml:math></inline-formula>. Work density
in the muscle may reach 40 <inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, compared to between 10
and 150 <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in silicone and VHB-based elastomers,
respectively. The continuous power output of dielectric elastomers
also matches or exceeds that of our skeletal muscle, with human muscle
producing about 50 <inline-formula><mml:math id="M4" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> compared to about
400 <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">W</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">kg</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> in the elastomers. In addition, it does not have a
temperature-dependent response like the shape memory alloys so that it
can work in different environments.</p>
      <p id="d1e241">As the design of the hand rehabilitation robotics is different from
the traditional design of robots because it involves humans, the
safety and availability of the device are essential
requirements for the rehabilitation system. This research aims to
design a bio-mimic, soft hand rehabilitation system that must be
portable, simple, and cheap. A cable-driven mechanism is proposed to
work instead of the rigid links and be actuated by the dielectric
elastomer actuator. This design mimics the natural procedure of finger
motion as the cable-driven and the dielectric elastomer actuator (DEA) represent, instead, the
natural tendon and muscle, respectively. While there are a variety of
hand rehabilitation devices for the patients whose therapy needs
are different to others, the target patients for
this rehabilitation system are those who have a solitary impairment of
their hand extension, as in peripheral radial nerve compression or
injury. Nicholls and Furness (2019) indicated that most patients
respond well to conservative therapy. They are considering relative
rest from offending muscle activity, such as limiting repetitive
pronation, supination, wrist flexion, and ulnar deviation. If symptoms
are not resolved with the cessation of activity and rest, then splinting is considered.</p>
      <p id="d1e244">The rest of the paper is organized as follows. The kinematic and
dynamic analysis of the natural hand is given in Sect. 2. The
proposed design of the cable system is presented in Sect. 3. The
development and fabrication of the DEA are presented in Sect. 4, while
Sect. 5 presents the performance characterization of the
DEA. The conclusion and future work are presented in Sects. 6 and 7,
respectively.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e249">The human hand–finger structure.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f01.png"/>

      </fig>

</sec>
<?pagebreak page359?><sec id="Ch1.S2">
  <label>2</label><title>The human hand</title>
      <p id="d1e266">The natural hand is a complex combination of bones, muscles, and
ligaments which determine the direction and range of motion. The
natural hand has several kinds of motion such as flexion and extension and adduction and abduction for each finger and opposing movements between the thumb and other fingers, which present 27 <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">DOF</mml:mi></mml:mrow></mml:math></inline-formula>, as mentioned in Agur and Lee (1999). This large degree of freedom (DOF) makes the rehabilitation of
all simultaneous motion challenging. For this research, we focus on
the patients who have problems in their hand extension motion, so the
other types of motion are being neglected, and each finger will be
represented as a planar 3R mechanism. The patients will control their hand's
flexion motion while the wiring systems will control the hand
extension, as shown in Fig. 1. The fingertip pose <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msup><mml:mi>P</mml:mi><mml:mi>i</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula> for each
finger can be defined as a function of joint coordinates and described
by the following equations:

              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M8" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msup><mml:mi>P</mml:mi><mml:mi>i</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:mfenced open="[" close="]"><mml:mtable rowspacing="5.690551pt 5.690551pt" class="array" columnalign="center"><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi>P</mml:mi><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi>P</mml:mi><mml:mi>y</mml:mi><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msup><mml:mi mathvariant="italic">φ</mml:mi><mml:mi>i</mml:mi></mml:msup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced open="[" close="]"><mml:mtable rowspacing="5.690551pt 5.690551pt" class="array" columnalign="center"><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mi>C</mml:mi><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mi>C</mml:mi><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">12</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mi>C</mml:mi><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">123</mml:mn><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mi>S</mml:mi><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mi>S</mml:mi><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">12</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mi>S</mml:mi><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">123</mml:mn><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">12</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">123</mml:mn><mml:mi>i</mml:mi></mml:msubsup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced></mml:mrow></mml:math></disp-formula></p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e479">The average dimension of the human hand finger.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="justify" colwidth="30mm"/>
     <oasis:colspec colnum="3" colname="col3" align="justify" colwidth="30mm"/>
     <oasis:colspec colnum="4" colname="col4" align="justify" colwidth="30mm"/>
     <oasis:colspec colnum="5" colname="col5" align="justify" colwidth="30mm"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">The index finger</oasis:entry>
         <oasis:entry colname="col3">The middle finger</oasis:entry>
         <oasis:entry colname="col4">The ring finger</oasis:entry>
         <oasis:entry colname="col5">The small finger</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Proximal phalanges</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>PP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">56.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M11" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">19.27</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M12" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>PP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">52.2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M14" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">17.69</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>PP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">50.6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M18" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">14.99</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>PP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">39.6</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">9.13</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Middle phalanges</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>MP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">21.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">6.03</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>MP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">25.7</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7.27</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>MP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">23.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.8</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>MP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">16.9</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M38" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">3.34</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M40" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Small phalanges</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>DIP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">26.9</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M42" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">6.13</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M44" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>DIP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">26.9</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M46" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">6.2</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>DIP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">26.9</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.58</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mtext>DIP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">25.5</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M54" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> <?xmltex \hack{\hfill\break}?> <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:mi>m</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">4.23</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M56" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1091">where <inline-formula><mml:math id="M57" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is the number of fingers (<inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:math></inline-formula>) excluding the thumb,
<inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>y</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the position of fingertip position in <inline-formula><mml:math id="M61" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and
<inline-formula><mml:math id="M62" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> direction, <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M65" display="inline"><mml:mrow><mml:msubsup><mml:mi>l</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mi>i</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> are the proximal,
middle, and distal phalanges lengths, respectively, and <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are the angular displacement around the
<inline-formula><mml:math id="M69" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula> axis for the three revolute joints. Table 1 shows the average
dimension of the human hand finger which was reported by Serbest
et al. (2018). According to the Lagrangian form, the equation of
motion of each finger can be defined as follows:

              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M70" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>M</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>)</mml:mo><mml:mover accent="true"><mml:mi mathvariant="italic">θ</mml:mi><mml:mo mathvariant="normal">¨</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:mi>C</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mover accent="true"><mml:mi mathvariant="italic">θ</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>)</mml:mo><mml:mover accent="true"><mml:mi mathvariant="italic">θ</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>+</mml:mo><mml:mi>g</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        where <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:mi>M</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:mi>C</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mover accent="true"><mml:mi mathvariant="italic">θ</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M73" display="inline"><mml:mi>g</mml:mi></mml:math></inline-formula> are the joint
inertia matrix, the matrix of the centrifugal and Coriolis torques, and
the gravity vector, respectively. <inline-formula><mml:math id="M74" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> is the required joint torque
to move the finger, and it can be described as the difference between
<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">τ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the active joint torque (from active muscle or the
external actuator), and <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">τ</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the passive resistance
torque (from the natural elasticity and damping of human joints), as follows:

              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M77" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">τ</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">τ</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e1400">By using biomechanical models, as reported in Kuo and Deshpande (2012)
and Agarwal et al. (2013), a passive joint torque for the various
joints of the finger was calculated. To estimate the actuator's power
requirements for the fingers' extension, a rigid dynamic model of the
natural hand is developed by using ANSYS workbench software. In this
model, rigid bodies to model the hand parts, such as the lower arm, the palm, and the phalanges, have been assumed. The links between the
phalanges are described by rotational joints having fixed positions
and fixed revolute axes. The thumb movements and both the abduction
and adduction movements of the fingers are neglected. The wrist is
fixed. The joint orientation was the input, and the joint torque <inline-formula><mml:math id="M78" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> was the output. The required joint torques from the actuator to
extend the fingers joints from the relaxation state in (N mm) are
presented in Table 2. Figure 2 shows the active metacarpal phalangeal (MCP) joint torque for the index finger to extend the finger from the relaxed position (<inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">35</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>) to (<inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2"><?xmltex \currentcnt{2}?><label>Table 2</label><caption><p id="d1e1445">The required joint torque in N mm for each finger.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.95}[.95]?><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">The index</oasis:entry>
         <oasis:entry colname="col3">The middle</oasis:entry>
         <oasis:entry colname="col4">The ring</oasis:entry>
         <oasis:entry colname="col5">The small</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">MCP joint</oasis:entry>
         <oasis:entry colname="col2">42.55</oasis:entry>
         <oasis:entry colname="col3">43.15</oasis:entry>
         <oasis:entry colname="col4">41.42</oasis:entry>
         <oasis:entry colname="col5">38.93</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">PIP joint</oasis:entry>
         <oasis:entry colname="col2">6.35</oasis:entry>
         <oasis:entry colname="col3">6.546</oasis:entry>
         <oasis:entry colname="col4">6.341</oasis:entry>
         <oasis:entry colname="col5">6.042</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">DIP joint</oasis:entry>
         <oasis:entry colname="col2">0.476</oasis:entry>
         <oasis:entry colname="col3">0.476</oasis:entry>
         <oasis:entry colname="col4">0.449</oasis:entry>
         <oasis:entry colname="col5">0.385</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e1543">Active MCP joint torque of index finger for extension motion.</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Design of a cable system</title>
      <p id="d1e1560">The proposed hand rehabilitation mechanism is physically connected to
the natural hand exoskeleton, so it has a direct correspondence with
the human joints and limbs. The device has been designed to
exercise the extension motion for each finger, excluding the
thumb. Using the cable-driven system instead of rigid links decreases
the number of DOF from three to one as the linear motion of the cable
wire moves the three revolute joints of the finger instantly. The
system<?pagebreak page360?> structure has been designed independently for each finger
phalanx, as shown in Fig. 3a. A pair of small plastic links with
pulleys are used to define a specific cable path around each finger
joint. These links save the cable wire tension and prevent
injuries due to the contact between the finger skin and the
wire. These pairs of links are related to other fixed links built
above the finger to support the system and are fabricated from Teflon to
decrease the friction losses. To make the system more compact, the
actuator will be on the hand's dorsal side. The kinematic model of the
cable-driven system (CDS) was analysed to refer to the relationships
between the cable lengths and the motion of the finger.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e1565">The cable-driven mechanism.</p></caption>
        <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f03.png"/>

      </fig>

<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>The kinematic model for the wiring system</title>
      <p id="d1e1581">Cable kinematics represent the relation between cable lengths and the
fingertip end pose. The length of the force transmission cable should
be calculated in terms of the angles of the finger joints. As shown in
Fig. 3a, the linear displacement of the wire on one finger depends on
the angular displacement of each joint as follows:
            <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M81" display="block"><mml:mtable columnspacing="1em" rowspacing="0.2ex" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">M</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">D</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">6</mml:mn><mml:msub><mml:mi>l</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
          where <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the wire length, <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">M</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi>l</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are constant values, and
the values of <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and
<inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are functions of the finger joint. From Fig. 3b, we can
calculate the values of the previous parameter as follows:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M88" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E5"><mml:mtd><mml:mtext>5</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>l</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:msup><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E6"><mml:mtd><mml:mtext>6</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>H</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:msub><mml:mi>R</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mi>sin⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the length of the <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mtext>arc</mml:mtext><mml:mo>(</mml:mo><mml:mi>a</mml:mi><mml:mi>b</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> with blue colour,

                <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M91" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mi>r</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi mathvariant="normal">∅</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msup><mml:mi>sin⁡</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mi>r</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          <inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the length of the <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mtext>arc</mml:mtext><mml:mo>(</mml:mo><mml:mi>d</mml:mi><mml:mi>c</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> with green colour,

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M94" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E8"><mml:mtd><mml:mtext>8</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mi>r</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="italic">π</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">∅</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msup><mml:mi>cos⁡</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mn mathvariant="normal">4</mml:mn><mml:mi>r</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E9"><mml:mtd><mml:mtext>9</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi mathvariant="normal">∅</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mfenced open="(" close=")"><mml:mrow><mml:msup><mml:mi>cos⁡</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi>R</mml:mi><mml:mi>sin⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M95" display="inline"><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M96" display="inline"><mml:mi>r</mml:mi></mml:math></inline-formula>, <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are constant. By substituting with the same sequence for
the other two pairs of links, we can find the values of <inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> as
functions of finger joint angles.</p>
      <p id="d1e2253">To decrease the power-transmitted losses due to the cable wire
friction, the cable system has been modified depending on the robust
correlation between the motion of a proximal interphalangeal joint (PIP)
and distal interphalangeal joint (DIP), as reported by Rijpkema and
Girard (1991) and Kamper et al. (2003). Jo et al. (2019) experimented to determine this correlation and indicated the following relation:

                <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M105" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mtext>DIP</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.006</mml:mn><mml:msubsup><mml:mi mathvariant="italic">θ</mml:mi><mml:mtext>PIP</mml:mtext><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.674</mml:mn><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mtext>PIP</mml:mtext></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">0.174</mml:mn><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

          The modified system is shown in Fig. 4a, and the following
equation can enable the maximum displacement of the wire for each finger:

                <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M106" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">P</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">M</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">4</mml:mn><mml:msub><mml:mi>I</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          by calculating the difference in the wire length in both cases of the full extension and full flexion of the finger. The maximum displacement of the wires is presented in Table 3.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><?xmltex \currentcnt{3}?><label>Table 3</label><caption><p id="d1e2388">The required cable length (in millimetres) for each finger.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">The index finger</oasis:entry>
         <oasis:entry colname="col3">The middle finger</oasis:entry>
         <oasis:entry colname="col4">The ring finger</oasis:entry>
         <oasis:entry colname="col5">The small finger</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Maximum <inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>L</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">8.22 <inline-formula><mml:math id="M108" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">8.22 <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">8.12 <inline-formula><mml:math id="M110" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5">7.52 <inline-formula><mml:math id="M111" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>The cable tension force calculation</title>
      <?pagebreak page361?><p id="d1e2497">Weir (2003) indicated that the natural hand could exert an average of
95.6 <inline-formula><mml:math id="M112" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> forces at its fingertips during the power grasp motion. In
this system, the desired exerted force is only for the extension
motion of the fingers from the relaxed state, which needs much less
than this value. The cable tension force at the end of the cable
system wire <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be calculated by using
inverse kinematics as follows:

                <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M114" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi mathvariant="bold">J</mml:mi><mml:mi>T</mml:mi></mml:msup><mml:mo>⋅</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M115" display="inline"><mml:mi mathvariant="italic">τ</mml:mi></mml:math></inline-formula> is the joint torque, and <inline-formula><mml:math id="M116" display="inline"><mml:mi mathvariant="bold">J</mml:mi></mml:math></inline-formula> is the Jacobian matrix of the
cable wire, which represents the cable wire motion related to the finger
joint motion as follows:

                <disp-formula id="Ch1.E13" content-type="numbered"><label>13</label><mml:math id="M117" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mover accent="true"><mml:mi>L</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="bold">J</mml:mi><mml:mo>⋅</mml:mo><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>=</mml:mo><mml:mo>[</mml:mo><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:msup><mml:mo>]</mml:mo><mml:mi>T</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>, and

                <disp-formula id="Ch1.E14" content-type="numbered"><label>14</label><mml:math id="M119" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="bold">J</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mtable class="array" rowspacing="8.535827pt" columnalign="left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>⋅</mml:mo><mml:mi>cos⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>r</mml:mi><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mi>sin⁡</mml:mi><mml:msub><mml:mi mathvariant="italic">φ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>⋅</mml:mo><mml:mi>cos⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:mfenced open="[" close="]"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>r</mml:mi><mml:mrow><mml:msub><mml:mi>E</mml:mi><mml:mi>l</mml:mi></mml:msub><mml:mi>sin⁡</mml:mi><mml:msub><mml:mi mathvariant="italic">φ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:mfenced><mml:mi>T</mml:mi></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

          To avoid the redundancy of the mechanism, as the hand finger is a
planar 3R mechanism, the cable tension force will be calculated from the following:

                <disp-formula id="Ch1.E15" content-type="numbered"><label>15</label><mml:math id="M120" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="italic">τ</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi>J</mml:mi><mml:mo>∗</mml:mo></mml:msup><mml:mo>⋅</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

          where <inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msup><mml:mi>J</mml:mi><mml:mo>∗</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> is pseudo-inverse. Table 4 shows the required cable
tension force to extend each finger from the relaxed state to a
fully extended state. The friction force must be considered when we
calculate the required tension force as the cable is routed through
multiple segments. The friction transmission losses between the wire
cable and the system parts model by the efficiency factor <inline-formula><mml:math id="M122" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> is calculated as follows:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M123" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E16"><mml:mtd><mml:mtext>16</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E17"><mml:mtd><mml:mtext>17</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>=</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            where <inline-formula><mml:math id="M124" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula> is the coefficient of friction of the cable (<inline-formula><mml:math id="M125" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mtext>teflon</mml:mtext></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula>), and <inline-formula><mml:math id="M126" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> is the bending angle along with
the transmission. Table 5 represents the required cable tension force
in each finger to make a full extension. The proposed prototype of a
hand exoskeleton system was fabricated and assembled by using a 3D
printer. Figure 4 shows the prototype for the index finger with the
actuator that can be easily worn on the human hand.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T4"><?xmltex \currentcnt{4}?><label>Table 4</label><caption><p id="d1e2905">The required tension force (in N) for each finger.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Index finger</oasis:entry>
         <oasis:entry colname="col2">Middle finger</oasis:entry>
         <oasis:entry colname="col3">Ring finger</oasis:entry>
         <oasis:entry colname="col4">Small finger</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">3.36 <inline-formula><mml:math id="M127" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">3.41 <inline-formula><mml:math id="M128" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">3.32 <inline-formula><mml:math id="M129" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">3.3 <inline-formula><mml:math id="M130" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T5"><?xmltex \currentcnt{5}?><label>Table 5</label><caption><p id="d1e2989">The cable tension force (in N) for each finger.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <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:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Index finger</oasis:entry>
         <oasis:entry colname="col2">Middle finger</oasis:entry>
         <oasis:entry colname="col3">Ring finger</oasis:entry>
         <oasis:entry colname="col4">Small finger</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">4.18 <inline-formula><mml:math id="M131" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col2">4.24 <inline-formula><mml:math id="M132" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">4.124 <inline-formula><mml:math id="M133" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4">4.0322 <inline-formula><mml:math id="M134" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

<?xmltex \hack{\newpage}?>
</sec>
</sec>
<?pagebreak page362?><sec id="Ch1.S4">
  <label>4</label><title>The dielectric elastomer actuator</title>
      <p id="d1e3081">To supply the required tension force for the cable-driven mechanism, a
dielectric elastomer (DE) actuator has been designed and fabricated. The spring-rolled DE actuator is a linear actuator that extracts under the application of a high voltage and then returns to its original length after
releasing the voltage. So, for this application, the actuator motion
is inversely proportional to the hand finger motion, as the actuator
will be activated for fingers' flexion and deactivated for fingers'
extension.</p>
      <p id="d1e3084">A DE actuator is basically a compliant capacitor, where a soft, thin
(<inline-formula><mml:math id="M135" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>) elastomer film is sandwiched between two compliant
electrodes. When applying an electric voltage between the electrodes,
plus charges on one electrode attract minus charges on the
other. Then, electrostatic forces are the result and cause
polymer stretching. The electrostatic pressure <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
depends on the applied voltage <inline-formula><mml:math id="M137" display="inline"><mml:mi>V</mml:mi></mml:math></inline-formula> and the thickness of the DE film
<inline-formula><mml:math id="M138" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, according to the following relation:

              <disp-formula id="Ch1.E18" content-type="numbered"><label>18</label><mml:math id="M139" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub><mml:mo>×</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>V</mml:mi><mml:mi>t</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        where <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the free space permittivity (<inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mn mathvariant="normal">8.85</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:math></inline-formula>–12 <inline-formula><mml:math id="M142" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">As</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">Vm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>), and <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ε</mml:mi><mml:mi mathvariant="normal">r</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
relative dielectric constant of the elastomer. However, the DEAs
require a high voltage to work, and the supplied current is very low and
with a magnitude in micro-amperes, so there is no fear of danger in
using the high voltage as reported by Pourazadi et al. (2017).</p>
      <p id="d1e3213">Kofod (2008) indicated that the pre-strain of the DE material has a
good impact on the actuator performance and enhances the breakdown
strength. Due to the need to balance the pre-stretch of DE material
and sustain the reaction force, Kovacs et al. (2008) proposed
different methods to maintain the required pre-stretch. The spring
roll actuator represents a common solution for this problem and
achieves a large activation force with DE material. Since the force
resulting from one layer of rolled DE material is not enough,
several layers should be stacked together and warped around an elastic
compressed spring core to increase the resulting force. The balance of
the forces' reactions between the compressed spring and the pre-strained
DE material is extremely vital in preventing the failure of the actuator.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e3219"><bold>(a)</bold> The modified cable system, and <bold>(b)</bold> the prototype of a hand exoskeleton system.</p></caption>
        <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f04.png"/>

      </fig>

<sec id="Ch1.S4.SS1">
  <label>4.1</label><title>Design of the DEA</title>
      <p id="d1e3240">Amin and Assal (2018) mentioned that the suitable design DEA consists
of the main three steps. First, estimating the initial dimensions of
the actuator that can produce the target output. Second, calculating
the DE materials' pre-stretch force. Finally, selecting a suitable
compression spring that can sustain this pre-stretch force.</p><?xmltex \hack{\newpage}?>
<sec id="Ch1.S4.SS1.SSS1">
  <label>4.1.1</label><title>Determine the initial dimension of the actuator</title>
      <p id="d1e3251">By using ANSYS Multiphysics Software, a numerical simulation for the
DE actuator layers has been done to estimate the suitable dimensions
of the actuator. There are several assumptions that might be taken
into consideration while carrying out the electro-elastic analysis for
the actuator. Mainly, the roll elastomer layers are cylindrical layers
that shrink inside each other, the electrodes have no thickness and the electrode is equally distributed over all areas, except at the edges, and the electrodes are not adding any stiffness to the actuator. Several actuators with a different number of layers are being simulated under various loads.  In the beginning, roll elastomers of one layer with different thicknesses and under the same activation voltage are analysed to determine the suitable thickness of the DE layer to enable the target axial displacement. The DEA with
76 <inline-formula><mml:math id="M144" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> thickness can obtain a 35 % axial strain under a
6.5 <inline-formula><mml:math id="M145" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Kv</mml:mi></mml:mrow></mml:math></inline-formula> activation load. With this thickness, the number of
layers is gradually increased to achieve 4.5 <inline-formula><mml:math id="M146" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> at 20 layers,
with a 5 <inline-formula><mml:math id="M147" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> initial radius.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e3290">The DE actuator during the wrapping process.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f05.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e3301"><bold>(a)</bold> The schematic design of the spring roll DE actuator, and <bold>(b)</bold> the fabricated DE actuator.</p></caption>
            <?xmltex \igopts{width=312.980315pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f06.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS2">
  <label>4.1.2</label><title>Calculate the pre-stretch force of the DE material</title>
      <p id="d1e3323">By using Cauchy stress in the Cartesian coordinates, as reported by
Kovacs et al. (2007), the stresses in the pre-stretch stage are  analysed by assuming that the thickness of the pre-stretched film is
very small compared to the radius of the coil spring core and the same
previous assumptions. The wrapped elastomer film is treated as <inline-formula><mml:math id="M148" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula>
cylindrical layers wound around a spring core. For <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mi>N</mml:mi></mml:mrow></mml:math></inline-formula>,
the Cauchy stresses in the deactivated stage could be calculated from
the derivative of the strain energy potential <inline-formula><mml:math id="M150" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula>, considering
the stretch ratio <inline-formula><mml:math id="M151" display="inline"><mml:mi mathvariant="italic">λ</mml:mi></mml:math></inline-formula> as follows:

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M152" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E19"><mml:mtd><mml:mtext>19</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E20"><mml:mtd><mml:mtext>20</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi mathvariant="italic">φ</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E21"><mml:mtd><mml:mtext>21</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>z</mml:mi></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="normal">z</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mi>P</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi mathvariant="italic">φ</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, and
<inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> are stresses of layer <inline-formula><mml:math id="M156" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> in radial, circumferential, and
axial directions, respectively, and <inline-formula><mml:math id="M157" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> is a hydrostatic pressure, given
in Eq. (<xref ref-type="disp-formula" rid="Ch1.E22"/>) as follows:

                  <disp-formula id="Ch1.E22" content-type="numbered"><label>22</label><mml:math id="M158" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>P</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

            According to the Yeoh form, the terms of strain energy <inline-formula><mml:math id="M159" display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula> are related to the first invariant of the so-called left Cauchy–Green deformation tensor <inline-formula><mml:math id="M160" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula>, as follows:

                  <disp-formula id="Ch1.E23" content-type="numbered"><label>23</label><mml:math id="M161" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>W</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>I</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">20</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>I</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">30</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mi>I</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:msup><mml:mo>)</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">20</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mn mathvariant="normal">30</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are the material parameters, and the first invariant <inline-formula><mml:math id="M165" display="inline"><mml:mi>I</mml:mi></mml:math></inline-formula> is given by the following:

                  <disp-formula id="Ch1.E24" content-type="numbered"><label>24</label><mml:math id="M166" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi>I</mml:mi><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">φ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>z</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

            The following recursive equation may show that the hydrostatic pressure on the layers increases based on the accumulated number of layers and the
equilibrium condition for one layer.

                  <disp-formula id="Ch1.E25" content-type="numbered"><label>25</label><mml:math id="M167" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi>n</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>P</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi mathvariant="italic">φ</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>t</mml:mi><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>n</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M168" display="inline"><mml:mi>n</mml:mi></mml:math></inline-formula> is the layer number, and <inline-formula><mml:math id="M169" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is the radius of the layer, while
<inline-formula><mml:math id="M170" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> is the film thickness. In the activation stage, the electrostatic
pressure <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is added in the radial direction; so, it follows that:

                  <disp-formula id="Ch1.E26" content-type="numbered"><label>26</label><mml:math id="M172" display="block"><mml:mstyle class="stylechange" displaystyle="true"/><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mi>a</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi>n</mml:mi><mml:mi>a</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi>n</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">e</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

            Therefore, the Cauchy stresses in the activation stage can be given as
follows:

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M173" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E27"><mml:mtd><mml:mtext>27</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>r</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mi>a</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:msup><mml:mi>P</mml:mi><mml:mi>a</mml:mi></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E28"><mml:mtd><mml:mtext>28</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi mathvariant="italic">φ</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mi>a</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi mathvariant="italic">φ</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:msup><mml:mi>P</mml:mi><mml:mi>a</mml:mi></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E29"><mml:mtd><mml:mtext>29</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mrow><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mi>a</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>z</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:msup><mml:mi>P</mml:mi><mml:mi>a</mml:mi></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              <?xmltex \hack{\newpage}?>From Eqs. (<xref ref-type="disp-formula" rid="Ch1.E22"/>) and (<xref ref-type="disp-formula" rid="Ch1.E23"/>), the hydrostatic pressure in
the activation stage is given as follows:

                  <disp-formula id="Ch1.E30" content-type="numbered"><label>30</label><mml:math id="M174" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msup><mml:mi>P</mml:mi><mml:mi>a</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi mathvariant="italic">λ</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:msubsup><mml:mi>P</mml:mi><mml:mi>n</mml:mi><mml:mi>a</mml:mi></mml:msubsup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

            A similar recursive equation of the hydrostatic pressure  (Eq. <xref ref-type="disp-formula" rid="Ch1.E25"/>) could be applied in this activation stage. By using
th<?pagebreak page364?>e previous Eqs. (26)–(30), we can calculate the pre-stretch axial
force in the material.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><?xmltex \currentcnt{7}?><label>Figure 7</label><caption><p id="d1e4192">The electric circuit of the DE actuator. <bold>(a)</bold> The schematic diagram. <bold>(b)</bold> A photo of the electric circuit.</p></caption>
            <?xmltex \igopts{width=483.69685pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f07.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><?xmltex \currentcnt{8}?><label>Figure 8</label><caption><p id="d1e4209">The DE actuator measurements. <bold>(a)</bold> The uniaxial tension test. <bold>(b)</bold> The isometric test.</p></caption>
            <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f08.png"/>

          </fig>

</sec>
<sec id="Ch1.S4.SS1.SSS3">
  <label>4.1.3</label><title>Design spring core</title>
      <p id="d1e4233">Selecting a suitable compression spring is a very complicated step as
the spring should not only sustain the pre-stretch force of the DE
materials in the deactivation stage but also allow the actuator to
extend freely in the activation stage. In the deactivation stage, the
equilibrium force equation is as follows:

                  <disp-formula id="Ch1.E31" content-type="numbered"><label>31</label><mml:math id="M175" display="block"><mml:mstyle displaystyle="true" class="stylechange"/><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo movablelimits="false">∑</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>k</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

            where <inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the axial DE material force under the
deactivation stage that equals to the pre-stretch force,
<inline-formula><mml:math id="M177" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> is the spring
constant, and <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the initially compressed displacement of
spring. The equilibrium equation in the activation stage is as follows:

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M179" display="block"><mml:mtable displaystyle="true"><mml:mlabeledtr id="Ch1.E32"><mml:mtd><mml:mtext>32</mml:mtext></mml:mtd><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo movablelimits="false">∑</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>k</mml:mi><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr><mml:mlabeledtr id="Ch1.E33"><mml:mtd><mml:mtext>33</mml:mtext></mml:mtd><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>≤</mml:mo><mml:mi>x</mml:mi><mml:mo>≤</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where the <inline-formula><mml:math id="M180" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the activation force, <inline-formula><mml:math id="M181" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M182" display="inline"><mml:mi>a</mml:mi></mml:math></inline-formula> are
the axial displacement and acceleration, respectively, and <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the
displacement under the fully activated voltage.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T6" specific-use="star"><?xmltex \currentcnt{6}?><label>Table 6</label><caption><p id="d1e4423">The constructional parameters of the spring roll DE actuator.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <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:tbody>
       <oasis:row>
         <oasis:entry colname="col1">DE actuator dimension</oasis:entry>
         <oasis:entry colname="col2">Length (L)</oasis:entry>
         <oasis:entry colname="col3">10 <inline-formula><mml:math id="M184" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Outer diameter</oasis:entry>
         <oasis:entry colname="col3">10 <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Number of layers</oasis:entry>
         <oasis:entry colname="col3">20</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Activation voltage</oasis:entry>
         <oasis:entry colname="col3">6.5 <inline-formula><mml:math id="M186" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Kv</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">DE materials specification</oasis:entry>
         <oasis:entry colname="col2">Type</oasis:entry>
         <oasis:entry colname="col3">Acrylic VHB 4910</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Initial thickness</oasis:entry>
         <oasis:entry colname="col3">1 <inline-formula><mml:math id="M187" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Pre-strain ratio</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.14</mml:mn><mml:mo>×</mml:mo><mml:mn mathvariant="normal">4.2</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spring core dimension</oasis:entry>
         <oasis:entry colname="col2">Outer diameter</oasis:entry>
         <oasis:entry colname="col3">10 <inline-formula><mml:math id="M189" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Stiffness</oasis:entry>
         <oasis:entry colname="col3">340 <inline-formula><mml:math id="M190" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">mm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">DE actuator output</oasis:entry>
         <oasis:entry colname="col2">Blocked force</oasis:entry>
         <oasis:entry colname="col3">4.35 <inline-formula><mml:math id="M191" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Maximum displacement</oasis:entry>
         <oasis:entry colname="col3">11.3 <inline-formula><mml:math id="M192" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><label>Figure 9</label><caption><p id="d1e4643">The result of the uniaxial tension test.</p></caption>
            <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f09.png"/>

          </fig>

</sec>
</sec>
<sec id="Ch1.S4.SS2">
  <label>4.2</label><title>Fabrication of the DEA</title>
      <p id="d1e4661">The fabrication process of the spring roll dielectric elastomer
actuator was done manually and consisted of three main processes:
<list list-type="bullet"><list-item>
      <p id="d1e4666">Acrylic films of VHB 4910 (1 <inline-formula><mml:math id="M193" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>) are used since they are
commercially available and offer a strong adhesiveness, which
simplifies the manufacturing of actuators. As the pre-strain of DE
materials is an essential step, due to enhancing the electric breakdown
strength of the material, two layers of a commercial DEMs (3M VHB 4910
tape) were biaxially stretched and fixed on the acrylic frame until the
the electrode layer was added.</p></list-item><list-item>
      <p id="d1e4678">A conductive carbon grease was introduced as the electrode material. It is characterized by low tensile stiffness and electrical conductivity, and it allows continuous contact with the adjacent film layers. The electrode layers are manually put on to both sides of one pre-stretch DE layer, as shown in Fig. 5. The copper conductive tape was used to connect the electricity to the two electrodes. After adding the electrode layers, the two pre-stretch layers are stacked together and fixed onto the frame.</p></list-item><list-item>
      <p id="d1e4682">By using plastic caps with a telescopic cylinder and screw hub, the
spring core is compressed. A thin latex layer covers the spring
outside surface to prevent<?pagebreak page366?> contact with the electrode layer. Then
wrapped manually around a compressed spring as shown in Fig. 5.</p></list-item></list></p>
      <p id="d1e4685">Figure 6 shows a schematic configuration and a fabricated prototype of the DE actuator. Table 6 lists the specifications of the required DEA for the hand rehabilitation system. As the actuator works under high-voltage activation, there are several points that must be taken into consideration. The EMCO high voltage (HV) DC–DC converter has been used to supply the high voltage. This converter is characterized by a lower output current (167 <inline-formula><mml:math id="M194" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:mrow></mml:math></inline-formula>), which guarantees the safety of the user. It was controlled by using a digital potentiometer and Arduino software, as shown in Fig. 7. While the actuator is basically a capacitor, a dissipation circuit with 100 <inline-formula><mml:math id="M195" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">M</mml:mi><mml:mi mathvariant="normal">Ω</mml:mi></mml:mrow></mml:math></inline-formula> resistance and high-voltage relays (to avoid sparks) is used. A high-voltage diode was connected to the output of the HV DC converter to prevent current reversal.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><?xmltex \currentcnt{10}?><label>Figure 10</label><caption><p id="d1e4710">The result of the isotonic test.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f10.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><?xmltex \currentcnt{11}?><label>Figure 11</label><caption><p id="d1e4722">The result of the isometric test.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://ms.copernicus.org/articles/11/357/2020/ms-11-357-2020-f11.png"/>

        </fig>

<?xmltex \hack{\newpage}?>
</sec>
</sec>
<sec id="Ch1.S5">
  <label>5</label><title>DEA characterization</title>
      <p id="d1e4743">In order to determine the actuator performance, uniaxial tension tests
in the deactivated stage and isotonic and isometric tests in the
activated stage have been carried out. The isotonic test gives the
relative change in the actuator's length vs. the voltage under a
constant load. The isometric test measures the resulting force vs. the
voltage, while the actuator's length remains constant.</p>
<sec id="Ch1.S5.SS1">
  <label>5.1</label><title>Measurement setup</title>
      <p id="d1e4753">During the uniaxial tensile force, the actuator is hung from a rigid
support, and weights are attached at the lower end to keep the
initial pre-stretch, as shown in Fig. 8a. The weight load gradually increased by steps equal to 50 <inline-formula><mml:math id="M196" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula>, and the
displacement was measured by using a digital Vernier caliper with
a 0.01 <inline-formula><mml:math id="M197" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> resolution. In this way, the actuator does not move
until the axial load equals the pre-stretch force of the<?pagebreak page367?> material. For
this research, the compressed spring must sustain the pre-stretch
force so that the actuator moves under applied loads.</p>
      <p id="d1e4772">With the same technique, the axial displacement due to the activation
voltage in the isotonic test has been measured by applying voltage
incrementally. An isometric test was done to measure the resulting
axial force of the actuator under an activation voltage with blocked
strain. The actuator was fixed axially, and the axial force was
measured by increasing the applied voltage by using force sensors
attached to one end of the actuator, as shown in Fig. 8b. The actuator
was blocked in its deactivated length by applying a linear increased
DC voltage from 0 to 6.5 <inline-formula><mml:math id="M198" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Kv</mml:mi></mml:mrow></mml:math></inline-formula>, and the compression blocked force
was measured.</p>
</sec>
<sec id="Ch1.S5.SS2">
  <label>5.2</label><title>Measurement results and discussion</title>
      <p id="d1e4791">Several spring roll DE actuators in different groups were fabricated
and tested. The relation between the applied force and displacement  seemed to be a quasi-linear relation, as shown in Fig. 9. For the
uniaxial test, the displacement increased linearly to achieve
2 <inline-formula><mml:math id="M199" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> at 12.5 <inline-formula><mml:math id="M200" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula>. The stiffness of the actuator equalled
610 <inline-formula><mml:math id="M201" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e4827">When applied to the high voltage in the DEA, the axial displacement
increases gradually with the voltage. The actuator raises to its
maximum displacement, equal to 11.3 <inline-formula><mml:math id="M202" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>, when
6.5 <inline-formula><mml:math id="M203" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Kv</mml:mi></mml:mrow></mml:math></inline-formula> voltage is applied. As shown in Fig. 10, the experimental and numerical results are approximately the same.</p>
      <?pagebreak page368?><p id="d1e4846">Figure 11 shows that the actuator achieved its maximum compressive
blocking force of 4.35 <inline-formula><mml:math id="M204" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula> at its passive equilibrium length of
9 <inline-formula><mml:math id="M205" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula>. When the displacement reached a displacement of
11.3 <inline-formula><mml:math id="M206" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>, this blocking force decreased to 0 <inline-formula><mml:math id="M207" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula>. This
displacement of 11.3 <inline-formula><mml:math id="M208" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula> represented the maximum displacement
of the actuator.</p>
      <p id="d1e4889">While the DEA achieved the target requirement output, some points
must be taken into consideration. First, it is highly recommended that one uses a fully automated fabrication process to limit damage during
the fabrication process. Also, using dielectric elastomer material,
which is prepared and fabricated for actuator purposes, will provide a
positive result and decrease the probability of material damage.</p>
</sec>
</sec>
<sec id="Ch1.S6" sec-type="conclusions">
  <label>6</label><title>Conclusions</title>
      <p id="d1e4901">The design of a soft hand rehabilitation system, based on a cable-driven
mechanism, to exercise the fingers' extension movements was
proposed. A kinematic and dynamic analysis of the human hand was
obtained to determine the required torque to extend the fingers. The
cable-driven design was analysed, and a prototype of the system was
fabricated and assembled. The dielectric elastomer actuator was
introduced as a smart actuator for the system. Theoretical analysis of
the actuator was done to choose its suitable parameter. Several DE
actuators were fabricated manually. Uniaxial, isotonic, and isometric
tests for DE actuator were done to characterize the actuator's
performance. A spring roll dielectric elastomer actuator with maximum
axial displacement (11.3 <inline-formula><mml:math id="M209" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mm</mml:mi></mml:mrow></mml:math></inline-formula>) and maximum axial force
(4.35 <inline-formula><mml:math id="M210" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">N</mml:mi></mml:mrow></mml:math></inline-formula>) was produced. The number of the required DE
actuators for the hand rehabilitation system is four, as each actuator
can only move one finger.</p>
</sec>
<sec id="Ch1.S7">
  <label>7</label><title>Future work</title>
      <p id="d1e4928">Future work will focus on evaluating the performance of the
cable-driven system on several patients. The evaluation will include
its efficacy, safety, and comfort.</p>
</sec>

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

      <p id="d1e4935">The data in this study can be requested from the corresponding author.</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e4941">HA did all of the work for this research under the
supervision of SFMA and HI.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e4947">The authors declare that they have no conflict of interest.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e4953">This paper was edited by Chin-Hsing Kuo and reviewed by two anonymous referees.</p>
  </notes><?xmltex \hack{\newpage}?><ref-list>
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<abstract-html><p>The increasing number of patients with hand disabilities after strokes or peripheral nerve injuries necessitates the continuous development of rehabilitation system devices to accelerate muscle recovery and to help patients regain the motor functions of their hands. This paper introduces the design of a hand rehabilitation system for patients who have a solitary impairment of their hand extension. The system was designed to be portable, simple, and cheap. Using a system based on a cable-driven mechanism instead of traditional rigid links reduces the degrees of freedom of the finger to one. The dielectric elastomer actuator was designed and fabricated as a smart actuator for the system, which supports the low cost of the system. A kinematic analysis of the cable-driven mechanism has been done. Parameters of the actuator were optimized to reach the required output. In order to characterize the performance of the actuator, a uniaxial tension test, isotonic test, and isometric test have been implemented.</p></abstract-html>
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</mixed-citation></ref-html>--></article>
