Selection Route of Precursor Materials in 3D Printing Composite Filament Development for Biomedical Applications
Abstract
:1. Introduction
2. Materials and Methods
2.1. Sample Preparation
2.2. Sample Characterisation
2.2.1. FTIR-ATR Spectroscopy Measurements
2.2.2. Raman Spectroscopy Measurements
2.2.3. Morphological Evaluation
2.2.4. Biocompatibility Experiments
3. Results and Discussion
3.1. FTIR-ATR Measurements
- ABS: The bands were attributed to (a) styrene isomers—deformation (out of phase sequence) of C–H groups (702, 759 cm−1); (b) acrylonitrile isomers—symmetric stretching of C≡N groups (2239 cm−1); and (c) butadiene isomers—asymmetric bending of CH2 groups as low-frequency peaks (1370, 1449 cm−1), symmetric stretching of C=C (1648 cm−1) and C=O (1754 cm−1) groups. Additionally, a split-peak corresponding to the symmetric stretching of C–O–C groups and a low-intensity peak associated with the aliphatic symmetric stretching of C–H groups were identified at 1041, 1080 cm−1, and 2925 cm−1, respectively. However, the emergence of the carbonyl (C=O) stretching band, slightly shifted from its usual position at 1718 cm−1 (when identified), could be assigned to an oxidation state of the polymer in the butadiene region, as also found in ref. [7], thus suggesting reduced elasticity features that could interfere with the polymer processing and final mechanical performance.
- PLA: The main functional bands were assigned to the C=O groups—symmetric stretching (756, 1754 cm−1); C–O–C groups—symmetric (1090 cm−1) and asymmetric (1193 cm−1) stretching; methyl (CH3) groups—symmetric (1453 cm−1) and asymmetric (2997 cm-1) stretching; and (–CH) groups—symmetric (2858 cm−1) and asymmetric (2927 cm−1). Additionally, the deformation (bending mode) of the C–H groups and the possible vibration of the C–COO group could be identified as low-intensity peaks at 1368 and 873 cm−1, respectively, as also found in refs. [13,25,27].
- GNP: For both types of graphene nanoplatelets (grade C and M), at similar intensities, the characteristic bands were ascribed to C–O groups—symmetric stretching (1045 cm−1); C=C groups—aromatic stretching (1567, 1645 cm−1); and C=O groups—symmetric stretching (1721 cm−1). Comparatively, at very low intensities, the deformation (bending mode) of the hydroxyl (–OH) functionalities and the symmetric (phenolic) stretching of the C–OH groups were identified at 1388, 1440 cm−1 and 1159, 1254 cm−1, respectively. At wavenumbers slightly shifted to the right for the grade M sample as compared to the grade C sample, the bands for the aromatic deformation of the C–H groups (870, 874 cm−1) and the symmetric stretching of CH2 groups (2910, 2917 cm−1) were also present, as similarly reported in ref. [50]. No additional peaks specific to the hydroxyl group (free or connected) in the >3000 cm−1 range were found here, in contrast to other records [37,51,52].
- HA: The bands characteristic of the symmetric and asymmetric stretching of orthophosphate tetrahedral units (PO4)3− were assigned at 963 cm−1 and 1038 cm−1, respectively. Compared to pure, highly crystalline commercial HA [53], the spectra of the bovine bone-derived HA also elicited low-intensity bands specific to asymmetric stretching (centred at ~1455 cm−1) modes of carbonate groups. Carbonation of calcium phosphates synthesised under normal atmospheric conditions was expected and repeatedly reported in our previous studies [12,15,16]. Moreover, the involved HA is also monophasic and free of any traces of other molecules, confirming the reproducibility of the synthesis method [16,44].
ABS | PLA | GNP_C | GNP_M | HA | IR Band Assignment |
---|---|---|---|---|---|
Wavenumber Positions [cm−1] | |||||
702 | - | - | - | - | def. (out of phase) of C–H groups in S 1 [26,54,55,56] aromatic bending of C–H groups [7] |
- | 756 | - | - | - | sym. stretching of C=O group [21] |
759 | - | - | - | - | def. (out of phase) of C–H groups in S 1 [26,54,55,56] aromatic bending of C–H (=CH) groups [7] |
- | - | 870 | 874 | - | aromatic deformation of C–H groups [50] |
- | 873 | - | - | - | C–COO group vibrations [13] |
- | - | - | - | 963 | sym. stretching (ν1) of (PO4)3− groups [3,16,20,44] |
- | - | - | - | 1038 | asym. stretching (ν3) of (PO4)3− groups [3,16,44] |
1041 | - | - | - | - | sym. stretching of C–O–C groups [56] |
- | - | 1045 | 1045 | - | sym. stretching (ν1) of C–O groups [52,57,58] |
1089 | - | - | - | - | sym. stretching of C–O–C groups [56] |
- | 1090 | - | - | - | sym. stretching of C–O–C groups [13,21,59] |
- | - | 1159 | 1159 | - | sym. (phenolic) stretching (ν1) of C–OH groups [50,58] |
- | 1193 | - | - | - | asym. stretching of C–O–C groups [13,21,59] |
- | - | 1254 | 1254 | - | sym. (phenolic) stretching (ν1) of C–OH groups [37,50,58] |
- | 1368 | - | - | - | def. bending of C–H groups [25,27] |
1370 | - | - | - | asym. bending of CH2 groups in B 3 | |
- | - | 1388 1440 | 1388 1440 | - | def. bending of (–OH) groups [50,58] |
1449 | - | - | - | - | asym. bending of CH2 groups in B 3 [7,54,56,60,61] |
- | 1453 | - | - | - | sym. stretching of CH3 groups [21,25,27] |
- | - | - | - | 1455 | asym. stretching (ν3) of (CO3)2− groups [15,16,25] |
- | - | 1567 1645 | 1567 1645 | - | aromatic stretching of C=C groups [52,57,62] |
1648 | - | - | - | - | sym. stretching of C=C groups in B 3 [7,56,63] |
- | - | 1721 | 1721 | - | sym. stretching of C=O groups [50,57,58] |
1754 | - | - | - | - | stretching of C=O group in B 3 [7] |
- | 1754 | - | - | - | sym. stretching of C=O groups [20,21,25,27,59,64] |
2239 | - | - | - | - | sym. stretching of C≡N groups in AN 2 [26,56,60,61,63,65] |
- | 2858 | - | - | - | sym. stretching of (–CH) groups [21,25] |
- | - | 2910 | 2917 | - | sym. stretching of CH2 groups [50] |
2925 | - | - | - | - | aliphatic sym. stretching of C–H groups [7,54,56,60,61,63] |
- | 2927 | - | - | - | asym. stretching of (–CH) groups [13,21,25] |
- | 2997 | - | - | - | asym. stretching of CH3 groups [5,13,21,25] |
3.2. Raman Measurements
- ABS: The main bands were designated to (a) the vibrational modes of the benzene ring in styrene isomers—deformation (in-plane mode) (636 cm−1), breathing mode (1006 cm−1), shearing (in-plane mode deformation) of the C–H groups (1183 cm−1), symmetric stretching of the C–C groups (1602 cm−1), and stretching of the (=C–H) groups (3059 cm−1) with the highest intensity; (b) the deformation of CH2 groups (1326 cm−1); and (c) the stretching of C≡N groups (2239 cm−1) in acrylonitrile isomers.
- PLA: The main vibrational bands corresponded to the C=O groups—weak (677 cm−1), moderate (760 cm−1) and stretching (1871 cm−1) modes; the CH3 groups—asymmetric functional mode (1115 cm−1), symmetric (1388 cm−1), and asymmetric (1549 cm−1) deformation of the functional mode, symmetric (2933 cm−1) and asymmetric (2979 cm−1) stretching modes with the most prominent intensities. In addition, the symmetric stretching of the C–COO groups (917 cm−1) and the asymmetric moderate mode of the C–O–C groups (1203 cm−1) were confirmed, according to ref. [21].In the case of the reinforcement materials, the Raman shifts outlined the following:
- GNP: The two sets of intense characteristic peaks for carbon nanostructures were assigned to the D band—specific to disordered/disrupted hexagonal graphitic lattice or internal structural defects [50,57,68] at 1362 cm−1 and 1359 cm−1 for grade C and M samples, respectively. The G band, generated by the stretching of the functional C–C groups, was also indexed at 1593 cm−1 and 1567 cm−1 for grade C and M samples, respectively, and is related to the structural disorder [57,68]. It was stated that the broader the G band in the Raman spectra, the higher the oxidation performance of the graphite [50]. As such, given the prominent intensity and narrower G band position, we can assume that for the grade M sample, a significant number of graphitic areas remained unmodified after processing [57,69]. However, for both sample types, the identification of the 2D (G’) band (sensitive to the thickness, number, and stacking of graphene layers in a flake [36,70,71,72]) in the 2700–2930 cm−1 range was supported by other studies [70,71,72]. In the case of the GNP_grade M sample, due to the higher diameter surface and thickness of the nanoparticles that interact with the laser beam [70], a well-defined high intensity peak was formed in this area, as expected. It was also reported that the intensity is directly dependent on the number of graphene layers [71].
- HA: Only the typical bands of the (PO4)3− groups in the HA structure were depicted: the asymmetric (1044 cm−1) and symmetric (960 cm−1) stretching mode, the bending (431 cm−1) mode, and the out-of-plane bending (589 cm−1) mode.
ABS | PLA | GNP_C | GNP_M | HA | Raman Shift Assignment |
---|---|---|---|---|---|
Raman Shifts [cm−1] | |||||
- | - | - | - | 431 | bending (ν2) of (PO4)3− groups [3,13,20,73] |
- | - | - | - | 589 | bending (ν4) of (PO4)3− groups [3,13,20,73] |
636 | - | - | - | - | def. (in-plane mode) of benzene ring [66,67,74] |
- | 677 | - | - | - | weak C=O groups [21] |
- | 760 | - | - | - | moderate C=O groups [21] |
- | 917 | - | - | - | sym. stretching of C–COO groups [13,21,64] |
- | - | - | - | 960 | sym. stretching (ν1) of (PO4)3− groups [3,20,73] |
1006 | - | - | - | - | breathing of benzene ring [66,67,74] |
- | - | - | - | 1044 | asym. stretching (ν3) of (PO4)3− groups [3,20,73] |
- | 1115 | - | - | - | asym. functional CH3 groups [21] |
1183 | - | - | - | - | def. shearing (in-plane mode) of C–H groups in benzene ring [66,74] |
- | 1203 | - | - | - | asym. moderate C–O–C groups [21] |
1326 | - | - | - | - | def. of CH2 groups [66] |
- | - | 1362 | 1359 | - | D (disordered) band [50,57,68,69,75] |
- | 1388 | - | - | - | sym. def. of functional CH3 groups [21,76,77] |
- | 1549 | - | - | - | asym. def. of functional CH3 groups [21,76,77] |
- | - | 1593 | 1567 | - | G (graphitic) band [50,57,68,69,75] |
1602 | - | - | - | - | sym. stretching of C–C groups in the benzene ring in S 1 [54,66,67] |
- | 1871 | - | - | - | stretching of C=O groups [13,21,76,77] |
2239 | - | - | - | - | stretching of C≡N groups in AN 2 [54,61,66,67] |
- | - | 2706 | 2719 | - | 2D (G’) band [70,71,72] |
- | - | 2929 | - | - | 2D (G’) band [70,71,72] |
- | 2933 | - | - | - | sym. stretching of CH3 groups [13,21,77] |
- | 2979 | - | - | - | asym. stretching of CH3 groups [13,21,77] |
3059 | - | - | - | - | stretching of (=C–H) groups in benzene ring [66,67,74] |
3.3. Morphology Evaluation
- ABS: Regardless of the physical state, the ABS surface outlined the presence of a continuous and homogenous matrix (also known as the SAN matrix) and some light-white sub-micrometric inclusions corresponding to the butadiene-specific particle content, as mentioned in refs. [61,65]. The microstructure of the new material depicted a slightly rough and uneven distribution of the two phases at a higher magnification. Moreover, the ABS in the form of a thin plate conversed to a morphology of rubbery-like lines and grooves after flattening. Implicitly, in this state, a more prominent roughness and irregular disposal of the content materials occurred.
- PLA: The initial PLA granules mainly displayed a wrinkled surface with few pores of sub-micrometric diameters. In contrast, the processing into a plate shape acted as an adjuvant for uniform surface smoothing and complete reduction of the pores/voids.
- GNP: The microstructure was clearly influenced by the GNP nanoplatelet dimensions: the grade C samples demonstrated an accentuated tendency to form clusters/irregular aggregates with a width of a few micrometres, which appeared mostly as particulates, rather than as platelets structures, which is consistent with other reported findings [36,38]. This predilection of the GNP_grade C graphene is well-known and attributed to the strong van der Waals interactions [50]. Comparatively, the grade M samples exposed a unitary flake-like microstructure with well-separated and layered nanoplatelets of variable sizes and orientations [58,62,71].
- HA: The coarse surface and polyhedral form of the ceramic particles were conserved for all dimensional sorts. However, if the particles size was in the <40 μm range, they tended to conglomerate into larger micrometric aggregates. Additionally, as a direct consequence of the synthesis technology [45], the HA particles acquired a microporous surface, which is considered to be beneficial for a more intimate contact and adhesion to other materials used as matrix for composite filaments (e.g., polymeric materials) [43]. When addressed differently, this feature of the ceramic particles is sometimes challenging and rather difficult to achieve [5,27].
3.4. In Vitro Pre-Osteoblast Behaviour
4. Conclusions
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Conflicts of Interest
References
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Mocanu, A.-C.; Miculescu, F.; Constantinescu, A.E.; Pandele, M.-A.; Voicu, Ș.I.; Cîmpean, A.; Miculescu, M.; Negrescu, A.M. Selection Route of Precursor Materials in 3D Printing Composite Filament Development for Biomedical Applications. Materials 2023, 16, 2359. https://doi.org/10.3390/ma16062359
Mocanu A-C, Miculescu F, Constantinescu AE, Pandele M-A, Voicu ȘI, Cîmpean A, Miculescu M, Negrescu AM. Selection Route of Precursor Materials in 3D Printing Composite Filament Development for Biomedical Applications. Materials. 2023; 16(6):2359. https://doi.org/10.3390/ma16062359
Chicago/Turabian StyleMocanu, Aura-Cătălina, Florin Miculescu, Andreea Elena Constantinescu, Mădălina-Andreea Pandele, Ștefan Ioan Voicu, Anișoara Cîmpean, Marian Miculescu, and Andreea Mariana Negrescu. 2023. "Selection Route of Precursor Materials in 3D Printing Composite Filament Development for Biomedical Applications" Materials 16, no. 6: 2359. https://doi.org/10.3390/ma16062359
APA StyleMocanu, A. -C., Miculescu, F., Constantinescu, A. E., Pandele, M. -A., Voicu, Ș. I., Cîmpean, A., Miculescu, M., & Negrescu, A. M. (2023). Selection Route of Precursor Materials in 3D Printing Composite Filament Development for Biomedical Applications. Materials, 16(6), 2359. https://doi.org/10.3390/ma16062359