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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Hardware and software implementation of a parallel-plates rotational rheometer</article-title>
      </title-group>
      <contrib-group>
        <aff id="aff0">
          <label>0</label>
          <institution>Guendalina Nicoletti Department of Civil Engineering and Architecture University of Catania</institution>
          ,
          <country country="IT">Italy</country>
        </aff>
      </contrib-group>
      <fpage>8</fpage>
      <lpage>13</lpage>
      <abstract>
        <p>-A rotational strain controlled rheometer with parallel-plate was designed and realized in SMT configuration, which allows exhaustively to characterize materials having highly viscoelastic properties. In this particular case, composite materials, reinforced by dispersed particles, were tested: they are constituted by the elastomer polydimethylsiloxane (PDMS), with addition of different filler concentrations, in particular carbon black, electrically conductive elastomers useful in electronic devices.The study of rheological material properties can contribute to the better realization and manufacturing process of the product. Since the dynamic properties evaluation has been done through oscillatory testing at fixed range of frequencies, in order to measure the complex modulus G* of the material. Index Terms-Rheometer, Complex modulus G*, Viscoelastic, Carbon black Fig. 1. 3D CAD model Solidworks of rheometer and its realization</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>I. INTRODUCTION</title>
      <p>
        The linear viscoelasticity theory is a prerequisite for the
understanding of the rheological characteristic of many materials
[
        <xref ref-type="bibr" rid="ref1">1</xref>
        ]. Defining a viscoelastic system by properties intermediate
between solid and a fluid. A dissipation of internal energy
and hence the stress - deformation deviation usually are
verified in two phases interaction of solid - liquid and elastic
- viscose, respect to a perfectly elastic state. In fact, a perfect
elastic response requires a potential energy acquired during
deformation phase,restoring it totally in order to observe the
transformation reversibility [
        <xref ref-type="bibr" rid="ref2">2</xref>
        ], [
        <xref ref-type="bibr" rid="ref3">3</xref>
        ], [
        <xref ref-type="bibr" rid="ref4">4</xref>
        ].
      </p>
      <p>
        The major or lesser influence of the solid matrix on liquid
phase causes an infinite variety of viscoelastic responses,
whose extreme limits are the solid pure elastic and viscous
fluid. Afterwards the main viscoelastic mathematical relations
are explained widely in rheological analysis. In the physical
phenomena, the real materials are identified with a continuous
homogeneous and isotropic model [
        <xref ref-type="bibr" rid="ref5">5</xref>
        ].
      </p>
      <p>
        The study of the rheological properties and viscosity
measurement arise for exploration of materials dynamic
behavior; a special equipment called rheometers are used to this
purporse, which generally allow to measure dynamics (forces
and torques) and kinematics (displacement, velocity and time)
variables [
        <xref ref-type="bibr" rid="ref6">6</xref>
        ], [
        <xref ref-type="bibr" rid="ref7">7</xref>
        ]. Rheological quantity is obtained by
mathematical equation solutions and experimental test, considering
also some geometric parameters of the used instrument and
physical parameters of tested material.
      </p>
      <p>Copyright c 2017 held by the authors.</p>
      <p>For instance, the polymeric materials are characterized by
complex rheological properties, in particular for flow
conditions in real applications. For this reason in the laboratory
are created simple kinematically flow situations and easily
controllable.</p>
      <p>Operational protocols definition and processing of
experimental results are fondamental for execution of rheological
tests. Usually the rheological properties of polymers such as
elastic, viscous and viscoelastic are typically determined using
equipment operating in sweep frequencies, including the DSR
Dyanamic Shear Rheometer. An independent variable, called
forcing, varies over the time, and in general is considered a
stress, deformation or deformation gradient.</p>
    </sec>
    <sec id="sec-2">
      <title>II. HARDWARE IMPLEMENTATION</title>
      <p>
        The strain controlled rotational rheometer are constituted by
two parallel plates, the bottom plate is moved by a
steppermotor, which allows to apply a predetermined rotation speed,
which thus determines a sliding flow inside the fluid interposed
between the two plates. This motor can apply a torque in both
directions, generating the oscillatory stresses; in this case the
device can control both the intensity of the deformation that
its frequency [
        <xref ref-type="bibr" rid="ref8">8</xref>
        ], [
        <xref ref-type="bibr" rid="ref9">9</xref>
        ].
      </p>
      <p>The phase shift between the deformation and stress is
determined by the transducer to measure the torque keeping
the plate in motion, obtaining the stress undergone by fluid.</p>
      <p>The measurement of viscoelastic properties have been
analized at different frequencies using the rotational rheometer
made in laboratory.
The undercarriage of the testing machine is structured on
one central axis, constituted by beams made of metal, with the
L shape , fixed on a wooden base, which had been carried out
to integrate to the test bench so as in order to reduce vibrations
and oscillations during the testing.</p>
      <p>The lower part of the rheometer machine is composed of a
component, attributable to the cup shape, made up of a bushing
for the connection with the stepper motor shaft, fixed by a
screw. The upper part of the cup acts as a container in which
it is located the specimen to be tested, and used for biological
materials it allows to contain their physiological solution. This
component was derivated by aluminum cylinder in the Heavy
Equipment Mechanics Laboratory of the University of Catania,
realized with the lathe and milling machine, dimensioning
the component taking in account the available space presents
between the two horizontal rails.</p>
      <p>
        A motor Phidgets 3321-0 - 28STH32 NEMA-11 Bipolar
Stepper, with integrated planetary gearbox Gearbox 27: 1 and
stepper function, characterized by a maximum speed of 120
rpm and a rated torque of 1.4 Nm has been implemented [
        <xref ref-type="bibr" rid="ref10">10</xref>
        ],
[
        <xref ref-type="bibr" rid="ref11">11</xref>
        ]. All system was designed as sine wave generator to apply
the desired shear strain to the specimen.
      </p>
      <p>Aluminum was chosen as the optimal solution to solve the
problems, such as the excessive weight of the cup that could
stress the lower stepper, and the oxidation caused by the saline
solution for in-vitro tests on biological materials. Moreover, it
has been provided the realization of a hole in the container,
threaded to be able to connect a flexible rubber tube (Fig. 2).
An another stepper motor, on upper part of rheometer,
equipped with a worm screw in order to convert its rotary
motion into linear, and thus assume the function of the linear
actuator to apply an appropriate compression to the specimen.</p>
      <p>A load cell was tied to actuator, with a capacity of 150N,
necessary for the detection of the compression force. In
addition, the appropriate metal guides have been fixed to the
upper beam, by bolts, in order to maintain in axis the load
cell during the ascent and descent of the upper plate. The
load cell is connected to a signal amplifier of Transducer
Tecniques TMO-01 able to modify the voltage output of the
load cell [mV], supplied with the correct voltage (12 VDC)
by generator.</p>
      <p>The other plate made of aluminum has the shape of a
cylindrical punch. In its upper side the bearing housing has
been obtained with mechanical interference. Using a bolt,
inside of all system, enables to make it integral with the
load cell and free rotation of upper plate in function of the
viscoelastic response. The end of the punch in contact with
the specimen has been knurled, in order to ensure a greater
adherence and avoid slippage of its during the test (Fig. 3).
By means a transducer, the phase difference is calculated
between the angular deformation and the tangential stress. In
this regard, specifically another type of load cell was made to
measure the deformations undergone by the specimen during
the test. In this case, the tested specimen can be compared to a
band pass filter, having a similar frequency response. This load
cell consists of a flexible styrene sheet (Plasticard with 1 mm
thickness), containing a strain gauge configured in Wheatstone
quarter-bridge, placed on the middle line of the foil to provide
a measure without mistakes.</p>
      <p>A lateral slot has been formed on the top plate, which allows
the insertion of the foil, and the other side is stuck to the
undercarriage by corner plates and the bolts.</p>
      <p>The two motors have the same electrical characteristics, for
this reason a single control device of Phidgets Controllers 1067
was chosen, with a sensitivity of 1/16 step, required for precise
positioning, using a switch of activation of stepper-motor.</p>
      <p>For the acquisition of the signals supplied by the load cell
and strain gauge, a PXI platform of the National Instrument
is used. It is able to offer solutions for high - performance
measurement and automation systems. But the most important
thing is the ability to perfectly synchronize the signals from
the various sensors. In this project, the system implemented is
as follows:</p>
    </sec>
    <sec id="sec-3">
      <title>Chassis NI PXIe - 1073</title>
      <p>NI PXIe - 6341 PXI Multifunction I/O Module for DAQ
NI PXIe - 6341 PXI Multifunction I/O Module for DAQ
Front-Mounting Terminal Block NI TB -4330 8Ch Bridge
Input, necessary for the acquisition of the strain gauge.</p>
      <p>The signal of the load cell is acquired by NI SCB - 68A and
subsequently processed in the control system. Furthermore,
all the above mentioned modules have a double insulation
between each channel and the ground, for safety purposes and
barrier against any noises during the testing.</p>
    </sec>
    <sec id="sec-4">
      <title>III. SOFTWARE IMPLEMENTATION</title>
      <p>The rheometer is controlled by the CS control software
developed in environment N I LabV IEW tm, to activate the
system and to analyze the results. The block diagram contained
all the codes for the machine automation and algorithms to
perform the required measures. To facilitate the debugging,
the entire block diagram is divided into several sections, each
designed to perform a specific function.</p>
      <p>The first step of the measure process consists to apply
compression of the sample until reaching the desired value,
by driving the actuator. This compression is expressed by the
percentage of the sample thickness, and already the upper plate
touches the sample, the percentage of fixed displacement is
applied.</p>
      <p>The actuator is moved with a gradual descent up until to
touch the sample, checking that the signal of the load cell is
around zero, displaying the graph on front panel. When the
top plate starts to compress the sample, a slight increase of
the signal is verified. The value represented the regulation of
the actuator movement depending on the desired compression
rate is called threshold, in this is set at - 0.016. In this way
the contact position is defined with extreme precision. The
control logic of this mechanism is controlled by the While
loop shown in Fig. 4. Within this loop a comparison between
the signal of the load cell and the above-mentioned threshold
value has been done, which is managed by the Flip - Flop SR
custom-made in LabVIEW:</p>
      <p>If the signal of the load cell is below the threshold, the
actuator will drop quickly with a continuous movement
If this threshold value is exceeded, the actuator has
touched the sample, resulting in a slowing it down,
performing a controlled displacement and applying the
percentage of compression.</p>
      <p>The particular materials, as biological cartilage, require a
certain waiting time after compression for the achievement of
the equilibrium state.</p>
      <p>
        The second step of the measure process is the heart of the
CS, imposing the oscillations to the sample, by stepper - motor
[
        <xref ref-type="bibr" rid="ref12">12</xref>
        ].
      </p>
      <p>In the last step, the acquired data are processed to extract
the necessary rheological quantities, for the characterization
of the materials, including the complex modulus G and the
loss factor tan . Finally all required data will be saved in an
Excel file.</p>
    </sec>
    <sec id="sec-5">
      <title>IV. TESTED MATERIAL</title>
      <p>The rheological tests were performed on samples of
composite polymeric material. The aim is to demonstrate that the
composite material has superior properties to those of each one
component, as the reinforcing phase has significantly better
mechanical properties, both in terms of resistance and rigidity.</p>
      <p>
        The composite materials generally are classified according
to the physical structure of the reinforcement and not for its
composition. In this activity were tested samples of composite
material in dispersed particles, constituted by the elastomer
polydimethylsiloxane (PDMS), Sylgard 184, with various
carbon black concentrations [
        <xref ref-type="bibr" rid="ref13">13</xref>
        ], [
        <xref ref-type="bibr" rid="ref14">14</xref>
        ].
      </p>
      <p>Fig. 5. Tested samples: pure PDMS and PDMS with a % of CB
Sylgard 184 belongs to the ”silicones family.” They are
seeds of thermoplastic materials - highly crosslinked
crystalline. It is characterized by a low glass transition temperature,
125 C, which gives it a good thermal stability compared to
other polymers.</p>
      <p>The fully crosslinked polydimethylsiloxane is a very
transparent and brittle material, which crumbles at low stresses and
deformations. It presents other properties, including a high
permeability, good dielectric properties, weather resistance,
lubrication properties, good biocompatibility, and visual
clarity. PDMS is the most important polixanes, and used in the
scientific and commercial areas. The mechanical strength of
the pure polydimethylsiloxane products plays a subordinate
role, for instance silicon gel for encapsulation of electronic
parts, prosthesis, absorption of vibrations.</p>
      <p>
        To obtain an improvement of the properties of the fracture,
like tensile strength, tear strength and abrasion, and also a
consequent increase in the elastic modulus, the use
reinforcing fillers is necessary, usually addeding them in the
noncrosslinked silicon at the production stage of compounding.
The main reinforcing filler is carbon black [
        <xref ref-type="bibr" rid="ref15">15</xref>
        ], [
        <xref ref-type="bibr" rid="ref16">16</xref>
        ].
      </p>
      <p>The reinforcement phase, dispersed within the matrix,
presents basic physical and geometric characteristics to
improve the mechanical and rheological properties of the final
composite. To synthesize these composites was used the
method of solution blending. This method provides initially to
identify an appropriate solvent (chloroform, acetone, toluene),
in which the polymer is treated in solution. The chosen solvent
is used to mix with the polymer, so the suspension of the
additive is dispersed in the same solvent. In the mixing phase,
the surface of the additive is coated by the polymer and, after
the removal of the solvent, is favored interconnection between
the additive and the polymer. The carbon black was added
before the beginning of the crosslinking, previously dispersed
in chloroform and then added to the silicon.</p>
      <p>The carbon black is presented as finely carbon powder, black
in color, formed by particles of almost spherical shape. The
carbon black particles generate the aggregates agglomerate in
cluster. The particles size is a fundamental property, which
does not change when carbon black is mixed in any other
polymeric material. Finer particles provide a more effective
reinforcement and a higher viscosity, resulting in an increase
in the coagulation force, with the necessity of more energy to
make possible their dispersion in a composite material.</p>
      <p>The increase of the amount of carbon black improves the
hardness and the resistance to traction of the rubber, which
becomes more rigid with a remarkable wear resistance. This
filler provides different physical characteristics, ultraviolet
absorption and electrical conductivity, used in equipment and
high-performance electronic devices. For the realization of
samples, it has been designed an aluminum mold, in order to
obtain the same thickness, diameter, regular and homogeneous
shape. This mold allows to solidify the polymer melt by
curing, even at high temperatures. In fact, the samples tested
in this activity have undergone a hardening process at a
temperature of 100 C.</p>
    </sec>
    <sec id="sec-6">
      <title>V. EXPERIMENTAL TESTS</title>
      <p>
        The creep and relaxation tests in the linear regime are
important for the determination of the viscoelastic behavior
of a material. More frequently, however, the viscoelasticity
of a fluid is measured through mechanical - dynamic tests,
commonly referred to as frequency response [
        <xref ref-type="bibr" rid="ref17">17</xref>
        ], [
        <xref ref-type="bibr" rid="ref18">18</xref>
        ], [
        <xref ref-type="bibr" rid="ref19">19</xref>
        ],
[
        <xref ref-type="bibr" rid="ref20">20</xref>
        ], [
        <xref ref-type="bibr" rid="ref21">21</xref>
        ]. In this project the strain controlled rheometer works
in SMT configuration, ie separate motor and transducer. The
tests in oscillatory regime consist in subjecting the sample,
placed between the two parallel plates, at a compression,
depending on the percentage of the thickness specimen, and
at a shear strain defining by an harmonic equation, so as to
measure the resulting stress. The equation that describe the
sinusoidal displacement by stepper-motor, is given by:
s =
s0 sin ( ! t )
(1)
      </p>
      <p>Therefore the corresponding deformation of the sample is
expressed by:
= s(t) r = s0 r sin (! t) = 0 sin (! t) (2)
h h
with r radius of sample, h its thickness, ! oscillation
frequency and 0 maximum angular strain amplitude.</p>
      <p>It is necessary that the sample has the same diameter of the
upper plate, for a better distribution of the load, to minimize
the mistakes during the measurement. The sample provides
a tangential stress obtained by a transducer, measuring the
torque transmitted to the upper plate by the sample:
M (t) = M sin ( ! t +
) )
= 0 sin ( ! t +
) (3)</p>
      <p>Phase angle represents the delay between the application
of the deformation and the stress. The shear stress is
represented by the sum elastic and viscous components:
= 0 cos sin ( ! t ) + 0 sin cos ( ! t )
(4)
dividing for the maximum deformation is obtained the
so-called complex modulus G :</p>
      <p>G = 0 = G0 sin ( ! t ) + G00 cos ( ! t ) (5)
0</p>
      <p>It is possible to define G as the measure of the total
resistance relative to the deformation of material, when it is
repeatedly subjected to a shear stress. It can be estimated as
the vector sum of the storage module G0 and the loss module
G00.</p>
      <p>G0 = 00 cos G00 = 00 sin (6)</p>
      <p>The ratio between the storage modulus and the loss
modulus measures the relation between dissipated energy and the
potential energy stored during a cycle, knowned as loss factor:
tan
=</p>
      <p>G00
G0</p>
      <p>Referring to the rheometer used in lab, the styrene sheet
with the strain gauge acts as a transducer, through which it
is possible to determine the response of the tested sample in
terms of torque, and therefore shear stress. Considering the
scheme shown in Fig. 6, in which is shown the top view of the
set constituted by the upper plate and the sheet, it is possible
to derive the appropriate mathematical relationships between
the physical quantities.</p>
      <p>By equilibrium of moments in the insertion point of the
sheet into the notch of the top plate, it is possibile to derive the
relationship between the bending moment to which is subject
the plate and transmitted torque by the sample to the upper
plate:</p>
      <p>Mf = F
Mt = F
b r
r ) Mt = Mf b
(7)
(8)</p>
      <p>Fig. 6. Top view of the set constituted by the upper plate and the sheet
b is the distance from the center of the strain gauge at the
point of application of the tangential force F, and r the radius
of the sample, which coincides with the radius of the top plate.
The bending moment is represented by the equation of the
calibration curve of sheet.</p>
      <p>It is possible to determine the shear stress :
=</p>
      <p>Mt =
Wt</p>
      <p>Mt
Ip
r =</p>
      <p>
        The rheological tests were performed on specimens
composite polymeric material specimens having different
concentration of carbon black. The samples have problems inherent
repeatability of execution tests on the same specimen, due to
the dependence of filler agglomerations by state deformation
undergone [
        <xref ref-type="bibr" rid="ref22">22</xref>
        ], [
        <xref ref-type="bibr" rid="ref23">23</xref>
        ]. It was decided to adopt a standard test
procedure, in the following way:
1) By stepper - motor, an angular deformation is fixed on
the sample, with three different amplitudes: 5 , 10 and
15 .
2) Three different percentages of compression have been
defined, in function of the sample thickness: 25%, 50%
and 75%, each of which is applied for strain amplitude
specified at point 1.
      </p>
      <p>
        The protocol of each test requires that the stepper - motor
takes 5 oscillations at the same frequency, for a number of
times equal to 10. Furthermore, after the desired compression,
a waiting time is set equal to 60 seconds, for the redistribution
of the tensions into the polymer. All samples were tested at
a constant ambient temperature (T = 24 C). The obtained
experimental data are rapresented according to the angular
deformation applied to the sample or at different frequencies
[
        <xref ref-type="bibr" rid="ref24">24</xref>
        ].
      </p>
      <p>By frequency response of the tested sample, it is possible to
extract one of the rheological variables, the complex modulus
G . In Fig. (7) is shown parameterized curves according to
the filler concentrations and the percentage of compression
applied, at a given angular deformation / frequencies, in
logarithmic scal.</p>
      <p>PDMS samples were tested and considered as reference
for comparison with other composite materials, in order to
highlight the reinforcing effect of the filler. Increasing the
percentage of carbon black CB causes a consequent increase
of G , as found in the literature.</p>
      <p>Moreover, the dynamic modulus is independent by applied
compression. By experimental data analisys, the values of
complex modulus G is acquired at a specific frequency,
(0.1 Hz and 1.95 Hz), varying the shear strain. In the short
linear viscoelastic range (LVE) at low strain G is manteined
constant; in correspondence of a certain shear strain value,
the linear viscoelastic region end and the modulus decrease
slightly. Furthermore this critical value of deformation
assumes values lower than the decreasing of the concentration of
carbon black. With the addition of carbon black, the composite
material become more rigid and viscous, with a consequent
increasing of the module G , with also the probability of
deterioration at low deformations, causing a reduction of the
LVE region.</p>
      <p>
        Some scientists have observed that for elastomers enriched
with carbon black, there was no presence of agglomerations
induced by deformation [
        <xref ref-type="bibr" rid="ref25">25</xref>
        ], [
        <xref ref-type="bibr" rid="ref26">26</xref>
        ]. However, if this
phenomenon is verified, the curve of the complex modulus G
presents a maximum point at the low deformation region,
rather than a plateau. In order to form this plateau, it is
necessary that create the filler agglomerates in the microscopic
structure of the sample. Since the reinforcing phase is
dispersed randomly, it can form a single agglomeration due to
the low filler concentrations. This phenomenon could occur in
a short average distances between the aggregates, since their
densification result in the formation of a crosslinked structure.
The heterogeneity of the material is also due to the size of the
agglomerates, which increases with the applied load.
      </p>
      <p>By amplitude strain sweep is also possible to observe
a frequency dependence, with an increase of the complex
modulus, for each concentration of filler.</p>
      <p>To analyze the variation of viscoelastic response for the
tested material is represented in terms of shear stress, plotted
vs. time and applied to different amplitudes of angular
deformation.</p>
      <p>In Fig. (9), at fixed frequency (1Hz), the increasing
amplitude of deformation is observed and also a proportional
increasing of the stress undergone by the tested specimen. The
curves are shifted, showing the viscoelastic behavior of the</p>
      <p>The aim of this paper was to verify the accuracy and
reliability of a rotational rheometer with parallel plates, made
in Heavy Equipment Mechanics Laboratory of the
University of Catania, with the implementation of hardware and
software components. To evaluate their effectiveness were
tested PDMS samples enriched with different concentrations
of carbon black.</p>
      <p>The dynamic tests were performed subjecting the samples
to a standard oscillatory regime, which allowed to obtain
the rheological characteristics of the elastomers viscoelastic
behavior. The performed study is focused on the evaluation of
the complex modulus G to varying of the working frequency
and the adopted filler percentages</p>
    </sec>
  </body>
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