Yiyao Ren1, Lei Xu1,2,3, Xiaobiao Shang3, Zhigang Shen4, Rongzheng Fu4, Wei Li3, Lirong Guo1. 1. Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology, Kunming 650093, People's Republic of China. 2. State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science and Technology, Kunming 650093, People's Republic of China. 3. Key Laboratory of Unconventional Metallurgy, Ministry of Education, Kunming University of Science and Technology, Kunming 650093, People's Republic of China. 4. Sinopec Shanghai Research Institute of Petrochemical Technology, Shanghai 201208, People's Republic of China.
Abstract
Disposal of the waste from carbon fiber reinforced polymers (CFRPs) has become an urgent problem due to the increasing application of CFRPs in many industries. A novel method for the rapid recovery of carbon fibers by a microwave pyrolysis and oxidation process was proposed in this study. The resin matrix was rapidly pyrolyzed by heating CFRPs directly with microwave radiation, and then the residual carbon and organic matter on the surface of carbon fibers were removed by oxidation to obtain recycled carbon fibers (RCFs). The recovery rate of recycled carbon fibers was measured, and their mechanical properties were evaluated by tensile strength and tensile modulus tests. The results showed that, after microwave pyrolysis at 500 °C for 15 min and oxidation at 550 °C for 30 min, the maximum tensile strength of RCFs was 3042.90 MPa (about 99.42% of that of virgin carbon fibers), the tensile modulus was 239.39 GPa, and the recovery rate was about 96.5%. The microstructure and chemical composition of RCFs were characterized by scanning electron microscopy, X-ray diffraction, Raman spectroscopy, Fourier transform infrared spectroscopy, and X-ray photoelectron spectroscopy, and the components of the pyrolysis byproducts were detected by gas chromatography-mass spectrometry. These results indicate that this method is suitable for the effective recovery of high-quality carbon fibers from CFRPs.
Disposal of the waste from carbon fiber reinforced polymers (CFRPs) has become an urgent problem due to the increasing application of CFRPs in many industries. A novel method for the rapid recovery of carbon fibers by a microwave pyrolysis and oxidation process was proposed in this study. The resin matrix was rapidly pyrolyzed by heating CFRPs directly with microwave radiation, and then the residual carbon and organic matter on the surface of carbon fibers were removed by oxidation to obtain recycled carbon fibers (RCFs). The recovery rate of recycled carbon fibers was measured, and their mechanical properties were evaluated by tensile strength and tensile modulus tests. The results showed that, after microwave pyrolysis at 500 °C for 15 min and oxidation at 550 °C for 30 min, the maximum tensile strength of RCFs was 3042.90 MPa (about 99.42% of that of virgin carbon fibers), the tensile modulus was 239.39 GPa, and the recovery rate was about 96.5%. The microstructure and chemical composition of RCFs were characterized by scanning electron microscopy, X-ray diffraction, Raman spectroscopy, Fourier transform infrared spectroscopy, and X-ray photoelectron spectroscopy, and the components of the pyrolysis byproducts were detected by gas chromatography-mass spectrometry. These results indicate that this method is suitable for the effective recovery of high-quality carbon fibers from CFRPs.
Carbon fiber reinforced
polymers (CFRPs) have higher specific strength
than metal materials, as well as excellent properties such as high
temperature resistance, corrosion resistance, and impact resistance.[1,2] These characteristics make CFRPs powerful substitutes for traditional
metal materials in the automobile, vessel, aviation, and aerospace
fields.[3−5] The annual consumption of carbon fibers (CFs) is
about 100000 tons, 15.4% of which is used in the aerospace field and
11.7% in the automobile industry, and the annual market of CFs is
growing by more than 11%.[6] In recent years,
the biggest challenge facing the automobile and aircraft industry
has been to find ways to save fuel and reduce weight to reduce carbon
dioxide emissions. CFRPs have been widely used in the automobile industry
as an effective means to realize lightweight vehicles.[7] By 2022, the demand for CFs is expected to reach 117000
tons.[2,7] The increasing demand of CFs will result
in more and more CFRP waste, making the disposal of CFRPs an urgent
problem.At present, most CFRP wastes are disposed of by landfill.[8] Epoxy resin is widely used in CFRPs because of
its low viscosity, good compatibility with the fiber surface, heat
resistance, and excellent mechanical properties. However, after being
disposed of as industrial waste in landfills, CFRPs have caused tremendous
resource waste and serious environmental problems such as landscape
destruction, soil pollution, and water pollution.[9−11] After CFRPs
are disposed of in a landfill, the partial degradation of the resin
will produce toxic substances remaining on the land, causing soil
pollution. In addition, toxic substances will cause water pollution
when they are transferred into the water.[2,6] Consequently,
most developed countries have started to legally prohibit the landfill
disposal of CFRPs. In addition, the use of CFRPs as vehicle materials
has greatly increased the necessity of developing a recycling technology.[12] Therefore, it is imperative to recycle CFs.Generally, the main recycling methods of CFs include mechanical,[13−15] chemical,[16−19] and thermal methods.[20−22] In the mechanical method, CFRP waste is crushed into
particles or milled into powder, which can be directly used as a filler.
Only short CFs can be obtained by the mechanical method, and their
mechanical properties are severely damaged after grinding and shearing.[12] In the chemical method, the cross-linked bonds
in the resin are broken by solvent and heat and the resin is decomposed
into low-molecular-weight polymers or small organic molecules and
dissolved in the solvent, thereby separating CFs from the resin matrix.
CFs recycled by chemical method can retain a tensile strength of 80%
and up to 99% under extreme conditions. However, this is not an appropriate
recovery method because it involves high cost and produces harmful
gases,[21] such as nitrogen oxides, sulfides,
and volatile organic solvents. In the pyrolysis method, the resin
in the composite is decomposed into small organic molecules at high
temperature to recover CFs. At present, pyrolysis is used in most
commercial-scale CF recycling operations in the world.[2] When CFs are recycled by pyrolysis, the tensile strength
of the recycled carbon fibers (RCFs) can be maintained at 50–85%,[7] and long CFs can be obtained. More importantly,
recycling CFs by pyrolysis can save energy and reduce the environmental
impact. The production of virgin carbon fibers (VCFs) requires 198–595
MJ/kg of energy consumption and emits 30–80 kg of CO2,[23−25] while RCFs consume only 30 MJ/kg and emit less CO2.[24]Microwave radiation has been used as a
heat source in the pyrolysis
of composites.[6] Microwave heating has the
characteristics of internal, rapid, and selective heating, which has
broad development potential in the preparation, sintering, and recycling
of materials.[26] The materials recovered
by microwave technology mainly include metals,[27] lithium-ion batteries,[28] CFRPs,
spent carbon cathodes,[29] sewage,[30] and circuit boards.[31] Lester[32] of the University of Nottingham
and others studied the feasibility of recycling the CF/epoxy resin
composite material recovery by microwave pyrolysis and proved that
microwave heating could effectively recycle CFs.Microwave-assisted
pyrolysis was used for recycling CFs in this
study, which was different from the traditional pyrolysis method. Scheme shows the cyclic
utilization route of CFs. First, CFs are recycled from CFRP waste
by microwave pyrolysis. Then the obtained RCFs are converted into
thermoplastic or thermosetting composites to realize the cyclic utilization
of CFs in the automobile, sports, construction, aerospace, and electric
power fields. In this study, the technical advantages of microwave
heating were combined with the technical characteristics of recycling
CFs from CFRP by the pyrolysis method. The epoxy resin in CFRPs was
decomposed by direct microwave heating, and then the pyrolyzed carbon
and residual organic matter on the CF surface were removed by oxidation.
The surface morphology, recovery rate, mechanical properties, chemical
structure of RCFs and the components of the pyrolysis byproducts were
characterized to investigate the effects of different reaction conditions
on the recycling of CFs.
Scheme 1
Cyclic Utilization Route of Carbon Fibers
Experimental Section
Materials
CFRP sheets with a size
of 100 × 20 × 1 mm were provided by Gongyi Fanruiyihui Composites
Co., Ltd., Henan Province, China. The VCFs were produced by Formosa
Plastics Group in Taiwan. CFRP was prepared with epoxy resin (E51)
as s matrix, carbon fiber cloth (TC33-3K) as s reinforcement, methyl
tetrahydrophthalic anhydride (MethPA) as s curing agent, and tris(dimethylaminomethyl)phenol
(DMP-30) as an accelerator. The carbon fiber cloth was plain woven,
and the above/below pattern of the wire rope was woven to provide
a highly stable and compact structure. Each CFRP sheet contains six
layers of carbon fiber cloth. CFs in CFRP have a mass fraction of
about 76 wt % and a volume fraction of about 68 vol %.
Experimental Procedure
The pyrolysis
and oxidation of CFRPs were studied in a microwave tube furnace and
a traditional tube furnace respectively. The schematic diagram of
the experimental device is shown in Figure . The microwave frequency was 2.45 ±
0.05 GHz, and the microwave power was 0–1000 W. The microwave
tube furnace was connected to an argon gas cylinder, a pyrolysis oil
collection bottle, a condenser tube, a drying tube, and an exhaust
pipe. Before the reaction, argon gas was first introduced into the
furnace, and then the air was exhausted for several minutes. This
process was repeated three times to ensure the complete removal of
air. After the argon gas was stably introduced into the microwave
tube furnace with a flow rate of 50 mL/min, microwave radiation was
applied, and the CFs in CFRPs were directly heated by microwave radiation,
so that the resin could be pyrolyzed quickly. Part of the pyrolysis
gas was condensed to form an oil, and the noncondensable part and
argon gas were collected after drying. After the pyrolysis experiment,
the solids were cooled to room temperature, and the residual solids
were taken out and put into a traditional tube furnace. After introduction
air, the pyrolytic carbon and residual organic matter on the CF surface
were oxidized for a period of time, and finally the RCFs were obtained.
The experimental scheme and sample code are presented in Table .
Figure 1
Schematic diagram of
microwave pyrolysis.
Table 1
Experimental
Scheme and Sample Code
microwave
pyrolysis
thermal oxidation
experiment (sample
code)
temp (°C)
time (min)
experiment
(sample code)
temp (°C)
time (min)
P400T15
400
15
D500T40
500
40
D500T50
500
50
P500T15
500
15
D550T30
550
30
D550T40
550
40
Schematic diagram of
microwave pyrolysis.
Characterization Methods
Thermogravimetric
analysis (TGA) data of CFRP pyrolysis were collected with a DSC/DTA-TG
analyzer (STA 449 F3 Jupiter, Netzsch, Germany). The CFRP (10 mg)
sample was heated from 30 to 1000 °C at an increment of 15 °C/min
under an argon atmosphere with a flow rate of 20 mL/min. The residual
solids (10 mg) were heated from 30 to 1000 °C in an air atmosphere
with a flow rate of 20 mL/min at an increment of 15 °C/min. The
surface morphology of RCFs was observed by a scanning electron microscope
(SEM, VEGA3 SBH, TESCAN, Czech). The mechanical properties of RCFs
were tested by an automatic single-fiber universal tester (Robot 2,
Textechno, Germany). The structure of RCFs was detected by X-ray diffraction
(XRD, Rigaku Ultima IV, Japan) with a scanning speed of 5°/min
in the scanning range of 10–80°. The absorption spectra
of the functional groups in RCFs were characterized by Fourier transform
infrared spectroscopy (FT-IR, Nicolet IS 50, Thermo Nicolet, USA)
with a spectral resolution of 4 cm–1 in the range
of 1000–3000 cm–1. Raman spectra of RCFs
were obtained with a laser wavelength of 532 nm and a scanning wavenumber
ranging from 500 to 2300 cm–1 (LabRAM HR Evolution,
Horiba Scientific, France). The surface elements and groups of RCFs
were analyzed by X-ray photoelectron spectroscopy (XPS, K-Alpha+,
Thermo Fisher Scientific, USA). The compositions of the pyrolysis
oil and gas were detected by gas chromatography–mass spectrometry
(GC-MS, Thermo Finnigan Trace DSQ, USA), in which the pyrolysis oil
and gas were tested by a headspace method and a direct injection method,
respectively.
Results and Discussion
Analysis of Pyrolysis Process
To
study the pyrolysis behavior of CFRPs and the oxidation behavior of
residual solids, thermogravimetric analyses were carried out under
atmospheres of argon and oxygen, respectively. As can be seen from
the TG curve in Figure a, the relative mass of residual solids after pyrolysis is about
77%, which is slightly higher than the mass fraction of CFs in the
CFRPs provided by the manufacturer. This is due to the formation of
pyrolytic carbon during pyrolysis.[19] The
epoxy resin in the CFRPs began to pyrolyze at about 300 °C, and
the pyrolysis was finished at about 600 °C. Therefore, a pyrolysis
temperature of CFRPs at 400–800 °C is more suitable. As
can be seen from the DTG curve in Figure b, the residual solids are slowly oxidized
in the range of 350–600 °C, and the oxidation rate increases
sharply after exceeding 600 °C due to the oxidization of CFs,
which is not conducive to the control of the oxidation degree. On
consideration of the performance, recovery rate, and processing efficiency
of RCFs, the suitable oxidation temperature in the experimental research
process was set in the range of 500–600 °C.
Figure 2
Thermogravimetric
analysis of (a) CFRP under an argon atmosphere
and (b) residual solids in an air atmosphere and simulation results
of (c) a model of the furnace cavity, (d) a model of CFRPs, (e) electromagnetic
field distribution in the furnace cavity, (f) electromagnetic field
distribution on CFRPs, (g) temperature field distribution on CFRPs,
and (h) heating curves.
Thermogravimetric
analysis of (a) CFRP under an argon atmosphere
and (b) residual solids in an air atmosphere and simulation results
of (c) a model of the furnace cavity, (d) a model of CFRPs, (e) electromagnetic
field distribution in the furnace cavity, (f) electromagnetic field
distribution on CFRPs, (g) temperature field distribution on CFRPs,
and (h) heating curves.To further study the
effect of microwave radiation on the pyrolysis
process of CFRPs, the electromagnetic field and temperature distribution
during the microwave heating of CFRP were simulated with COMSOL software.
The cavity of the microwave tube furnace and CFRP sheet were designed
on the basis of the actual object. As shown in Figures c,d, the dimensions of the furnace cavity
and CFRP sheet are 31 × 28 × 26 and 10 × 2 × 0.1
cm, respectively. Figure e shows the distribution of the electromagnetic field in the
furnace cavity, which is not symmetrical because the microwave generator
is in the upper left part instead of the center of the microwave tube
furnace. Figure f,g
gives the distributions of the electromagnetic and temperature fields
on the surface of CFRPs, respectively, indicating that the distribution
of temperature is directly related to the distribution of electromagnetic
field and that the stronger the electromagnetic field, the higher
the temperature. Figure h compares the actual heating curves and the simulated heating curve.
The simulated power was 500 W, and the actual powers were 400 and
500 W. It shows that the simulated heating curve has a high degree
of fitting with the actual curve, suggesting that the simulation results
will be consistent with the experimental results.
Mechanical Properties of RCFs
The
macroscopic morphologies of CFRP, residual solids, and RCFs are shown
in Figure . Figure a indicates that
CFs are coated with epoxy resin and tightly bonded together in CFRPs. Figure b shows the residual
solids obtained after pyrolysis of CFRPs, which have a flaky structure
and easily delaminate, but there are no filamentary products. RCFs
shown in Figure c
cannot be obtained directly, but they are obtained from oxidizing
the residual solids, which are filamentous products that can be easily
dispersed.
Figure 3
Pictures of (a) CFRP, (b) P500T15, and (c) P500T15D550T30 and SEM
images of (d) VCFs, (e) P500T15, and (f) P500T15D550T30.
Pictures of (a) CFRP, (b) P500T15, and (c) P500T15D550T30 and SEM
images of (d) VCFs, (e) P500T15, and (f) P500T15D550T30.The microscopic morphology of VCFs is shown in Figure d, and the fiber surface is
smooth and defect-free with a grooved structure. The microscopic morphology
of residual solids shown in Figure e indicates that some carbon residue is deposited on
the surface of CFs after pyrolysis, which makes it difficult to separate
a single carbon fiber. Laura et al.[33] also
observed that CFs after pyrolysis were covered by pyrolytic carbon,
which was caused by decomposition of the resin. Figure f shows the microscopic morphology of RCFs
obtained by oxidation, indicating that after the residual solids are
oxidized at 550 °C for 30 min the surface of RCFs is smooth and
clean, without carbon deposition and resin residue, and the grooved
structures are retained.By measurement of the mechanical properties
and recovery rate of
RCFs, the effects of different recycling conditions were evaluated. Figure a shows the tensile
strength of RCFs. With an increase in oxidation temperature and oxidation
time, the tensile strength of RCFs first increased and then decreased.
Under the condition of high oxidation temperature and long oxidation
time, part of the CFs will be oxidized to produce defects, resulting
in a decrease in the RCF mechanical properties.[34] In comparison with VCFs, the tensile strength of RCFs was
maintained at above 73% and the RCFs obtained under the condition
of P500T15D550T30 maintained the highest tensile strength (about 99.42%
of that of VCFs). Hao et al.[35] studied
the effect of different pyrolysis temperatures on the tensile properties
of RCFs. Under the condition of oxidation at 550 °C for 30 min,
the tensile strength loss was 13–20%. Figure b shows the tensile modulus of RCFs. With
an increase in oxidation temperature and oxidation time, the tensile
modulus increased continuously. In comparison with VCFs, the tensile
modulus of RCFs remains about 87.21% at the lowest level and increases
to 118.69% of that of VCFs at the highest level. Zabihi et al.[36] reported that the tensile modulus of CFs recycled
by a microwave-assisted chemical method was slightly improved by about
1.7%. The high retention rate of tensile strength and tensile modulus
indicates that microwave pyrolysis can recycle high-quality CFs.
Figure 4
Mechanical
properties and recovery rate of RCFs: (a) tensile strength;
(b) tensile modulus; (c) recovery rate.
Mechanical
properties and recovery rate of RCFs: (a) tensile strength;
(b) tensile modulus; (c) recovery rate.In Figure c, the
recovery rates of RCFs were calculated according to the weight of
CFs recycled under various reaction conditions. Under the condition
of P400T15D500T40, the highest recovery rate (97.9%) was obtained.
Under the condition of P500T15D550T40, the lowest recovery rate (96.4%)
was obtained. With the increase in reaction temperature and time,
the recovery rate of RCFs decreased gradually. However, the recovery
rate of RCFs can exceed 96% under all conditions. The recovery loss
is caused by the decomposition of the sizing agent on CF surface and
the partial oxidation of CFs; thus, an increase in temperature will
also reduce the recovery rate.
Structural
Changes of RCFs
XRD, Raman,
FT-IR, and XPS were used to study the changes of the carbon structure,
composition, and free radicals of RCFs. To analyze the structural
changes of RCFs, XRD patterns under different conditions are shown
in Figure a. The calculation
and analysis results of Figure a are given in Table . The diffraction peaks of all (002) crystal planes shift
to the left, which means that the unit cell parameters become larger
and the crystal plane spacing becomes larger. In comparison with VCFs,
the half-peak width of the diffraction peak of RCFs on the (002) crystal
plane becomes larger, while the grain size of the (101) crystal plane
becomes smaller, which means that the crystallinity is reduced, resulting
in the formation of defects and damage to the microstructure of RCFs.
These may lead to the degradation of the mechanical properties of
RCFs.
Figure 5
XRD patterns (a), Raman (b), FT-IR (c), and total XPS spectra (d)
of RCFs and C 1s spectra of VCFs (e), P500T15 (f), and P500T15D550T30
(g).
Table 2
Lattice Parameters
of RCFsa
(002)
peak
(101)
peak
2θ (deg)
d002 (Å)
fwhm
(deg)
Lc (Å)
2θ (deg)
d101 (Å)
fwhm (deg)
La (Å)
VCFs
25.04
3.63
5.33
15.11
43.71
2.56
2.98
28.43
P500T15
24.86
3.67
5.51
14.64
43.83
2.59
3.22
26.41
D500T40
24.80
3.69
5.27
15.27
43.74
2.59
3.15
26.88
D500T50
24.78
3.70
5.39
14.95
43.72
2.61
3.10
27.38
D550T30
24.86
3.64
5.44
14.79
43.64
2.58
3.11
27.37
D550T40
24.86
3.67
5.37
14.95
43.64
2.55
3.16
26.87
2θ is the position of the
diffraction peak, fwhm is the half-peak width of the diffraction peak, d002 and d101 are
the longitudinal and transverse plane spacings of the crystal in RCFs, L is the thickness of the (002)
plane, and L is the
grain size of the (101) plane.
XRD patterns (a), Raman (b), FT-IR (c), and total XPS spectra (d)
of RCFs and C 1s spectra of VCFs (e), P500T15 (f), and P500T15D550T30
(g).2θ is the position of the
diffraction peak, fwhm is the half-peak width of the diffraction peak, d002 and d101 are
the longitudinal and transverse plane spacings of the crystal in RCFs, L is the thickness of the (002)
plane, and L is the
grain size of the (101) plane.As shown in Figure b, two Raman peaks of CFs can be observed at around 1360 and 1580
cm–1. The D peak at 1360 cm–1 represents
the defect and graphitization disorder degree of carbon atoms, and
the G peak at 1580 cm–1 represents the in-plane
stretching vibration of sp2 hybridization of C atoms. The
intensity ratio R (ID/IG) reflects the disorder degree of
carbon atoms. The smaller the R value, the higher
the crystal integrity of CFs and the higher the proportion of ordered
structure of carbon atoms.[6] With an increase
in reaction temperature and reaction time, the Raman shift of the
D peak decreases and the R value increases, indicating
the decrease of the graphitization degree of RCFs. Jeong et al.[34] considered that a decrease in R value could increase the tensile strength of RCFs. According to
the results of this study, the change in tensile strength with the R value is consistent with the previous report.The
FT-IR spectra of RCFs are shown in Figure c. The tensile vibration peaks of the methyl
C–H bonds at 2960 and 2920 cm–1, the bending
vibration peaks of the methyl group at 1380 cm–1, and the tensile vibration peaks of the methylene group at 2850
cm–1 are all observed. The peaks at 2370 and 2340
cm–1 are caused by the tensile vibration of the
C≡N bond, and the peak at 1630 cm–1 corresponds
to the tensile vibration of the C=O bond. The symmetrical tensile
vibrations of the C–O bond are located at 2960 and 2920 cm–1. In comparison with VCFs, the peaks of methyl and
methylene groups and the C–O bond of the residual solid P500T15
are increased significantly, which was caused by the organic matter
attached to the surface of CFs after pyrolysis. After an oxidation
treatment of the residual solid, the intensity of the methyl peak
at 1380 cm–1 and the C–O bond peak at 1110
cm–1 decreased, and the methyl peaks at 2960 and
2920 cm–1 and the methylene peak at 2850 cm–1 disappeared, which was similar to the case for VCFs,
indicating that the oxidation treatment had a good recycling effect
and could achieve the expected purpose. Kim et al.[18] observed similar functional groups in their study and found
that these functional groups could form covalent interfacial bonds
with −COOH groups in the cross-linked polymer adhesives, effectively
transfer the stress between the matrix and fibers, and improve the
interfacial adhesion.XPS was used to further study the chemical
structure of the surface
of RCFs, as shown in Figure d–g. For VCFs and RCFs, the spectra contain three main
peaks, which represent carbon (C 1s, 284.99 eV), nitrogen (N 1s, 400.17
eV), and oxygen (O 1s, 532.42 eV), respectively. Table shows the contents of elements
and functional groups in the CFs. In comparison with VCFs, the content
of N atoms in RCFs increased, which was due to the incomplete removal
of sizing agents according to a study by Liu et al.[37] This can also be seen in the FT-IR spectra in Figure c, where the intensity
of the C≡N peak of RCFs is stronger than that of VCFs. The
differences between the functional groups on VCFs and RCFs were further
studied by fitting C 1s spectra, and the percentages of functional
groups are shown in Table . As shown in Figure e–g, the main peaks of C 1s spectra include C–C
(284.43 eV), C–O (286.28 eV), and O–C=O (288.63
eV), where C–O and O–C=O correspond to the functional
groups C–OH and −COOH, respectively.
Table 3
Contents of Elements and Functional
Groups in RCFs
element
content (%)
functional
group content (%)
C
O
N
O/C
C–C
C–O
O–C=O
VCFs
80.35
17.79
1.86
22.14
69.85
27.50
2.64
P500T15
86.85
10.03
3.12
11.55
84.15
12.81
3.04
D550T30
78.41
18.36
3.22
23.42
74.33
22.31
3.36
As shown in Table , in comparison with VCFs, the lower O/C ratio during
CFRP pyrolysis
results in higher contents of C and N atoms and C–C bonds but
lower contents of O atoms and C–O bonds. After the pyrolysis
of epoxy resin, C and N atoms remained on the surface of CFs, while
O atoms were released. After the oxidation of the residual solids,
the contents of C atoms and C–C bonds decreased, while the
contents of O atoms, C=O bonds and C–O bonds increased,
leading to a higher O/C ratio. Therefore, it can be inferred that
the oxidation of carbon leads to the breakage of C–C and C=C
bonds, resulting in the formation of C=O and C–O bonds.[36] The proportion of functional groups of RCFs
regenerated after oxidation treatment is similar to that of VCFs,
indicating that the regeneration effect of CFs is significant.
Composition Analysis of Pyrolysis Products
To study
the composition of the resin matrix after pyrolysis, GC-MS
was used to analyze the composition of the pyrolysis products at 500
°C. As shown in Table , the gas products mainly include carbon monoxide, carbon
dioxide, methane, ethane, and ethylene and the liquid products mainly
include benzene, phenol, p-isopropylphenol, bisphenol
A, and methyl tetrahydrophthalic anhydride. Bisphenol A is the monomer
of the epoxy resin, which is separated from the cured epoxy resin,
and further decomposes into benzene, phenol and p-isopropylphenol. This provides a reference for the harmless treatment
of pyrolysis products.
Table 4
Compositions of Pyrolytic
Gases and
Pyrolytic Oils
Conclusion
In this work, CFs were successfully recycled
from CFRPs by microwave
pyrolysis combined with an oxidation process. The resin matrix in
CFRP was rapidly decomposed by microwave pyrolysis. The pyrolytic
carbon and organic residues on the surface of CFs were removed by
oxidation at 500–550 °C for 30–50 min, and finally
RCFs with a smooth surface were obtained. The RCFs retained good mechanical
properties. The tensile strength ranged from 2243.81 to 3042.90 MPa,
and the tensile modulus ranged from 195.40 to 265.94 GPa. After microwave
pyrolysis and oxidation treatment, the chemical bond types of CFs
did not change significantly. For the resin decomposition product,
the main components were carbon monoxide, carbon dioxide, methane,
ethane, and ethylene in the gaseous product and the major liquid components
were benzene, phenol, p-isopropylphenol, bisphenol
A, and methyl tetrahydrophthalic anhydride. In short, RCFs with excellent
properties can be obtained from CFRPs by microwave pyrolysis combined
with an oxidation process. It has a huge market potential and is has
promise to be scaled up in the future.