1. Introduction
In recent years carbon fibers (CFs) have found applications in a wide variety of fields, including automotive, aircraft, electronic equipment, and sporting goods industries. Their use as reinforcement in composite materials is constantly growing even in fields more oriented towards mass production by replacing traditional metallic components, providing high specific mechanical properties which result in lower CO
2 emissions [
1]. Data analyses of this trend suggest that world production of CFs already doubled between 2009 and 2014 from 27 to 53 ktons and reached a maximum in 2022 with 117 ktons [
2].
Such a boost in the use of CFs affects the generation of wastes that derive both from the production process (process wastes representing about 30-40 wt.% of the total) and from the end of life of the products [
3].
Currently the main ways for the disposal of composite waste are incineration or landfilling, but these strategies will no longer be adequate due to environmental pollution and loss of CFs with high added value [
1].
Recently several recycling technologies have been proposed to treat composite materials with CFs and recover the CFs to reuse them in other applications for both economic and environmental reasons, aiming at the production of sustainable composites made by recycled reinforcement and recyclable matrix [
4].
The main technologies explored so far include mechanical recycling (shredding, crushing, milling), chemical recycling (solvent, catalyst, or supercritical fluids), and thermal recycling (pyrolysis, oxidation, steam thermolysis) and the objective of these techniques is to recover CFs in conditions as close to their initial state as possible to facilitate reuse in other applications [
5].
Mechanical recycling is currently one of the consolidated methods and involves several steps to reduce the size of waste. First, the composites are ground to a size of about 50-100 mm and then further grinding is applied to obtain recycled materials with different dimensions which can range from powder to fibrous agglomerates. The materials obtained from this type of recycling can be used as reinforcements in short-fiber composite materials such as those used for extrusion and injection molding. Because of the resultant limited fiber aspect ratio, these materials have a low market value [
6].
Due to the friction caused by materials during recycling, damage to equipment can occur, which directly increases the cost of various operations, and this decreases the economic margin of recycled materials, often making this choice less feasible. Dust produced by the recycling system is a major safety and health hazard, but it can be easily reduced with engineering controls and good ventilation [
3,
6].
In the case of chemical recycling, called solvolysis, the polymeric matrix is decomposed by a solution of acids, bases, and solvents whose composition must be adjusted according to the nature of the matrix. To increase the contact surface with the solution and aid in the dissolution of the matrix, solid composites are ground first. At the end of the process the CFs are washed to remove the decomposed polymer residues and the solvent residues.
Recycled CFs obtained in this way can be longer than mechanically ground ones and have been shown to maintain their tensile strength, with only a small percentage less than virgin CFs. However, the use of hazardous and concentrated chemicals has a significant environmental impact [
7].
In thermal recycling high temperatures are used to degrade the polymeric matrix and leave the CFs as a residue and it can be divided into different types. For thermal processes the operating parameters must be carefully controlled to avoid the loss of valuable products or the change in the chemistry of the recovered materials. If the process temperature is too low, the fiber surface is covered by a layer of amorphous carbon following the limited degradation of the matrix whereas if the temperature is too high, the CFs surfaces oxidizes with consequent reduction of the diameter of the fibers and mechanical properties in general [
1,
8,
9].
Therefore, the best way is at first to recover the long fibers through the process of pyrolysis, which will be later used to produce semi-finished products, such as non-woven fabrics, to be impregnated in a subsequent step. This step, in turn, generates a waste, namely the short fibers. The latter, through further processing, could be used in Fused Deposition Modeling (FDM) technology.
The mechanical properties of composite materials depend on many factors and the length of the fibers must certainly be mentioned among the main ones [
10].
Normally, short CFs reinforced composite materials are prepared using extrusion compounding and injection molding techniques and in addition to the initial length of the fibers it should be remembered that during the production of these composites, fiber breakage occurs due to fiber-fiber interaction [
11].
The manufacturing of filaments for 3D printing also falls within the scope of extrusion, which was the focus of this study.
3D printing has already been successfully applied in the manufacture of polymeric components ranging from prototypes to final products, but the main problem is that the resulting parts have inferior mechanical performance compared to parts fabricated using conventional techniques such as injection molding. To solve this problem, it has been seen that the addition of fibers in the polymer matrix forming a composite produces a significant improvement in the resistance of the molded parts [
12].
At present, thermoplastic polymers are the ones mostly used in these processes including acrylonitrile butadiene styrene (ABS), polylactic acid (PLA), polycarbonate (PC), and polyamide (PA).
In recent years many authors have studied the addition of short fibers in a thermoplastic polymer to create filaments of composite material used as raw material [
13]. All these studies analyzed the effect of fiber content, fiber orientation and length [
14], on the processability and performance of the manufactured components. In addition, some studies have reported comparisons between the properties of 3D printed composites and those manufactured with traditional molding techniques [
12,
15].
Among them, it can be worth mentioning the work of mechanical and morphological characterization and of PLA reinforced with 15 wt.% of short CFs carried out by Ferreira et al. [
14], the study of the effects of process parameters on the tensile properties of parts fabricated in ABS and CFs by Ning et al. [
16] and the investigation of engineering applications of PEEK composites and short CFs by Wang et al. [
17]. In their work, Ferreira et al. however show problems in the adhesion between PLA and CFs and an embrittlement of the reinforced material due to the addition of short CFs is reported [
14]. In the study by Ning et al. the effects of the process parameters on the tensile properties of the composites made by FDM are described, which have much in common with the composites made in the context of this study with the additive manufacturing technique [
16]. Wang et al. in their research instead deal with the production of composite materials in PEEK and CFs with variable fiber content between 5 and 15% by weight successfully produced by extrusion [
17].
In addition, the work by Giani et al. [
18], in which the applicability of recycled carbon fibers to produce CF-reinforced PLA composites is demonstrated, is also worth mentioning. In this case the comparison between the neat and the reinforced samples showed about a doubling of the elastic modulus and of the maximum stress.
All these results are particularly interesting given the ease of manufacturing filaments for FDM and 3D printing and confirm the possibility of applying CFs in these areas, also by exploiting different matrices as environmental and economically sustainable alternatives.
The carbon fibers used in this study fall into the category of waste generated directly by the production process that uses a waste material and the main aim lies in the identification of a potential application for this by-product considered as a processing waste up to now. In particular the rCFs have been evaluated as reinforcement in a PA6,6 matrix for the production of filaments for 3D printing.
In this article the problems related to the size of the fibers used and the presence of a preponderant dusty fraction will be addressed. Furthermore, the possible solutions to this problem will be considered and the improvements in terms of mechanical properties will be evaluated.
4. Optimization Hypothesis
In the light of what has been investigated, it can be said that the reinforcing action of rCF was not significant due to the implementation of a filler with an unsuitable l/d ratio. For instance, the values of the Young's modulus and the tensile strength in our case for the composite loaded with 10 wt.% of rCF are respectively 2.24 GPa and 59.53 MPa on average, which correspond to an improvement in mechanical behavior of 21% and 5% compared to the neat PA6,6 specimens. These values are markedly lower than results available in the literature (reviewed in
Section 3.2.1.) implementing CF in 3D printed composites.
The main cause that led to such limited strength performance is certainly the unsuitable average size of the CFs used. As already mentioned, indeed, in the reinforcement used there is a preponderant dusty fraction, and the longer fibers are then further crushed during the various phases of extrusion of the filament and subsequent printing. As mentioned, the fibers used as reinforcement are obtained by grinding, in a ball mill, inextricable agglomerates of recycled fibers. A possibility of optimization is therefore to act on the grinding phase, studying in detail an operation that allows to grind the agglomerates, untangling the fibers, but obtaining fibers of adequate length to improve the mechanical properties of rCF-reinforced composites.
In this regard it is possible to obtain an ideal length measurement through studies on the mechanical behavior of short-fiber composites. First, it is necessary to understand the effect of discontinuous fibers in a polymeric matrix by studying the mechanism of reinforcement of the fibers. The fibers exert their effect by limiting the deformation of the matrix and in this way the applied external load is transferred to the fibers by shear at the fiber/matrix interface. In short fibers the tensile stress increases from zero at the ends up to a value σ
max which would occur if the fibers were continuous. σ
max can be determined from equation (1):
where σc is the stress applied to the composite and El can be determined via the rule of mixtures.
Therefore, there is a minimum fiber length that will allow the fiber to reach its full loading potential. The minimum fiber length at which maximum fiber stress can be achieved is called the load transfer length (l
t) and the value can be determined from a force balance (2):
where
τ is the shear strength of the fiber/matrix interface and
d is the diameter of the fiber [
38]. Note that
lt is also a function of the stress applied to the composite.
Let us consider the case of the composite material with 10 wt.% of rCFs. To carry out the calculation and estimate an attempt value for lt for our specific case we need to extrapolate the values for σmax, τ and the Young's modulus of the CFs only (Ef).
As regards the σ
max, as a first approximation it can be assumed that the specimen breaks during the tensile test for pull-out as observed from the SEM analysis. As regards the τ value, reference was made to the experimental value obtained for a PA matrix composite reinforced with desized CFs by Kim et al. [
37]. The value of τ is set equal to 24 MPa. Finally, the value of Young's modulus for carbon fibers alone is considered equal to 230 GPa [
39].
Applying the rule of mixtures:
with Ef and Em modulus of fibers and matrix and Vf and Vm, volume fraction of the fibers and the matrix, respectively.
The fiber length obtained estimated in the calculation widely exceeds the average size of carbon fillers integrated in the composite with 10 wt% of rCF (~ 19 µm), supporting the poor performance improvement of the composite.
However, it should be noted that the ideal length of 115 µm must be the average length of the fibers already incorporated into the composite and not after the ball mill processing. It was verified that, between the milled rCF and the effective production of the composite material, the fibers undergo breaking which led to maximum loss of about 37% in length (for PA6,6 + 10 wt.% rCF). To compensate for the damaging effect of extrusion, preserving adequate l/d ratio for obtaining effectiveness in mechanical performances and assuring adequate printability of the material, an average dimension ranging between 200-300 µm can be proposed. These values clearly consider the average size of the input waste carbon agglomerates which are subjected to milling to obtain the filler implemented in the present research.
Figure 1.
Schematization of the double recovery action.
Figure 1.
Schematization of the double recovery action.
Figure 2.
SEM micrograph of a sample of carbon microfibers.
Figure 2.
SEM micrograph of a sample of carbon microfibers.
Figure 3.
EDS analysis spectrum and atomic percentage of the elements.
Figure 3.
EDS analysis spectrum and atomic percentage of the elements.
Figure 4.
Machine setup for the extrusion of 3D printing filaments.
Figure 4.
Machine setup for the extrusion of 3D printing filaments.
Figure 5.
3D printing filaments obtained from extrusion processing.
Figure 5.
3D printing filaments obtained from extrusion processing.
Figure 6.
Tensile test on a filament.
Figure 6.
Tensile test on a filament.
Figure 7.
Filament samples for density measurements.
Figure 7.
Filament samples for density measurements.
Figure 8.
3D printed dumbbell-shaped samples.
Figure 8.
3D printed dumbbell-shaped samples.
Figure 9.
SEM micrograph of neat PA6,6 filament – 250 x.
Figure 9.
SEM micrograph of neat PA6,6 filament – 250 x.
Figure 10.
(a) SEM micrograph of PA6,6 + 5 wt.% rCF filament; (b) Detail of rCF embedded into the matrix.
Figure 10.
(a) SEM micrograph of PA6,6 + 5 wt.% rCF filament; (b) Detail of rCF embedded into the matrix.
Figure 11.
(a) SEM micrograph of PA6,6 + 10 wt.% rCF filament; (b) Detail of rCFs embedded into the matrix.
Figure 11.
(a) SEM micrograph of PA6,6 + 10 wt.% rCF filament; (b) Detail of rCFs embedded into the matrix.
Figure 12.
Carbon microfibers under the optical microscope.
Figure 12.
Carbon microfibers under the optical microscope.
Figure 13.
Fiber size distribution.
Figure 13.
Fiber size distribution.
Figure 14.
Tensile test results: tensile strength and Young's modulus values of each manufactured filament.
Figure 14.
Tensile test results: tensile strength and Young's modulus values of each manufactured filament.
Figure 15.
Tensile test results: tensile strength and Young's modulus values of 3D printed dumbbell samples.
Figure 15.
Tensile test results: tensile strength and Young's modulus values of 3D printed dumbbell samples.
Figure 16.
3D printed composite specimens during tensile test: (a) PA6,6 neat and (b) PA6,6 composite.
Figure 16.
3D printed composite specimens during tensile test: (a) PA6,6 neat and (b) PA6,6 composite.
Figure 17.
Stress-strain behavior of 3D printed dumbbell samples.
Figure 17.
Stress-strain behavior of 3D printed dumbbell samples.
Figure 18.
SEM micrographs of neat PA6,6 specimen. The dotted circles highlight inter-filament voids in the matrix.
Figure 18.
SEM micrographs of neat PA6,6 specimen. The dotted circles highlight inter-filament voids in the matrix.
Figure 19.
SEM micrographs of (a) PA6,6 + 5 wt.% rCF and (b) PA6,6 + 10 wt.% rCF specimens. The dotted circles highlight inter-filament voids in the matrix.
Figure 19.
SEM micrographs of (a) PA6,6 + 5 wt.% rCF and (b) PA6,6 + 10 wt.% rCF specimens. The dotted circles highlight inter-filament voids in the matrix.
Figure 20.
SEM micrographs of fracture surface of PA6,6 + 5 wt.% rCF specimen: (a) general view of the surface and (b) distribution of rCFs in the matrix.
Figure 20.
SEM micrographs of fracture surface of PA6,6 + 5 wt.% rCF specimen: (a) general view of the surface and (b) distribution of rCFs in the matrix.
Table 1.
Physical and mechanical properties of BASF Ultramid® 1000-11 NF2001 PA6,6 from the technical data sheet.
Table 1.
Physical and mechanical properties of BASF Ultramid® 1000-11 NF2001 PA6,6 from the technical data sheet.
Properties |
Values |
Comments |
Density |
1.14 g/cc |
ISO 1183 |
Water Absorption |
8.5% |
ISO 62 |
Moisture Absorption at Equilibrium |
2.5% |
23 °C/50% R.H.; ISO 62 |
Tensile Strength, Yield |
83.0 Mpa |
50 mm/min; ISO 527 |
Elongation at Break |
25% |
50 mm/min, Normal strain; ISO 527 |
Elongation at Yield |
5.0% |
50 mm/min; ISO 527 |
Tensile Modulus |
3.00 Gpa |
1 mm/min; ISO 527 |
Flexural Strength |
117 Gpa |
ASTM Test |
Flexural Modulus |
2.90 Gpa |
ASTM Test |
Melting Point |
257 °C |
10 K/min ASTM Test |
Table 2.
Temperature profiles employed during extrusion of PA6,6 filaments (neat and composites).
Table 2.
Temperature profiles employed during extrusion of PA6,6 filaments (neat and composites).
|
PA6,6 neat filament |
PA6,6 + rCF |
Zone 1 Temperature, °C |
255 |
260 |
Zone 2 Temperature, °C |
255 |
260 |
Zone 3 Temperature, °C |
260 |
265 |
Zone 4 Temperature, °C |
260 |
265 |
Zone 5 Temperature, °C |
260 |
265 |
Zone 6 Temperature, °C |
255 |
260 |
Zone 7 Temperature, °C |
250 |
255 |
Die Temperature, °C |
235 |
240 |
Screw speed, rpm |
150 |
150 |
Table 3.
Standard deviation of fiber dispersion in the specimens.
Table 3.
Standard deviation of fiber dispersion in the specimens.
Sample |
std. dev. |
PA6,6 neat |
1.129 ± 0.026 g/cm3
|
PA6,6 + 5 wt.% rCF |
1.148 ± 0.019 g/cm3
|
PA6,6 + 10 wt.% rCF |
1.164 ± 0.014 g/cm3
|
Table 4.
Density values of CFs, neat PA6,6, and PA6,6 composites and estimated theoretical values of the percentage of reinforcement in composite filaments.
Table 4.
Density values of CFs, neat PA6,6, and PA6,6 composites and estimated theoretical values of the percentage of reinforcement in composite filaments.
Material |
Method |
Value |
rCFs |
helium pycnometer |
1.917 g/cm3
|
PA6,6 neat filament |
buoyancy balance |
1.129 g/cm3
|
PA6,6 + 5 wt.% rCF filament |
buoyancy balance |
1.148 g/cm3
|
PA6,6 + 10 wt.% rCF filament |
buoyancy balance |
1.164 g/cm3
|
Percentage of rCF reinforcement |
PA6,6 + 5 wt.% rCF filament |
Rule of mixtures |
2.41 %v/v |
PA6,6 + 10 wt.% rCF filament |
4.44 %v/v |
Table 5.
Effective percentage of reinforcement in composite filaments obtained by acid attack.
Table 5.
Effective percentage of reinforcement in composite filaments obtained by acid attack.
Material |
Value |
PA6,6 + 5 wt.% rCF filament |
3.40 %v/v |
PA6,6 + 10 wt.% rCF filament |
6.79 %v/v |