Characterization of nanocomposite filaments
developed for additive manufacturing
Cite as: AIP Conference Proceedings 1779, 100006 (2016); https://doi.org/10.1063/1.4965574
Published Online: 31 October 2016
Fugen Daver, Robert A. Shanks, and Milan Brandt
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AIP Conference Proceedings 1779, 100006 (2016); https://doi.org/10.1063/1.4965574
© 2016 Author(s).
1779, 100006
Characterization of Nanocomposite Filaments Developed for
Additive Manufacturing
Fugen Daver1, a), Robert A. Shanks2, Milan Brandt1
1
Centre for Additive Manufacturing
School of Aerospace, Mechanical, and Manufacturing Engineering, RMIT University, PO Box 71, 3083 Victoria,
Australia
2
School of Applied Sciences, RMIT University, GPO Box 2476, 3001, Victoria, Australia
a)
Corresponding author: fugen.daver@rmit.edu.au
Abstract. The study aims to characterize innovative filaments in the form of polyolefin-rubber nanocomposites
developed for additive manufacturing. Polyolefin-rubber filaments were consisted of linear low density polyethylene and
de-vulcanised, activated rubber. A compatibilizer in the form of maleic anhydride grafted polyethylene was used to
enhance adhesion between the two phases. Multi-walled carbon nanotubes were introduced for electrical conductivity.
Various compositions of filament material were tested for mechanical properties, electrical conductivity and timedependent deformation behavior as demonstrated in creep-recovery experiments. A four element model of Maxwell and
Voigt-Kelvin was employed to analyze the creep behavior of the nanocomposites. Results were discussed in terms of the
effect of (i) carbon nanotubes, (ii) compatibilizers and (iii) composition of each nanocomposites.
INTRODUCTION
Additive manufacturing aims to produce parts directly from Computer Aided Design (CAD) model of the part
without the need for building costly molds. Fused Deposition Molding (FDM) is one of the additive manufacturing
techniques which allows production of free-form manufacturing of prototypes and end-use parts. In FDM, plastic
filament of certain cross sectional area passes through an extruder and molten plastics is deposited on to a working
platform layer by layer by means of an extruder head travelling across the platform according to the CAD model of
the part. The platform is lowered as each layer is formed, subsequent layers bond via thermal fusion to form the
complete part. Flexibility and convenience offered by FDM techniques has opened the doors for automotive,
aerospace and biomedical applications. However, the number and type of materials available in filament form for
FDM applications are currently rather limited. In this study, we have explored polyolefin-rubber nanocomposites as
filament material in FDM applications and evaluated their time dependent deformation behavior and assessed their
electrical conductivity.
EXPERIMENTAL
Materials
Linear low-density polyethylene (LLDPE) was mixed with maleic anhydride grafted polyethylene (MA-g-PE)
which is grafted with maleic anhydride 0.90 %·w/w. Functionalized rubber particles (FRP), which were produced
according to a patented process, were obtained from Polymeric Powders Company [1,2,3]. Multi-walled carbon
nanotubes (MWCNT) were incorporated into the polyolefin–rubber composites in the form of a masterbatch
Plasticyl LDPE2001 which is based on low density polyethylene (LDPE) [4].
Proceedings of the Regional Conference Graz 2015 – Polymer Processing Society PPS
AIP Conf. Proc. 1779, 100006-1–100006-5; doi: 10.1063/1.4965574
Published by AIP Publishing. 978-0-7354-1441-9/$30.00
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Sample preparation
LLDPE was fed into the pre-heated non-intermeshing, counter rotating internal batch mixer at 180 °C and it was
mixed at 50 rpm for 1 min to ensure complete melting of polymer prior to the introduction of the masterbatch
Plasticyl LDPE2001, FRP and MA-g-PE, which aims to improve compatibility between the rubber and the
polyethylene. All four ingredients were mixed for another 5 min at 180 °C before the mixture was removed for
further processing. Table 1 shows the compositions of the LLDPE–FRP nanocomposites. All materials were
compression molded for characterisation purposes. Whereas, the composites PB4 and C-PB4 were formed into
filaments with an average diameter of 1.73 mm by means of a twin screw extruder which was equipped with a series
of rollers to take-up and wind the filament to be used in the fused deposition modelling process. Details of the
sample preparation are given elsewhere [5].
TABLE 1. Composition of the LLDPE–FRP nanocomposites.
Sample Code
Composition (%·w/w)
FRP
MA-g-PE
30
-
PB1
LLDPE
70
MWNT
-
PB3
30
70
-
-
PB4
65
30
5
-
PB5
25
70
5
-
C-PB4
62
30
5
3
C-PB5
22
70
5
3
Fused deposition modeling (3D printing) of nanocomposite filaments
Fused deposition modelling which is an additive manufacturing process was performed by means of Makerbot
Replicator 2. Filament of polyolefin rubber nanocomposite was heated up to 260 oC and extruded through a nozzle
that moves in the x-y plane. When the extruded material deposited, it solidified and generated a single layer. The
fusion of subsequent layers resulted in the actual test specimens formed based on the 3D CAD model of (i) Type 1
standard specimen according to Tensile Testing of Polymers (ASTM D638) and (ii) Rectangular specimens of
3.2x12.7x125 mm dimension according to Flexural Modulus Testing of Polymers (ASTM D790).
Characterization of polyolefin rubber nanocomposites
Tensile testing was performed using an Instron Series 4467 Universal Test Instrument equipped with a 2 kN load
cell and with Instron Bluehill Software (Instron Co., Canton MA, USA D638). The strain was measured with an
Instron Long Travel Extensometer. The 3D printed specimens were compared with the compression moulded
specimens. Compression molding was performed at 180 °C for 5 min under a force of 50 kN followed by watercooling of the mould to below 50 °C prior to pressure release and ejection from the mould. Data were collected by
averaging over five measurements.
Conductivity of the composites was measured by High Resistance Meter, Model HR2 (AlphaLab Inc., Utah,
USA). The specimens of 10 mm length were then inserted into the test fixture where the spring-loaded plunger
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applied a consistent pressure to each specimen. Five specimens were tested for each composition and the results
were averaged.
A TA Instruments Q800 Dynamic Mechanical Analyser in tensile mode was used for creep - recovery (static
force thermomechanometry, sf-TM). Sf-TM analysis was performed by subjecting the tests samples to an applied
stress of 1.2 MPa for 30 minutes followed by a recovery period of 120 minutes. The applied stress was chosen
within the linear viscoelastic region of the all samples. Tests were conducted at 25 oC. The four element model of
Maxwell and Kelvin-Voigt was used to interpret the creep component [6]. The springs correspond to elastic section
with moduli E1 and E, while the dashpots represent the viscosity K and K2. The overall deformation of the model
is given in Equation (1).
=
+
1
+
(
)
(1)
RESULTS AND DISCUSSION
The mechanical properties of all LLDPE–FRP composites showed significant decrease, except for elongation at
break when manufactured by fused deposition moulding (3D printing) compared with the compression moulded
composites. Porosity between the neighbouring extruded filaments is most likely to be the reason behind the
observed decrease in mechanical properties of the composites prepared by fused depositon modelling [5]. The
introduction of carbon nanotubes did not improve the mechanical properties of the compression moulded or the 3D
printed composites. This is most likely due to incorporation of MWCNT into the composites via a low viscosity
thermoplastic concentrate (Plasticyl LDPE2001) [5].
The electrical properties of the composites containing MWNT, both high rubber content, C-PB4, and low rubber
content, C-PB5, were tested for conductivity. All composites used for electrical testing were prepared by
compression molding. Composites with high rubber content (C-PB5) demonstrated much higher conductivity
compared with the low rubber content composites (PB4) [5]. As the rubber content increased, conductive channels
became more effective, due to the increased concentration of carbon nanotubes within the narrowing network of
LLDPE. This approach, based on selective localization of MWNT in only one of the phases, offers an innovative
method of increasing/adjusting the conductivity by employing polymeric composites with selective conductor
location or composites with varying amounts of each phase [7]. There was not a significant difference between the
conductivities of compression molded and 3D printed samples as discussed in our recent publication [5].
The creep and recovery curves of polyolefin-rubber composite (PB1) are presented in Figure 1 (a). The creep
stress varied between 1.2 MPa and 6 MPa. The total strain just before the release of the stress was measured and it
is plotted against the initial loading stress as shown in Figure 1 (b). The linear relationship between stress and strain
enabled to establish the maximum creep stress as 3 MPa, so that the material is tested within its linear viscoelastic
region during the following creep experiments. In all creep curves, an instantaneous increase in strain is occurs due
to elastic response of the material. This is followed by a viscoelastic response, which involves time-dependent
molecular rearrangement. Viscous flow is observed towards the end of the load application period. Removal of the
load results in rapid drop in strain response, which is equal to the initial elastic response. The recovery period
involves time-dependent molecular relaxation as the polymer attempts to regain original dimensions. Since the
polymer experienced viscous flow, the full recovery is not reached resulting in permanent deformation [8,9].
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(a)
(b)
FIGURE 1. Creep-recovery behavior of PB1 (a) at different initial stresses; (b) max strain vs initial stress
The creep and recovery curves for the composites PB1, PB3, PB4 and PB5 are shown in Figure 2 (a). The
addition of (MA-g-PE) proved to enhance the bonding between the phases and the creep deformation under the same
load was less in blends with (MA-g-PE).
The creep and recovery curves for the composites PB4, PB5, C-PB4 and C-PB5 are shown in Figure 2 (b).
Incorporation of MWCNT into the composites do not seem to introduce a positive effect on the creep behaviour.
This is most likely due to the fact that the carbon nanotubes were introduced via low viscosity masterbatch,
Plasticyl LDPE2001.
(a)
FIGURE 2. The effect of (a) (MA-g-PE) (b) MWCNT on creep-recovery behavior
(b)
To enable to understand the long term deformation behavior of the nanocomposites under long periods of time at
ambient temperatures, a series of creep experiments were conducted at different temperatures between 30 oC and
80 oC for the PB4 and PB5. Time temperature superposition principle was applied to estimate creep performance of
the filament material at longer durations.
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ACKNOWLEDGMENTS
The authors acknowledge the funding provided by the Victorian Government - Department of State
Development Business and Innovation under the Technology Development Voucher Program. Special thanks go to
M. Allan, Rheology and Processing Centre, RMIT University for his technical assistance in experimental work. The
opportunity to undertake the project was provided by Polymeric Powders Company Pty Ltd who stipulated the
polyolefin and rubber materials to be utilized, as well as provided direction on the incorporation of carbon nanotubes
for electrical conductivity.
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