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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>A New Approach Based on Neural Network for a 3d Reconstruction of the Dome of a Bulge Tested Specimen</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Damiano Alizzio</string-name>
          <email>damiano.alizzio@unime.it</email>
          <xref ref-type="aff" rid="aff2">2</xref>
          <xref ref-type="aff" rid="aff3">3</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Fabio Lo Savio</string-name>
          <email>flosavio@diim.unict.it</email>
          <xref ref-type="aff" rid="aff1">1</xref>
          <xref ref-type="aff" rid="aff3">3</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Marco Bonfanti</string-name>
          <email>bonfa.marco@tiscali.it</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff3">3</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Guido Garozzo</string-name>
          <xref ref-type="aff" rid="aff3">3</xref>
          <xref ref-type="aff" rid="aff4">4</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Electrical, Electronic and Computer Engineering, University of Catania</institution>
          ,
          <addr-line>Catania, CT</addr-line>
          ,
          <country country="IT">Italy</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Dip. di Ing. Civile e Architettura, Università di Catania</institution>
          ,
          <addr-line>Catania, CT</addr-line>
          ,
          <country country="IT">Italy</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Dip. di Ingegneria, Università degli Studi di Messina</institution>
          ,
          <addr-line>C.da Di Dio, 98166 Sant'Agata, Messina</addr-line>
          ,
          <country country="IT">Italy</country>
        </aff>
        <aff id="aff3">
          <label>3</label>
          <institution>ICYRIME 2020: International Conference for Young Researchers in Informatics, Mathematics, and Engineering</institution>
          ,
          <addr-line>Online</addr-line>
        </aff>
        <aff id="aff4">
          <label>4</label>
          <institution>Zerodivision Systems S.r.l.</institution>
          ,
          <addr-line>Piazza S. Francesco n. 1, 56127 Pisa</addr-line>
          ,
          <country country="IT">Italy</country>
        </aff>
      </contrib-group>
      <fpage>54</fpage>
      <lpage>58</lpage>
      <abstract>
        <p>A three-dimensional reconstruction of the dome formed by a thin hyperelastic specimen during a creep bulge test was carried out through two diferent techniques: stereoscopic reconstruction based on epipolar geometry and Digital Image Correlation. A suitable experimental device, provided with a sliding crossbar for acquiring dome images so to detect its strain state, was used for the epipolar geometric reconstruction. In 3D reconstruction based on the Digital Image Correlation, the cameras/sliding crossbar system was replaced by a diferent optical system. A new approach to exploit the greater accuracy obtained with Digital Image Correlation, using cheaper techniques, was based on the training of a Convolution Neural Network. This training consisted in using a set of points (x, y) of the specimen at diferent pressure values in order to obtain a heights (z) map of the dome. This approach is aimed to reconstruct the dome providing to the Network thus trained the images from a single camera placed on the vertical axis of the dome apex.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;Bulge Test</kwd>
        <kwd>Hyperelastic</kwd>
        <kwd>Epipolar</kwd>
        <kwd>3D-DIC</kwd>
        <kwd>Neural Network</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        verted into stress and strain values. Some of the
authors have already published a mobile crosshead
deNowadays elastomers are widely used in the automo- vice capable of subjecting a membrane to the bulge test
tive and mechanical industries to make tires, hydraulic in force control (creep) [
        <xref ref-type="bibr" rid="ref5 ref6">5, 6</xref>
        ].
or pneumatic drive units, hydraulic hoses, anti-vibrat- In this study, the three-dimensional reconstruction
ion mounts, pneumatic and hydraulic shock absorbers. of the dome of a bulge-tested specimen was performed
      </p>
      <p>
        These materials exhibit large deformations with high- with two diferent techniques: stereoscopic
reconstrucly non-linear hyperelastic behavior [
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. The mechan- tion based on epipolar geometry and Digital Image
Corical characterization, aimed at defining the hyperelas- relation (DIC) [
        <xref ref-type="bibr" rid="ref7 ref8">7, 8</xref>
        ]. The data obtained from the
lattic constants describing the behavior of elastomers, re- ter methodology were used to properly train a
convoquires the use of diferent types of tests. Among these, lutional neural network (CNN). The neural network
the bulge test is a consolidated technique for the study thus trained will be able to reconstruct the dome on
of membranes subjected to an equibiaxial tension state the basis of frames from a single camera placed on the
[
        <xref ref-type="bibr" rid="ref2 ref3 ref4">2, 3, 4</xref>
        ]; this test can also avoid the damage that can vertical axis of the apex dome, while maintaining the
occur on the edges when the specimen is stressed dur- level of accuracy achieved with 3D-DIC in the training
ing other types of tests. phase. This involves an obvious saving both temporal
      </p>
      <p>
        The bulge test consists in fixing a thin specimen be- and economical.
tween two circular flanges with holes in the center to
allow, through the insuflation of fluid inside the test
chamber, the inflation and therefore the deformation 2. Materials and Methods
of the material. During inflation, the characteristic
parameters of the test are monitored: pressure and
displacements. The data thus obtained will then be
conThe material tested in this study is SBR 20% carbon
black-filled that is an artificial rubber widely used for
making tires, seals and shoe soles [
        <xref ref-type="bibr" rid="ref10 ref11 ref9">9, 10, 11</xref>
        ]. A set
of 10 square specimens (180  × 180  ) were cut
from a single sheet of elastomer having a thickness of
3 mm. Each specimen presented a diferent pattern
on each of the two faces (Fig. 1). On the first,
useful for the epipolar reconstruction, a grid consisting
of five concentric circles ( parallels) was silk-screened,
a small central circle whose center corresponded to
the top of the dome and 73 equidistant rays
(meridians) radiating from the center. On the second face, on
which to carry out the 3D-DIC, a pattern of random
spots of white paint was airbrushed (with nozzle
diameter  = 0.18  ). In this way, spots obtained had
an average diameter  = 0.23  and a relative
surface  = 0.042  2.
      </p>
      <p>The bulge test technique is based on some restrictive
assumptions both on the tested material (isotropy and
incompressibility) and on the geometry of the inflated
specimen (hemispherical shape and reduced thickness
compared to the radius of curvature). Under these
assumptions, the stress state can be considered plane and
equibiaxial, allowing the Boyle-Mariotte law, valid for
thin-walled tanks, to be applied:
  =   =
 ⋅ 
2 ⋅ 
(1)
(2)
where  0 is the initial thickness of the specimen.</p>
      <p>(3)</p>
    </sec>
    <sec id="sec-2">
      <title>3. Experimental Setup</title>
      <p>The experimental setup (Fig. 2) consists of a bulge
chamber, inflated by a compressed air system
allowcrossbar to which two cameras are fixed to detect the
equibiaxial strain of the specimen.</p>
      <p>The mobile crosshead device, controlled by an
optical system, moves the fixed focus cameras following
the inflation of the specimen. This means that the
dimensions of the captured images depend exclusively
on the deformation at the dome and not on its
approaching to the camera lenses. The measurement of
the equibiaxial deformation (  ), according to the eq.
(2), is obtained by comparing the distances between
two homothetic markers relative to two successive
instants during the creep of the material (Fig. 3). To
mea, were acquired for each image.
length</p>
      <p>mations are:
R is the radius of curvature of the dome and p is the
inflation pressure.</p>
      <p>At the apex of the dome each meridian is a main
direction and the stress state is equibiaxial. Therefore,
on the surface of the dome the main deformations are
equal to each other ( 1 =  2 =  
edge of the undeformed length
). From the
knowland the deformed
of a membrane finite element, these
defor</p>
      <p>1 =  2 = 
where   and   are, respectively, the
circumferential and axial tension, s is the thickness at the apex, ing to accurately adjust the pressure, and of a mobile</p>
      <p>
        From the equation of the well-known equivalent de- sure the displacement more accurately 33 samples, at
formation of Von Mises, respecting the assumption of a sample rate of 1  
incompressibility of the material [
        <xref ref-type="bibr" rid="ref12">12</xref>
        ]:
The acquisition time was equal to 1/30  ,
corresponding to the camera frame rate. During each acquisition,
the average of the 33 values, as a representative value,
and the standard deviation of the series were
calculated. The resulting synchronization uncertainty was
1/30  , equal to the phase shift of a single frame.
Moreover, the displacement signal will be less afected by
the electronic noise.
      </p>
      <p>In order to achieve the 3D reconstruction based on
DIC, GOM ARAMIS 2M LT optical system replaced the
device with cameras/sliding crossbar (Fig. 4).</p>
      <p>Figures 5a and 5b show the three-dimensional
reconstructions obtained through epipolar geometry and
3D-DIC, respectively. The creep-test was performed
by inflating air into the chamber as quickly as possible
until reaching a pressure of 75 kPa, keeping it constant
for the entire test period (Fig. 6a). This value, much
lower than the breaking pressure of the specimen,
allowed to fall within the elastic range so that the two
faces of the specimen could be tested with the
measurement methods adopted. Fig. 6b shows the creep
strains measured with the two methods adopted.</p>
    </sec>
    <sec id="sec-3">
      <title>4. Description and Training of the Neural Network</title>
      <p>
        The architecture of the CNN is largely used in
computer vision problems. The main structure used is the
Inverted Bottleneck as residual block that allows
having a good performance together with limited impact
on the hardware [
        <xref ref-type="bibr" rid="ref13">13</xref>
        ].
      </p>
      <p>In this study, a CNN was trained with data extracted
from the mesh generated by the 3D-DIC system (Fig.
7).</p>
      <p>
        The CNN was trained in PyTorch [
        <xref ref-type="bibr" rid="ref14">14</xref>
        ] through the
ADAM optimizer and the Mean Squared Error (MSE)
as loss function for 100 epochs with an initial learning
rate (  ) of 0.001 and batch size of 4. The weight decay
was set to 10−5 and   was scaled of 0.1 after 20 and 90
epochs.
      </p>
      <p>To achieve the heights (z) map prediction, the CNN
needed 9 coordinate points (x, y) per creep test as
input: 8 points from the intersection of meridians 1, 19, Figure 8: CNN reconstruction of the dome.
37, 56 and parallels 2 and 3; 1 from the apex of the
dome. In addition, the current pressure was required.
by the value of 0.0147 found, over the testing set, for
5. Results and Conclusion the mean square error among test and train curves.
The application of the CNN neural network has
provFig. 8 shows the dome reconstructed by the CNN neu- ed useful both from the point of view of time and
ecoral network reached after a learning time of 100 epochs. nomic savings. In fact, the reconstruction of the dome
The good performance of this network is highlighted can be performed simply based on the frames of a
single camera placed on the vertical axis of the dome apex,
thus ensuring the same level of accuracy achieved with
3D-DIC in the training phase.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          [1]
          <string-name>
            <given-names>M. C.</given-names>
            <surname>Boyce</surname>
          </string-name>
          ,
          <string-name>
            <given-names>E. M.</given-names>
            <surname>Arruda</surname>
          </string-name>
          ,
          <article-title>Constitutive models of rubber elasticity: A review</article-title>
          ,
          <source>Rubber Chemistry and Technology</source>
          <volume>73</volume>
          (
          <year>2000</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          [2]
          <string-name>
            <given-names>J.-Y.</given-names>
            <surname>Sheng</surname>
          </string-name>
          , L.-Y. Zhang,
          <string-name>
            <given-names>G.-F.</given-names>
            <surname>Li</surname>
          </string-name>
          , Bo; Wang,
          <string-name>
            <given-names>X.- Q.</given-names>
            <surname>Feng</surname>
          </string-name>
          ,
          <article-title>Bulge test method for measuring the hyperelastic parameters of soft membranes</article-title>
          ,
          <source>Acta Mechanica</source>
          (
          <year>2017</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          [3]
          <string-name>
            <given-names>T.</given-names>
            <surname>Tsakalakos</surname>
          </string-name>
          ,
          <article-title>The bulge test: A comparison of the theory and experiment for isotropic and anisotropic films</article-title>
          ,
          <source>Thin Solid Films</source>
          <volume>75</volume>
          (
          <year>1981</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          [4]
          <string-name>
            <given-names>K.</given-names>
            <surname>Muammer</surname>
          </string-name>
          ,
          <string-name>
            <given-names>B.</given-names>
            <surname>Eren</surname>
          </string-name>
          ,
          <string-name>
            <given-names>N. C.</given-names>
            <surname>Ömer</surname>
          </string-name>
          ,
          <article-title>An experimental study on the comparative assessment of hydraulic bulge test analysis methods</article-title>
          ,
          <source>Materials &amp; Design</source>
          <volume>32</volume>
          (
          <year>2011</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          [5]
          <string-name>
            <given-names>F.</given-names>
            <surname>Lo Savio</surname>
          </string-name>
          , G. Capizzi,
          <string-name>
            <given-names>G.</given-names>
            <surname>La Rosa</surname>
          </string-name>
          ,
          <string-name>
            <surname>G.</surname>
          </string-name>
          <article-title>Lo Sciuto, Creep assessment in hyperelastic material by a 3d neural network reconstructor using bulge testing</article-title>
          ,
          <source>Polymer Testing</source>
          <volume>63</volume>
          (
          <year>2017</year>
          ).
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          [6]
          <string-name>
            <given-names>M.</given-names>
            <surname>Calì</surname>
          </string-name>
          ,
          <string-name>
            <given-names>F. L.</given-names>
            <surname>Savio</surname>
          </string-name>
          ,
          <article-title>Accurate 3d reconstruction of a rubber membrane inflated during a bulge test to evaluate anisotropy</article-title>
          ,
          <source>in: Advances on Mechanics, Design Engineering and Manufacturing</source>
          , Springer,
          <year>2017</year>
          , pp.
          <fpage>1221</fpage>
          -
          <lpage>1231</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          [7]
          <string-name>
            <given-names>H.</given-names>
            <surname>Schreier</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.-J.</given-names>
            <surname>Orteu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M. A.</given-names>
            <surname>Sutton</surname>
          </string-name>
          , et al.,
          <article-title>Image correlation for shape, motion and deformation measurements: Basic concepts</article-title>
          ,
          <source>theory and applications</source>
          , volume
          <volume>1</volume>
          , Springer,
          <year>2009</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref8">
        <mixed-citation>
          [8]
          <string-name>
            <given-names>J.</given-names>
            <surname>Neggers</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Hoefnagels</surname>
          </string-name>
          ,
          <string-name>
            <given-names>F.</given-names>
            <surname>Hild</surname>
          </string-name>
          ,
          <string-name>
            <given-names>S.</given-names>
            <surname>Roux</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M.</given-names>
            <surname>Geers</surname>
          </string-name>
          ,
          <article-title>Global digital image correlation for pressure deflected membranes</article-title>
          , in: G. A.
          <string-name>
            <surname>Shaw</surname>
            ,
            <given-names>B. C.</given-names>
          </string-name>
          <string-name>
            <surname>Prorok</surname>
            ,
            <given-names>L. A.</given-names>
          </string-name>
          <string-name>
            <surname>Starman</surname>
          </string-name>
          (Eds.),
          <source>MEMS and Nanotechnology</source>
          , Volume
          <volume>6</volume>
          , Springer New York, New York, NY,
          <year>2013</year>
          , pp.
          <fpage>135</fpage>
          -
          <lpage>140</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref9">
        <mixed-citation>
          [9]
          <string-name>
            <given-names>F.</given-names>
            <surname>Lo Savio</surname>
          </string-name>
          ,
          <string-name>
            <given-names>G.</given-names>
            <surname>La Rosa</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M.</given-names>
            <surname>Bonfanti</surname>
          </string-name>
          ,
          <article-title>A new theoretical-experimental model deriving from the contactless measurement of the thickness of bulge-tested elastomeric samples</article-title>
          ,
          <source>Polymer Testing</source>
          <volume>87</volume>
          (
          <year>2020</year>
          ). doi:
          <volume>10</volume>
          .1016/j. polymertesting.
          <year>2020</year>
          .
          <volume>106548</volume>
          .
        </mixed-citation>
      </ref>
      <ref id="ref10">
        <mixed-citation>
          [10]
          <string-name>
            <given-names>F.</given-names>
            <surname>Lo Savio</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M.</given-names>
            <surname>Bonfanti</surname>
          </string-name>
          ,
          <string-name>
            <given-names>G.</given-names>
            <surname>Grasso</surname>
          </string-name>
          ,
          <string-name>
            <given-names>D.</given-names>
            <surname>Alizzio</surname>
          </string-name>
          ,
          <article-title>An experimental apparatus to evaluate the nonlinearity of the acoustoelastic efect in rubberlike materials</article-title>
          ,
          <source>Polymer Testing</source>
          <volume>80</volume>
          (
          <year>2019</year>
          ). doi:
          <volume>10</volume>
          . 1016/j.polymertesting.
          <year>2019</year>
          .
          <volume>106133</volume>
          .
        </mixed-citation>
      </ref>
      <ref id="ref11">
        <mixed-citation>
          [11]
          <string-name>
            <given-names>F.</given-names>
            <surname>Lo Savio</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M.</given-names>
            <surname>Bonfanti</surname>
          </string-name>
          ,
          <article-title>A novel device for measuring the ultrasonic wave velocity and the thickness of hyperelastic materials under quasi-static deformations</article-title>
          ,
          <source>Polymer Testing</source>
          <volume>74</volume>
          (
          <year>2019</year>
          )
          <fpage>235</fpage>
          -
          <lpage>244</lpage>
          . doi:
          <volume>10</volume>
          .1016/j.polymertesting.
          <year>2019</year>
          .
          <volume>01</volume>
          .005.
        </mixed-citation>
      </ref>
      <ref id="ref12">
        <mixed-citation>
          [12]
          <string-name>
            <given-names>M.</given-names>
            <surname>Sasso</surname>
          </string-name>
          , G. Palmieri,
          <string-name>
            <given-names>G.</given-names>
            <surname>Chiappini</surname>
          </string-name>
          ,
          <string-name>
            <given-names>D.</given-names>
            <surname>Amodio</surname>
          </string-name>
          ,
          <article-title>Characterization of hyperelastic rubber-like materials by biaxial and uniaxial stretching tests based on optical methods</article-title>
          ,
          <source>Polymer Testing</source>
          <volume>27</volume>
          (
          <year>2008</year>
          )
          <fpage>995</fpage>
          -
          <lpage>1004</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref13">
        <mixed-citation>
          [13]
          <string-name>
            <given-names>M.</given-names>
            <surname>Sandler</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A.</given-names>
            <surname>Howard</surname>
          </string-name>
          ,
          <string-name>
            <given-names>M.</given-names>
            <surname>Zhu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A.</given-names>
            <surname>Zhmoginov</surname>
          </string-name>
          , L. Chen,
          <article-title>Mobilenetv2: Inverted residuals and linear bottlenecks</article-title>
          ,
          <source>in: 2018 IEEE/CVF Conference on Computer Vision and Pattern Recognition</source>
          ,
          <year>2018</year>
          , pp.
          <fpage>4510</fpage>
          -
          <lpage>4520</lpage>
          . doi:
          <volume>10</volume>
          .1109/CVPR.
          <year>2018</year>
          .
          <volume>00474</volume>
          .
        </mixed-citation>
      </ref>
      <ref id="ref14">
        <mixed-citation>
          [14]
          <string-name>
            <given-names>A.</given-names>
            <surname>Paszke</surname>
          </string-name>
          , et al.,
          <article-title>Pytorch: An imperative style, high-performance deep learning library</article-title>
          , in: H.
          <string-name>
            <surname>Wallach</surname>
            ,
            <given-names>H.</given-names>
          </string-name>
          <string-name>
            <surname>Larochelle</surname>
            ,
            <given-names>A.</given-names>
          </string-name>
          <string-name>
            <surname>Beygelzimer</surname>
            ,
            <given-names>F.</given-names>
          </string-name>
          <article-title>d'Alché-</article-title>
          <string-name>
            <surname>Buc</surname>
            ,
            <given-names>E.</given-names>
          </string-name>
          <string-name>
            <surname>Fox</surname>
          </string-name>
          , R. Garnett (Eds.),
          <source>Advances in Neural Information Processing Systems</source>
          <volume>32</volume>
          ,
          <string-name>
            <surname>Curran</surname>
            <given-names>Associates</given-names>
          </string-name>
          , Inc.,
          <year>2019</year>
          , pp.
          <fpage>8026</fpage>
          -
          <lpage>8037</lpage>
          .
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>