Published at : 31 Oct 2017
Volume : IJtech
Vol 8, No 5 (2017)
DOI : https://doi.org/10.14716/ijtech.v8i5.874
Pramono, A.E., Rebet, I., Zulfa, A., 2017. Electrical and Mechanical Properties of Phenolic Resin and Gigantochloa Apus Carbon Fiber Composites. International Journal of Technology. Volume 8(5), pp. 920-929
Agus Edy Pramono | Department of Mechanical Engineering, Politeknik Negeri Jakarta, Depok 16424, Indonesia |
Indriyani Rebet | Department of Mechanical Engineering, Politeknik Negeri Jakarta, Depok 16424, Indonesia |
Anne Zulfa | Department of Metallurgy and Material, Faculty of Engineering, Universitas Indonesia, Kampus UI Depok, Depok 16424, Indonesia |
This work
revealed electrical and mechanical properties of phenolic resin composites made
from Gigantochloa apus carbon fiber, or bamboo carbon fiber reinforced polymer
(BCFRP) composites. Bamboo fibers were carbonized at a temperature of 800°C,
with a temperature rate of 4.2°C/minutes, held for 120 minutes. Carbon fibers
were arranged in one direction. Phenolic resin weights were determined to be 5%
to 10%. Higher carbon fiber contents indicated higher electrical conductivity
of the composite. Increased carbon fiber content tends to increase the tensile
strength of the composite, although this result was unstable. Mechanical instability was caused by cracks
and cavities formed between the fiber and the phenolic resin. Cracks primarily
occurred at the interface between bamboo carbon fibers and phenolic resin. This
was most likely caused by the intrusion of air at the time the phenolic resin
was cast. This air became trapped in between the fiber surfaces. Bamboo carbon
fiber is fragile and easily broken in both longitudinal and transverse
directions. When an air bubble bursts between carbon fibers, the carbon fiber
braid breaks up, causing electrical resistance in composites. Not all carbon
fibers in phenolic resin disconnect this way; most still form the strands that
can conduct electricity. These breaks are the cause of the instability of the
electrical conductivity properties of the composite.
Carbon fibers; Electrical conductivity; Gigantochloa apus; Phenolic resin; Tensile and impact strength
This study will suggest alternatives in
producing and utilizing carbon fiber for electrically conductive polymer
composites. This research used Gigantochloa apus, a local bamboo plant in
Indonesia. Raw material made of a continuous bamboo fiber was carbonized in a
pyrolysis process at a temperature of 800°C in a continuous vacuum furnace. The
bamboo carbon fiber was produced by the researchers in a laboratory. The bamboo
carbon fiber was not an industrial or commercial product. Most researchers
utilize industrial-made carbon materials that are commercially available. This
research used state of art methods in the utilization of local bamboo
materials. Carbonization process was conducted in the laboratory by the
researchers. Phenolic and hardener was used as the adhesive matrix. The
phenolic resin material was a commercial product. The purpose of this study is
to explore the types of carbon composites that produce electrical conductivity
and their mechanical properties.
Research on electrically conductive composites has been
conducted for decades. Electrically conductive composites are made of two kinds of materials that have opposing electrical
properties. One kind of material is
electrically conductive, and the other is electrically non-conductive.
Electrically conductive material is applied as filler and reinforcement to a
matrix of the electrically non-conductive material to form the composite. This
matrix is most commonly made of a polymer material. Electrically conductive
material can be produced by carbonizing organic materials at high
temperatures.
Nine types of carbon
material have been studied to measure electric constraints. These carbon types
were electrographite, active carbon, carbon black, acetylene-black, petroleum
coke (1400°C), petroleum coke (1600°C), Babassu nut coke, and Eucalyptus lignin
carbon. Electrical resistance was measured under constant pressure, using a
resistance measuring device and circuit potentiometric. Sample volume was
calculated from the sample thickness measured and a cross-sectional area of the
pressure chamber (Espinola et al., 1986).
Electrical conductivity
of carbon nanotubes in an epoxy matrix has been investigated because increased
electrical conductivity and homogenization has applications for aeronautics.
Laminated carbon fiber/epoxy composites are a heterogeneous material, and
electrical conductivity depends on the orientation of the carbon fiber layers
within the mix (Lonjon et al., 2012).
The electrical
conductivity of the activated carbon produced from wood has also been tested.
Activated carbon in the form of compacted powder was then measured for
electrical constraints. Conductivity measurement of powder requires compacted
granules to ensure electrical contact. The paper deals with the electrical
conductivity of a number of carbonaceous powders undergoing a low compaction.
Compaction causes electrical conductivity because of the individual grains and
connections between them, and such a combination creates a strong particle
(Celzard et al., 2002).
Silicone is a polymer
containing silicon, carbon, hydrogen, oxygen and other elements. When silicone
is used as an electrical insulator, it can be made conductive by adding
conductive material extrinsically. Two types of silicone rubber prepared with
electrically conductive carbon fiber have shown the best results. Carbon fiber
increases the electrical conductivity of the rubber, even at a very low
percentage of weight (Saleem et al., 2010).
Carbon black particles
have good electrical and thermal properties. They can be used to coat the
surface of a textile to create heat-resistant fabric. Research has been done to
develop an electrically conductive fabric. One study utilized cotton yarn
coated with an electrically conductive black carbon-based solution (Negru et
al., 2012).
Conductive adhesives are
widely used in applications such as electronic packaging and solder-free connections,
component repairs, and heat dissipation. Conductive adhesive is used to form a
connection of sufficient strength between two surfaces, with electrical
interconnection formed between the two bound surfaces. This dual function
usually requires a composite with particles in the dispersion adhesive matrix
isolation. Commonly used fillers are conductive carbon black, flake graphite,
and micro- or nano-sized metal particles such as silver, nickel, copper, or
aluminum. The special polymer matrix is made of epoxy, silicone, polyamide, or
polyurethane. Epoxy adhesive substances can be filled with electrical
conductors such as nickel powder, flakes, and filaments, silver powder, and
copper powder. The material for this research was designed to be an electrically
conductive composite (Sancaktar & Bai, 2011).
Carbon nanotubes and
chitosan were added to a solution of acetic acid at a controlled temperature of
100°C. Platinum adsorption is better for carbon nanotubes modified by chitosan,
the conductivity for carbon nanotubes that are modified larger than carbon
nanotubes without modification. In addition, platinum adsorption and carbon
nanotube conductivity increase for higher deacetylation rates (Wu, 2014).
The influence of
pressure, volume, mechanical work, and carbon density were investigated. The
decline in volume under compression depends significantly on any particular
carbon and the pressure applied to it. The increase in conductivity by
decreasing the sample volume is greater for carbon where the volume under
compression is smaller. The increase in total conductivity is greater for the
denser carbon and at least for the lightest. Both the conductivity and its
variation in compression are positively related to carbon density. Six types of
commercial carbon blacks were compacted, then measured for electrical
conductivity properties (Sánchez-González et al., 2005). Methods have been
investigated to detect damage by electrical resistance in carbon fiber polymer
matrix composites. Rectangular panels or strips with electrode plates are
generally used when measuring the conductivity of materials such as composite
panels made of continuous carbon fiber and a polymer matrix. Surface electrical
resistance and levels of conductivity through various thicknesses are obtained
(Shen et al., 2007).
One experiment used
particles of carbon black. The average size of primary carbon black particles
is about 30 nm. All specimens used in this research were ethylene butyl
acrylate (EBA) copolymers filled with acetylene carbon black (Hasnaoui, 2011).
The carbon black was provided by a manufacturer. Five specimens were prepared
using the gravity casting method. Composites with epoxy resin as a matrix and
the graphite as a filler were cast. Polymer composite material containing graphite
was studied to observe the electrical properties of composites (Szczepanik et
al., 2009).
The shell of apple
wood used in this study was initially washed with water to remove dirt and then
dried in an oven to remove the moisture. The dry shells were converted into a
fine powder using a ball milling process and followed by sieve analysis to
measure particle size. The goal was to develop a carbon black material from
agricultural waste using pyrolysis at varied carbonization temperatures and to
use it as a reinforcement in polymer composites (Ojha et al., 2015).
Due to the electrical
conductivity of carbon black and the non-conductive nature of tar and sand, the
addition of carbon black to pitch or asphalt is expected to decrease electrical
resistance, especially when the volume of the carbon black exceeds the
percolation threshold. One study aims to examine the thermal, mechanical, and
electrical effects of adding carbon black to composite pitch. Research has
shown the effects of adding the electrical properties of carbon black to
decrease electrical resistivity (Wen & Chung, 2004).
In 2011, a method was
developed for measuring the electrical resistance of a single fiber made of
carbon. The electrical resistivity or conductivity of fibers can be measured by
using a simple electrical resistance probe. Variations of two and four probes
are often used when measuring the resistivity of a sample material (Rebouillat
& Lyons, 2011). Phenolic resin and carbon fiber type 12K have been used to
make carbon composites. A study tested the mechanical properties of these
composites (Sulaiman et al., 2008).
Bamboo charcoal
powder was mixed with polypropylene (PP) and low-density polyethylene (LDPE) to
form a composite. Bamboo powder was used as a filler, and polypropylene and
low-density polyethylene were used as a matrix. The best quality bamboo
charcoal was made from bamboo branches, shoots, and roots processed in
pyrolysis at 1000ºC. The electrical resistivity of the PP/bamboo charcoal and
LDPE/bamboo charcoal composite decreases as the charcoal’s bamboo content
increases. The electrical resistivity of both types of polyolefin
charcoal/bamboo composites seems to be substantially reduced (Kittinaovarat
& Suthamnoi, 2009).
2.1. Materials
The study used Gigantochloa apus bamboo that was manually made into
fibers with a diameter of ? 0.5 mm. Bamboo fibers were carbonized in a
continuous vacuum furnace at a temperature of 800°C, at a speed of
4.2°C/minute, held for 120 minutes.
The carbonization
process was carried out through pyrolysis without using inert gas. The
pyrolysis process required only an airtight tube without oxygen to produce
electrically conductive carbon.
Carbonization at a
temperature of 800°C eliminated non-carbon elements and created pores in the
carbon fiber (Ojha et al., 2015). Phenolic resins were prepared by fabricators
and commercially purchased, without prior customization. The densities of
bamboo carbon fibers are 1.3±0.12 gram/cm3.
2.2. Samples Preparation
Carbon fibers were arranged in one direction, with weights determined to
be 5% to 10% of the phenolic resin. The phenolic resin is poured into a mold
measuring 10×10×120 mm, with bamboo carbon fiber as a reinforcement. This
process was conducted manually. The test specimen data are shown in Table 1,
and the fabricated composite of carbon fibers and phenolic resin is shown in
Figure 1.
Table
1 Test specimen
Test |
Carbon fiber content, % |
|||||
5 |
6 |
7 |
8 |
9 |
10 |
|
Electric conductivity |
5 |
5 |
5 |
5 |
5 |
5 |
Tensile strength |
5 |
5 |
5 |
5 |
5 |
5 |
Impact strength |
5 |
5 |
5 |
5 |
5 |
5 |
Figure 1 Test specimens
2.3. Electrical
Conductivity Test
Electrical conductivity was measured with a
two-point probe method (Celzard et al., 2002), following the American Society
for Testing Materials (ASTM) standard D 578), by measuring the composite’s
electrical resistance. Static electric resistance was calculated with the
following equation (Espinola et al., 1986; Sancaktar & Bai, 2011; Saleem et
al., 2010; Rebouillat & Lyons, 2011; Shen et al., 2007):
(1)
Figure
2 Two-point probe method
where ? is the static resistance in ?.m, R is the electrical resistivity in ?, A is the cross-sectional area in m2,
and l is the distance of resistivity
in m. Electrical conductivity is determined by the formula (Sánchez-González et
al., 2005; Espinola et al., 1986):
or in (2)
2.4. Tensile Strength
Test
Tensile strength was tested with a tensile
testing machine. The tensile strength of carbon fiber/phenolic resin composites
was determined by the formula:
(3)
where F is the
tensile test load in N, and A is the cross-sectional area of the test specimen
in mm2.
2.5. Impact Strength
Testing
Impact strength testing followed the ISO
standard 179/1U. The value of the impact strength was calculated by the
following equation:
(4)
where acU
is Charpy un-notched impact strength (kJ.m-2), Ec is the
energy correction (joule) absorbed by the fracture of the test specimen, h is
the thickness (mm) of the test specimen, and b is the width (mm) of the test
specimen.
2.6. Morphology
Test
The morphology of carbon
fiber composites was examined with the scanning electron microscope (SEM) JEOL
JSM-6390A.
3.1. Morphology of Composites
Composite morphology testing was performed to observe the
shape of a cross section of bamboo fiber, bamboo carbon fiber, carbon fiber
interfaced with the phenolic matrix, and cracks in the composite. Composite
morphology was observed with the SEM JEOL JSM-6390A test machine. Test
parameters were as follows: Acquisition Parameter, Instrument: 6390 (LA); Acc.
Voltage: 20.0 kV; Probe Current: 1.00000 nA; PHA mode: T4. Composite specimens
with 10% carbon fiber content were used as a composite morphology specimen
because the sample has the highest electrical conductivity. Morphological test
results are shown in Figure 3.
Morphology pictures with 700× magnification show
cross-sectional shapes of bamboo carbon fiber bonded to the phenolic resin.
Carbon fiber bamboo shows visible parenchymal tissue of the bamboo carbon in an
irregular hexagon shape. Meanwhile, phenolic resin is flat, without any holes
or cavities, as shown in Figure 3a. The cross section of bamboo carbon fiber
magnified 2000× clearly shows holes in parenchymal tissue of bamboo carbon
fiber, as shown in Figure 3b. The cracks in the interface between bamboo carbon
fibers and phenolic resin is shown in Figure 3c in 200× magnification. The
cross section shows the honeycomb-like parenchymal tissue of bamboo carbon
fiber, while other parts show phenolic resin as a matrix. Figure 3d shows the
fibers before carbonization, highlighting a cross section of real vascular
bundles with Gigantochloa apus fibers at a magnification of 1500×. The bamboo
fiber cross section shows the irregular hexagon shape. This can be compared
with the already carbonized bamboo fibers.
(a)
(b)
(c) (d)
Figure
3 Morphology: (a) Morphology of composite; (b) Morphology of bamboo carbon
fiber; (c) Cracks in the composite; (d) Bamboo fiber cross section before
carbonizing
Occasionally
air is trapped in the resin at the time of casting, leading to cracks and
cavities in the composite. Reaction between the phenolic resin and hardener
catalyst produce heat, causing the trapped air to increase in pressure, and
break in between the fibers. This results in cracks in the interface between
the carbon fiber and phenolic resin. The crack weakens the mechanical
properties of such composites. The cracks also cause breaking of the carbon
fiber braid in the composite, causing weak electrical conductivity. Test
results show this instability of electrical conductivity in the composite. When
the air bubble bursts between carbon fibers, the carbon fiber braid will break
up, and cause electrical resistance in the composite. Not all carbon fiber in
phenolic resin disconnects; most still forms the strands that can become
electrically conductive. This inconsistency is the cause of the electrical
conductive instability in the composite.
3.2. Electrical Conductivity
Electrical conductive
testing data were obtained by measuring electrical resistance, sample length,
and cross-sectional areas. The measurement technique is shown in Figure 2.
There were five specimens measured with each carbon content variation. The electrical
conductivity was determined by Equation 2. Electrical
conductivity data were connected with the percentage of carbon content in the
composite to determine the best electrical conductivity based on carbon fiber
content. Figure 4 shows that the higher the percentage of carbon fiber content,
the higher the electrical conductivity of a carbon fiber/phenolic resin
composite. The highest electrical conductivity is generated by composites
containing 10% carbon fiber weight. The highest electrical conductivity is
generated by composites containing 10% carbon fiber weight. In this composite
also yields the highest tensile strength. As shown in Figure 5.
The results of the 2009 study suggested
that adding of the volume of graphite to the epoxy resin causes a decrease in
electrical surface resistivity (Szczepanik et al., 2009). A carbon fiber
content of 5% showed an electric conductivity of 5.2 S.m-1, while at
a carbon fiber content of 10%, the electrical conductivity reached 51.12 S.m-1.
A study stated that carbon black particles have good electrical properties
(Negru et al., 2012). Electricity can only pass through a material if there is
a sufficient conducting network of fillers that are electrically conductive
(Saleem et al., 2010).
Figure 4 The relationship of electrical conductivity vs carbon fiber content
Deviations are likely to be caused by
nonhomogeneous interconnections of carbon fiber, resulting in voids between
fibers. Phenolic resin as a matrix in these composites is not electrically
conductive (Szczepanik et al., 2009), so when it fills the gaps dissolution of
carbon fiber will increase the flow resistance. Research shows that electrical
conductivity depends on the number of effective electrical contacts formed
between carbon particles (Sánchez-González et al., 2005). Irregularities cause
unstable flow of electricity in the composite as a whole due to cracks or
cavities. This can be seen through the results of the morphology test.
3.3. Tensile strength
The composite tensile strength test was
conducted by a universal testing machine., universal testing machine (UTM),
Tarno testing, TARNOGROCKI, GA 0.3V/483, following ASTM D 3039-76 (Ojha et al.,
2015). Five specimens were tested to
show each variation of carbon fiber content. This test provided load test data.
The tensile strength of the test sample was determined by Equation 3. The
composite tensile strength was related to the percentage of carbon fiber
content in the composite, to determine the highest tensile strength based on
carbon fiber content, as shown in Figure 5.
The increase in carbon fiber content tends to increase the tensile
strength of these composites, but this effect is not stable. A carbon fiber
content of 5% has a tensile strength of 9 N/mm2, but when the carbon
fiber content increased from 6% to 9%, composite tensile strength decreased.
When fiber content increased again to 10%, the tensile strength increased to 12
N/mm2, as shown in Figure 5. Tensile strength instability was caused
by cavities formed in the phenolic resin matrix, and at the interface between
the fiber and the resin matrix. In the curing process, some physical and
chemical changes occur when the material changes from viscous to hard solid
(Sulaiman et al., 2008).
Figure 5 The relationship of tensile strength vs carbon fiber content
The distribution and
orientation of carbon fibers and the matrix affects the tensile strength
properties of composites. One cause of weakness in the mechanical properties of
composites were most likely the chemical reactions at the interface between
carbon fiber. These made the matrix too weak to move the tensile load (Ojha et
al., 2015). This condition can be proven through testing composite morphology
with SEM testing.
3.4. Impact Strength
Five specimens were used in the impact strength test specimen with each
variation of carbon fiber content represented. The impact strength test
followed ISO 179/1U standards. Specimens underwent Charpy impact testing,
un-notched, conditioned at a temperature of 23.3°C with 42.0% humidity for 48
hours. The test used a 2J pendulum impact tester with an impact speed of 2.9
m/s. The test was conducted using the CEAST Resil impact machine. The impact
strength value of the composite was determined by Equation 4. Impact strength
was compared to the percentage of carbon fiber in the composite to determine
the highest impact strength of the composites based on the percentage of carbon
fiber. This is shown in Figure 6.
Figure 6 The relationship of impact strength vs carbon fiber content
Impact strength of composites were unstable. Composites with a 7% weight
content of carbon fibers showed strength of 1.76 kJ.m-2. Meanwhile,
carbon fiber composites containing 5% weight showed 1.15 kJ.m-2.
When the carbon fiber content increased to 10% by weight, impact strength
decreased to 1.02 kJ.m-2. This shows the impact strength of bamboo
carbon fiber and phenolic resin composites in this study is not stable. This is
affected by cavities formed in the phenolic resin composites when casting into
molds.
Research
has been conducted on the electrical conductivity and mechanical properties of
bamboo carbon fiber/phenolic resin composites or bamboo carbon fiber reinforced
polymer (BCFRP) composites. The higher the percentage of carbon fiber in a
composite, the higher the electrical conductivity of the composite. Increased
carbon fiber in a composite tends to increase the tensile strength of these
composites. This study found instabilities in the impact strength of bamboo
carbon fiber and phenolic resin composites.
For
application with a combination of high electrical conductivity and tensile
strength, a composite of 10% carbon fiber content may be used. However, this
type of composite is not resistant to impact loads.
The
cracks are also the cause of breaking carbon fiber braids in the composite,
resulting in weak electric current conductivity. Some fibers remain intact, but
the frequent breakage leads to electrical instability. Local natural fiber is
widely available, in the future can also be developed carbonization of organic
natural fibers from sisal, coconut fiber, and organic waste, as electrically
conductive fillers.
The authors wish to
thank the Directorate of Research and Community Service, the Directorate
General of Higher Education, and the Ministry of Engineering Research and
Higher Education of the Republic of Indonesia for funding this work. This
research was funded through a national research strategy with the contract
number: 089/SP2H/PL/Dit.Litabmas/II/2015.
Celzard, A., Marêché,
J.F., Payot, F., Furdin, G., 2002. Electrical Conductivity of Carbonaceous Powders.
Carbon, Volume 40(15), pp. 2801–2815
Espinola, A., Miguel,
P.M., Salles, M.R., Pinto, A.R., 1986. Electrical Properties of Carbons-resistance
of Powder Materials. Carbon, Volume 68,
pp. 276–281
Hasnaoui, M.El.,
2011. Electric Modulus Analysis of Carbon Black/Copolymer Composite Materials. Materials Sciences and Applications, Volume
2(10), pp. 1421–1426
Kittinaovarat, S.,
Suthamnoi, W., 2009. Physical Properties of Polyolefin/Bamboo Charcoal
Composites. Journal of Metals, Materials
and Minerals, Volume 19(1), pp. 9–15
Lonjon, A., Demont, P.,
Dantras, E., Lacabanne, C., 2012. Electrical Conductivity Improvement of Aeronautical
Carbon Fiber Reinforced Polyepoxy Composites by Insertion of Carbon Nanotubes. Journal of Non-Crystalline Solids, Volume
358(15), pp. 1859–1862
Negru, D., Buda, C.T.,
Avram, D., 2012. Electrical Conductivity of Woven Fabrics Coated with Carbon
Black Particles. FIBRES & TEXTILES in
Eastern Europe, Volume 1(90), pp. 53–56
Ojha, S., Acharya, S.K.,
Raghavendra, G., 2015. Mechanical Properties of Natural Carbon Black Reinforced
Polymer Composites. Journal of Applied
Polymer Science, Volume 132(1), pp. 1–7
Rebouillat, S.,
Lyons, M.E.G., 2011. Measuring the Electrical Conductivity of Single Fibres. International Journal of Electrochemical
Science, Volume 6(11), pp. 5731–5740
Saleem, A., Frormann,
L., Soever, A., 2010. Fabrication of Extrinsically Conductive Silicone Rubbers
with High Elasticity and Analysis of their Mechanical and Electrical Characteristics.
Polymers, Volume 2(3), pp. 200–210
Sancaktar, E., Bai, L.,
2011. Electrically Conductive Epoxy Adhesives. Polymers, Volume 3(1), pp. 427–466
Sánchez-González, J.,
Macias-Garc?a, A., Alexandre-Franco, M.F., Gomez-Serrano, V., 2005. Electrical Conductivity
of Carbon Blacks under Compression. Carbon,
Volume 43(4), pp. 741–747
Shen, L., Li, J., Liaw,
B.M., Delale, F., Chung, J.H., 2007. Modeling and Analysis of the Electrical Resistance
Measurement of Carbon Fiber Polymer-matrix Composites. Composites Science and Technology, Volume 67(11–12), pp. 2513–2520
Sulaiman, S., Yunus, R.,
Ibrahim, N.A., Rezaei, F., 2008. Effect of Hardener on Mechanical Properties of
Carbon Fibre Reinforced Phenolic Resin Composites. Journal of Engineering Science and Technology, Volume 3(1), pp.
79–86
Szczepanik, M.,
Stabik, J., Lazarczyk, M., Dybowska, A., 2009. Influence of Graphite on
Electrical Properties of Polymeric Composites. Archives of Materials Science and Engineering, Volume 37(1), pp.
37–44
Wen, S., Chung, D.D.L.,
2004. Effects of Carbon Black on the Thermal, Mechanical and Electrical Properties
of Pitch-matrix Composites. Carbon, Volume
42(12–13), pp. 2393–2397
Wu, H., 2014.
Adsorption and Electrical Conductive Properties of Carbon Nanotube Modified by
Chitosan. Journal of Materials Science
and Engineering A, Volume 4(3), pp. 83–90