Crystallization Behavior and Mechanical Properties of Poly(ε-caprolactone) Reinforced with Barium Sulfate Submicron Particles

Abstract

Poly(ε-caprolactone) (PCL) was mixed with submicron particles of barium sulfate to obtain biodegradable radiopaque composites. X-ray images comparing with aluminum samples show that 15 wt.% barium sulfate (BaSO₄) is sufficient to present radiopacity. Thermal studies by differential scanning calorimetry (DSC) show a statistically significant increase in PCL degree of crystallinity from 46% to 52% for 25 wt.% BaSO₄. Non-isothermal crystallization tests were performed at different cooling rates to evaluate crystallization kinetics. The nucleation effect of BaSO₄ was found to change the morphology and quantity of the primary crystals of PCL, which was also corroborated by the use of a polarized light optical microscope (PLOM). These results fit well with Avrami–Ozawa–Jeziorny model and show a secondary crystallization that contributes to an increase in crystal fraction with internal structure reorganization. The addition of barium sulfate particles in composite formulations with PCL improves stiffness but not strength for all compositions due to possible cavitation effects induced by debonding of reinforcement interphase.

1. Introduction

In recent years, there has been an increasing interest in biodegradable polymers for biomedical applications as temporary surgical implants and templates for tissue engineering. Polyesters based on polylactides and polylactones present tremendous interest in this field because of their biocompatibility, tunable mechanical properties and biodegradability [1,2,3,4,5,6]. Among these polymers, poly(ε-caprolactone) (PCL) stands out, as it widely used in tissue engineering and drug delivery platforms [7,8,9,10,11,12].

Despite its success as implantable material, in comparison to metals, its low radiopacity makes it difficult to detect by X-ray imaging techniques. Hence, to overcome this difficulty, the use of composites with high radiopaque fillers is being investigated. Barium sulfate (BaSO₄) [13,14,15], ferrous oxide (Fe₃O₄) [16] and bismuth oxide (Bi₂O₃) [17,18] have been previously reported as radiopaque composite fillers, and BaSO₄ is currently the most commonly used in medical applications. Barium sulfate (BaSO₄) is a standard in medical applications, approved by the FDA and used for X-ray assisted implantation to control the position of polymer implants and drug delivery systems during biodegradation [9,19,20].

The incorporation of BaSO₄ has been reported to be an alternative to improve the toughness of, for example, polylactides [21,22]. However, its use also might negatively affect other mechanical properties depending on the particle content. For instance, barium sulfate as an inorganic reinforcement has been already reported to be used with various polymer matrices such as polyethylene, polypropylene and poly(lactic acid); performance was reported to be reduced at large filler contents [23,24,25,26]. The fail in mechanical properties is often explained in terms of poor compatibility of the matrix–reinforcement interface [27]. In the particular case of PCL, a number of authors have demonstrated poor compatibility with other fillers [28,29,30]. These two facts, the relative content of the particle and the matrix–reinforcement interface, play an important role in the correct use of PCL-based devices. On the one hand, to obtain sufficient radiopacity, weight percentages of about 25% are necessary for commonly used BaSO₄ particles in medical applications. On the other hand, the particle content that ensures sufficient radiopacity must preserve or improve the mechanical properties of the base material. Therefore, an equilibrium must be found between these two variables.

Moreover, incorporating inorganic particles in a crystallizable polymer matrix affects the crystallization kinetics, crystal morphology and final degree of crystallinity of the base polymer [22,31]. Therefore, in this work, a complete study of crystallization of PCL in presence of BaSO₄ particles is presented. PCL at human body conditions (≈37 °C) is above its glass transition temperature (T_g ≈ −60 °C). At these conditions, mechanical properties of PCL are soft and strongly related to degree of crystallinity. In fact, previous research has shown the important effect of fillers on polymer crystallinity depending on the composition, content, size and morphology of the reinforcement [29,30,32]

There is growing evidence in the literature that recognizes the importance of the development of biodegradable radiopaque polymeric systems for being used as medical devices. Studies over the past two decades have provided important information on the physical–mechanical properties of PCL. However, to date, the relationship between crystallization behavior, mechanical properties and radiopacity upon BaSO₄ particle addition has not yet been extensively studied. Therefore, the aim of this research work was to study the role of BaSO₄ in the crystallization behavior, mechanical properties in terms of the particle–matrix interface and radiopacity, establishing the minimum BaSO₄ content needed to preserve the mechanical performance.

2. Materials and Methods

Poly(ε-caprolactone) (PCL) CAPA6500, with an average molecular weight (M_w) of 147.6 KDa and a dispersity index (D) of 1.49 was provided by Solvay (Perstorp, Sweden). Barium sulfate (BaSO₄) was provided by Fluka Analytical (Sigma Aldrich). Particle size was determined by dynamic light scattering (DLS) on a Zetasizer ZS90 ZEN3690 (Malvern Instrument, UK), showing an average diameter of 577 ± 125 nm.

2.1. Sample Preparation

PCL and BaSO₄ composites were prepared by melt mixing in an MC5 conical twin-screw mixer (Xplore, The Netherlands) at 150 °C and 150 rpm for 30 min. Compositions with 5, 15, 25 and 35 wt.% BaSO₄ were prepared (see name codes in

Table 1. Name codes of composite samples showing real barium sulfate content after processing as calculated by TGA analysis.

Sample (Name Code)	BaSO4 Content (wt.%)	Real BaSO4 Content (wt.%)
PCL	0	0
PCL_05BaSO4	5	8.4
PCL_15BaSO4	15	14.2
PCL_25BaSO4	25	25.0
PCL_35BaSO4	35	32.5

). Sheets of 1 mm thickness of neat PCL and composites were prepared from pellets by compression molding in a Dr. Collin P200E hot press (Collin, Germany) at 150 °C and 25 MPa.

The amount of barium sulfate present in samples after processing was measured by thermogravimetric analysis (TGA) in a TGA model Q50 (TA instruments). Samples of 10–15 mg were heated from room temperature to 500 °C at a rate of 10 °C min⁻¹ under a nitrogen atmosphere. Three different samples (n = 3) were used to determine the content of BaSO₄ in the samples. A slide difference was found between the actual and real content of the particle (see Table 1).

2.2. Non-Isothermal Crystallization Kinetics

Before the non-isothermal crystallization treatments, the thermal history of the samples was erased by increasing the temperature to 100 °C, and then non-isothermal crystallization treatments were carried out from melt by cooling the samples at cooling rates of 1, 5 and 10 °C min⁻¹. Thermal properties of the samples were measured in a subsequent differential scanning calorimeter (DSC) run by heating from –85 to 100 °C at a rate of 20 °C min⁻¹ in a nitrogen atmosphere. The DSC employed was a Q80 differential scanning calorimeter (DSC) (TA instruments) calibrated with pure indium and sapphires. In all cases, three different samples (n = 3) weighting 7 ± 1 mg were used. Cooling cycles were monitored. The melting temperature (T_m) was determined from the endothermic peak position, and the melting enthalpy (ΔH_m) was obtained by calculating the area under the melting peak.

2.3. Crystal Morphology

Spherulitic morphology of samples was observed with a LEICA DM LM polarized light optical microscope (PLOM) (LEICA, Spain). Samples were dissolved in dichloromethane to obtain films by solvent casting on a microscope glass slide. Non-isothermal crystallization treatments were conducted by a heat controlling Mettler FP90 hot stage (Mettler Toledo, Spain) at the conditions described previously.

2.4. Mechanical Testing

Tensile testing was conducted in an Instron 5565 universal testing machine according to ISO 37-2 standard. Samples of 4 mm width were cut from the molded sheets, and at least five samples (n = 5) were employed for mechanical properties measurements. Testing was performed at a crosshead speed of 10 mm min⁻¹. Young’s modulus (E) with a linear fitting at initial 2% of strain, yield strength (σ_y), stress at break (σ_b) and strain at break (ε_b) were determined.

2.5. X-ray Images

Radiographs of samples were taken using an X-radiographic standard clinical machine X-ray IRIS 70 (Trophy, UK). As a reference, a 1 mm aluminum plate was employed. All the samples including the reference and neat PCL were tested using the same intensity for comparative purposes. Exposure time was 0.16 s.

3. Results

3.1. Crystallization Behavior and Crystal Morphology

The incorporation of barium sulfate (BaSO₄) decreased the melting temperature and increased the degree of crystallinity of poly(ε-caprolactone) (PCL), as revealed by diferential scanning calorimetry (DSC) (see Figure 1 and

Table 2. Thermal properties and degree of crystallinity of poly(ε-caprolactone) (PCL) and its BaSO₄ composites. T_m: melting temperature; ΔH_m: melting enthalpy; X_c: degree of crystallinity.

Sample (Name Code)	BaSO4 Content (wt. %)	Tm (°C)	ΔHm (J/g)	Xc (%)
PCL	0	67.0 ± 0.8	70.5 ± 1.1	46
PCL_05BaSO4	8.4	65.3 ± 0.8	68.2 ± 0.7	49
PCL_15BaSO4	14.2	64.5 ± 0.5	64.8 ± 0.6	49
PCL_25BaSO4	25.0	64.2 ± 0.5	59.1 ± 1.0	52
PCL_35BaSO4	32.5	63.4 ± 1.2	52.6 ± 2.0	51

). The melting temperature monotonously decreased from 67 °C for neat PCL to 63.4 °C when incorporating 35 wt.% BaSO₄, suggesting smaller and less perfect crystalline structures. The degree of crystallinity (X_c) of PCL and its composites was calculated according to Equation (1), where ΔH_m is the melting enthalpy, ΔH_m° is the melting enthalpy of 100 % crystalline PCL taken as 139 J g⁻¹ [33] and X_BaSO4 is the real barium sulfate fraction in samples obtained by thermogravimetric analysis (TGA) (see Table 1).

$$X_{\mathrm{c}}(\%)=\frac{\Delta H_{\mathrm{m}}}{\Delta H_{\mathrm{m}}^{°}}\times \left(\frac{1}{{1-X}_{\mathrm{BaSO}4}}\right)$$

(1)

The degree of crystallinity increased from 46% to 52%, which is statistically significant for compositions of 25 and 35 wt.% (p = 0.03 and p = 0.007).

PCL and its BaSO₄ composites were subjected to non-isothermal crystallization treatments in situ in a polarized light optical microscope (PLOM). The resultant crystal morphology after samples were cooled from melt at cooling rates of 1, 5 and 10 °C min⁻¹ were studied and compared. As expected, smaller spherulites were observed in samples cooled at higher cooling rates than in their counterparts due to molecules having less time for diffusion. In Figure 2, images taken at cooling rates of 1 and 10 °C min⁻¹ are compared for neat PCL and PCL containing 5 and 35 wt.% BaSO₄. Regardless of the cooling rate, no significant differences were found in crystal size between composites having low particle content, 5 wt.%, and neat PCL. However, the incorporation of higher particle contents, 35 wt.%, did have an influence on crystal size. For example, PCL shows a spherulitic structure with an average size of 100 µm and clear grain boundaries when cooled at 1 °C min⁻¹, whereas the composite having 35 wt.% BaSO₄ shows an average size of 5 µm. When comparing the crystal morphology of PCL at different cooling rates, the result reveals a highly distorted and more planar spherulitic structure at higher cooling rates. However, when BaSO₄ particles are incorporated, this spherulitic morphology, though distorted as in neat PCL, becomes rounder.

3.2. Non-Isothermal Crystallization and Kinetics Analysis

To analyze in more detail the non-isothermal crystallization, cooling curves from DSC were analyzed for PCL and its BaSO₄ composite cooled at cooling rates of 1, 5 and 10 °C min⁻¹ (see Figure 3). A crystallization peak is observed between 30 and 40 °C for all compositions, yet in composites, this is observed at higher temperatures, suggesting heterogeneous nucleation induced by BaSO₄ particles. At higher cooling rates, the crystallization peaks translate to lower temperatures for neat PCL and composite samples (see

Table 3. Crystallization temperature and crystallization enthalpy of PCL and its BaSO₄ composites at different cooling rates.

Sample (Name Code)	Cooling Rate (°C min−1)	Tc (°C)	ΔHc (J g−1)
PCL	1	33.7	62.3
	5	28.7	57.7
	10	24.8	54.1
PCL_05BaSO4	1	37.8	67.9
	5	32.8	62.6
	10	29.9	59.6
PCL_15BaSO4	1	37.5	68.1
	5	31.8	63.0
	10	28.8	60.4
PCL_25BaSO4	1	38.5	71.2
	5	33.2	66.5
	10	30.7	63.7

). Moreover, the crystallization degree during cooling increases with BaSO₄ content as deduced from the increase in the crystallization enthalpy (see Figure 4). Therefore, the presence of the inorganic particles in PCL not only provides nucleation sites and accelerates crystallization kinetics but also leads to a higher degree of crystallinity. Furthermore, lower cooling rates favor both nucleation and the final degree of crystallinity in neat PCL and its composites. The crystallization peak temperatures and crystallization enthalpy for each composition at the selected different cooling rates are summarized in Table 3.

The evolution of the degree of crystallinity with time is shown in Figure 5 for the different cooling rates. Crystallization kinetics was studied by analyzing the degree of crystallinity as a function of temperature according to Equation (2), where T₀ and T_∞ are initial and final temperatures of the crystallization process and dH_c is the crystallization enthalpy at temperature difference dT and at temperature T. The crystallization time during the process was assessed according to Equation (3), where T_c is the crystallization temperature at crystallization time t and Φ is the cooling rate.

$$X\left(T\right)={{\displaystyle \int }}_{T_0}^T\left(\frac{\mathrm{d}{H}_{\mathrm{c}}}{\mathrm{d}T}\right)\mathrm{d}T/{{\displaystyle \int }}_{T_0}^{T_{\infty }}\left(\frac{\mathrm{d}{H}_{\mathrm{c}}}{\mathrm{d}T}\right)\mathrm{d}T,$$

(2)

$$t=\left(T\mathrm{c}-T\right)/\Phi .$$

(3)

In accordance with DSC results, the evolution of the degree of crystallinity over time indicates the nucleating effect of BaSO₄ particles advancing the onset of crystallization in regard to PCL. Moreover, the results revealed that crystallization might be accelerated by the presence of BaSO₄. This was further assessed by employing crystallization models.

For crystallization kinetic analysis, the Avrami-Ozawa-Jeziorny (A-O-J) model was employed. Polymer crystallization kinetics can be described by Avrami’s model for phase changes at isothermal conditions [34] by Equation (4), where 1 – X_t is the non-crystallized volume fraction, “n” is a parameter that defines the type of crystal growth and Z_t is a combined factor of nucleation rate and crystal growth rate. In non-isothermal conditions, the Ozawa model [35] can be employed by following Equation (5). Note that both equations are quite similar, although the Z_t and “n” parameters do not have the same physical meaning because the temperature varies constantly in non-isothermal crystallization. For our study, the Ozawa model could not be employed as some bibliographic results show that this model does not satisfactorily fit the PCL crystallization process [36,37]. Therefore, the change to Z_t proposed by Jeziorny [38] was applied for Avrami´s model being used in non-isothermal conditions. Equation (6) describes the change proposed by Jeziorny in order to unify Avrami´s and Ozawa’s models for non-isothermal conditions. In this equation, Φ is the cooling rate and Z_c a factor obtained from non-isothermal conditions with the equivalent meaning of Z_t in the Avrami model. In order to obtain “n” and Z_c factors, a linear fitting must be applied for log(–ln(1 – X_t)) versus log(t) curves.

$$1-X_{\mathrm{t}}=e^{-Z_{\mathrm{t}}·t^n},$$

(4)

$$1-X_{\mathrm{t}}=e^{-Z_{\mathrm{t}}·{\mathsf{\Phi }}^m},$$

(5)

$$\log \left(Z_{\mathrm{c}}\right)=\frac{\log \left(Z_{\mathrm{t}}\right)}{\mathsf{\Phi }}.$$

(6)

Figure 6 shows the double logarithmic curves of PCL and its composites fitting the crystallization model proposed. The experimental data do not fit in a simple linear manner and show in all cases a more complex crystallization behavior. This finding is consistent with reported bibliographic results for PCL, suggesting the existence of a secondary crystallization process [36,37,39]. This secondary crystallization is common in other polymers with similar thermal properties, such as HDPE, when the working conditions are high above the glass transition temperature [40]. Therefore, in this work, a double linear behavior was considered for data fitting, obtaining positive results (r ≥ 0.9).

Figure 7 shows an example of the simple and double linear model adjustments of crystallization kinetics of PCL and its BaSO₄ composites. The values of the double fitting model parameters (n_i and Z_ci) are summarized in

Table 4. The parameters of the double linear Avrami–Ozama–Jeziorny model for PCL and its BaSO₄ composites at different cooling rates.

Sample (Name Code)	Φ (°C min−1)	Zc1 × 106	n1	r1	Zc2 × 106	n2	r2
PCL	1	393	3.06	0.96	112,010	1.12	0.90
	5	26,661	3.00	0.97	134,567	1.24	0.96
	10	93,981	2.46	0.97	138,174	1.65	0.98
PCL_05BaSO4	1	311	3.76	0.94	156,060	1.01	0.91
	5	22,345	3.68	0.94	157,177	1.08	0.95
	10	130,814	3.69	0.97	149,402	1.33	0.96
PCL_15BaSO4	1	353	3.68	0.91	171,962	0.98	0.92
	5	24,246	3.73	0.95	159,310	1.09	0.94
	10	145,824	3.65	0.97	161,103	1.30	0.95
PCL_25BaSO4	1	266	3.86	0.91	173,790	0.99	0.90
	5	25,408	3.79	0.95	169,341	1.05	0.94
	10	169,961	3.81	0.97	170,617	1.22	0.93
PCL_35BaSO4	1	339	3.70	0.91	136,477	1.08	0.89
	5	21,298	3.72	0.95	144,059	1.17	0.94
	10	229,399	3.92	0.97	147,983	1.39	0.92

.

For the first linear fitting, n₁ is always higher for composite samples and is close to the theoretical factor of 4corresponding to a three-dimensional crystallization according to the model. In contrast, neat PCL presents a factor closer to 3, which slightly decreases when the cooling rate is increased. The values for composite samples do not change with cooling rate and are not dependent on BaSO₄ quantity. For the same sample, Z_c1 rises abruptly with the cooling rate due to the usual effect of nucleation enhancement by fast cooling. The increase in particle content shows an incremental effect on this factor at high cooling rates, 10 °C min⁻¹, whereas for low cooling rates, 1 °C min⁻¹, all samples have similar behavior.

The kinetics study according to this model shows that nucleation of PCL crystals is led by the presence of BaSO₄ particles in a primary crystallization process to form spherulitic morphology. In fact, PLOM images showed that for low cooling rates, nucleation and growth of crystals in PCL were favored. The presence of BaSO₄ leads to heterogeneous nucleation points at the interfaces starting the crystallization process earlier than in neat PCL, with an increase in the degree of crystallinity also observed in previous results. When the cooling rate is increased, however, the nucleating effect becomes more relevant because the effect of particles on the crystallization of PCL is enhanced.

Secondary crystallization is also important; up to 40% of total crystallization has been attributed to it [41]. Three reasons might be proposed to explain this: (1) new lamellae are formed in the amorphous phase, (2) lamellae become thicker or (3) new lamellae grow at particle interfaces. This secondary crystallization just after primary crystallization (identified with a black arrow in Figure 7) is observable in the DSC normalized cooling curves (Figure 3) and crystallinity versus time plots (Figure 5). An inclination that can be attributed to secondary crystallization can be observed. Irrespective of BaSO₄ content, the value of the n₂ factor is low, between 1 and 2, suggesting a process more related to molecular reorganization than crystal growth. For the same sample, this factor increases with cooling rate, leading to distorted spherulitic crystals in accordance with the results obtained from PLOM analysis.

3.3. Mechanical Properties

The stiffness of PCL was significantly increased with the increase in barium sulfate content in composites, with values of Young’s modulus ranging from 308 MPa for non-reinforced PCL to 397 MPa for its 35 wt.% BaSO₄ composite counterpart. This effect on modulus was statistically significant starting from the 15 wt.% composite (p = 0.018) (see Figure 8c and

Table 5. Values of the mechanical properties measured by tensile test for neat PCL and its BaSO₄ composites. Young’s modulus (E), yield stress and yield strain (σ_y, ε_y), yield plateau stress (σ_yp) and elongation at break (ε_b)

Sample (Name Code)	E* (MPa)	σy (MPa)	εy (%)	σyp (MPa)	εb (%)
PCL	308 ± 9	13.8 ± 0.5	10.2 ± 1.5	12.1 ± 0.2	714 ± 27
PCL_05BaSO4	336 ± 11	14.1 ± 0.3	10.9 ± 0.8	11.9 ± 0.2	841 ± 23
PCL_15BaSO4	353 ± 4	13.7 ± 0.2	9.9 ± 0.3	11.4 ± 0.2	615 ± 92
PCL_25BaSO4	368 ± 8	13.6 ± 0.3	8.8 ± 0.7	11.3 ± 0.2	623 ± 28
PCL_35BaSO4	397 ± 19	12.7 ± 0.2	6.5 ± 0.3	10.1 ± 0.1	557 ± 50

* E is defined by linear fitting at first 2% of strain.

).

The yield strength remained constant irrespective of the presence of BaSO₄ content until 35 wt.% BaSO₄, for which a decrease was found (p = 0.03) (see Figure 8d). Focusing on the shape of plasticization peak curves at the yield point, one can observe that the region becomes narrower and appears at lower strains as the BaSO₄ content increases in composites (see Figure 8b). Moreover, yield plateau stress after plasticization peak decreased to lower stress levels, being significant for compositions of up to 15 wt.% BaSO₄ (p = 0.04) (see Figure 8e). This drop in stress after the peak is indicative of cavitation induced by debonding of matrix–reinforcement interphase, and thus it might be concluded that filler content has a negative effect.

Regarding ductility, some decrease in elongation at break was observed at higher amounts of reinforcement in composites in regard to neat PCL. However, it is noticeable that all samples regardless of BaSO₄ amount remained ductile with values of elongation at break higher than 557% (see Table 5 and Figure 8f). This result is statistically significant for 5 wt.% (p = 0.01), and the decreasing tendency for high content is notable (p = 0.065 for 35 wt.% BaSO₄).

The results demonstrate that the BaSO₄ particles in PCL are acting in the linear strain zone at low strains of the tensile stress–strain curve (see Figure 8a) as a usual stiff reinforcement for polymers. The increase in modulus in PCL with inorganic reinforcements is quite common [28,30,36,42]. The effect of the matrix-particle interfaces becomes relevant and affects the mechanical properties at higher strain values of the stress–strain curves. If the interface adhesion is poor [29], an increase in yield strength is not expected; debonding at the interfaces would prevent the reinforcing effect at the strain value at which the yield point appears. Interface debonding and cavitation explain the behavior of the yield region in which the strain is observed to appear at lower strain values; hence, yield stress drops for high amounts of BaSO₄. This behavior is consistent with previous works provided for PCL composites, which evidenced a decrease in yield stress even when compatibilizing agents for the interface were used to improve the adhesion level [28]. Barium sulfate as reinforcement with PCL behaves similarly to calcium sulfates, which show increments in yield stress at medium reinforcement amounts and then a decrease in yield stress at >15 wt.% [32]. The behavior observed here for the PCL matrix also corroborates effects found for BaSO₄ composites with other semicrystalline matrices such as polypropylene (PP) or polyethylene (PE) [23,43,44]. In this work, the falling in yield strength was not observed as BaSO₄ particle content increased to a high amount (35 wt.%). This fact suggests a contributing effect of the crystal nucleation and growth in presence of particles, as also observed by DSC and PLOM, leading to an increased degree of crystallinity in PCL composites that compensates the detrimental effects of cavitation and debonding.

Finally, the impact of BaSO₄ particles on the strain capacity of the polymer matrix can be discussed for submicron and nano-sized particles, as it has been proved that they provide an enhancement in the toughness of PLA at low particle amounts (≤10 wt.%) [21,44]. However, for higher particle amounts, a decrease in toughness is expected because debonding and cavitation occur, leading to a decrease in the strain capacity of composite formulations. Micron-sized holes, coalescence and, finally, cracks that develop during stretching of samples lead to decreasing values of elongation at break, as was observed here for PCL-BaSO₄ composites. Therefore, it can be concluded that the addition of BaSO₄ particles in quantities from 5 to 25 wt.% is optimal for polymer composites of PCL without a detrimental effect on toughness.

3.4. X-ray Imaging and Radiopacity Assessment

Figure 9 shows the X-ray images of 1 mm thickness films of PCL and its 5, 15, 25 and 35 wt.% barium sulfate composites compared to 1 mm thickness aluminum film. Barium sulfate particles increased the radiopacity of PCL, as expected. Samples with 5 wt.% barium sulfate were detectable, and samples with 25 wt.% barium sulfate had radiopacity comparable to that of aluminum.

4. Conclusions

The main goal of the current study was to study the relationship between crystallization behavior, mechanical properties and radiopacity of poly(ε-caprolactone) (PCL) and its barium sulfate (BaSO₄) composites. In this work, we prepared samples of PCL with different contents (0, 5, 15, 25 and 35 wt.%) of submicron particles of BaSO₄ with an average size of 577 nm.

Thermal studies showed a statistically significant increase in PCL degree of crystallinity during cooling from melt in presence of BaSO₄ particles. Non-isothermal crystallization kinetics of PCL in the absence and presence of BaSO₄ particles were assessed at 1, 5 and 10 °C min⁻¹ cooling rates from melt. The nucleating effect of BaSO₄ was found to change the morphology and degree of crystallinity of the primary crystals of PCL, which was also corroborated by the use of a polarized light optical microscope (PLOM). The experimental data were well fitted to the Avrami-Ozawa-Jeziorny model, and the determination of the corresponding parameters revealed a secondary crystallization that contributes to an increase in the degree of crystallinity with internal structure reorganization.

The addition of barium sulfate particles in composite formulations with PCL improved stiffness, but the other relevant mechanical properties (strength, elongation and toughness) were not optimal. This is attributed to the debonding and cavitation at the particle–matrix interfaces in which adhesion plays a pivotal role.

Moreover, X-ray images show that 15 wt.% BaSO₄ is sufficient to present radiopacity for devices to be visible for use in medical imaging techniques.

One of the more significant findings to emerge from this study is that PCL presents sufficient radiopacity with tough mechanical properties when mixed with 25 wt.% BaSO₄ submicron particles. This finding is of broad use to the scientific and biomedical communities, as this composite fulfilled the required conditions for monitoring implants and drug delivery devices by X-ray imaging techniques.