3.1. Box–Behnken Design Results
The experimental results obtained from the BBD are presented in
Table 3, which summarizes the tensile and flexural strength values corresponding to each of the 15 parameter combinations. These results provide valuable insights into how the selected printing parameters influence the mechanical behavior of FDM-printed parts. Specimens fabricated with PPA/Cf consistently exhibited the highest mechanical performance across all configurations. The highest tensile strength (75.8 MPa) and flexural strength (102.3 MPa) were recorded in Run 3, where the PPA/Cf material was used with “Cross” infill and “Flat” direction. This indicates that the synergistic effect of optimized fiber alignment and infill geometry plays a crucial role in enhancing load-bearing capacity. In contrast, ABS samples showed the lowest mechanical properties, with the minimum tensile strength (37.8 MPa) and flexural strength (49.5 MPa) observed in Run 11 (“Grid” infill, “Upright” direction), highlighting the relatively lower stiffness and interlayer adhesion of ABS compared to fiber-reinforced composites. The sandwich structures, which combine the ductility of ABS and the stiffness of PPA/Cf, demonstrated intermediate performance between the two pure materials. For instance, in Run 5 (“Grid” infill, “Flat” direction), the sandwich specimen achieved a tensile strength of 62.1 MPa and a flexural strength of 84.1 MPa, outperforming pure ABS while remaining below the best-performing PPA/Cf samples. This confirms the effectiveness of the hybrid configuration in balancing strength and material economy. The sandwich structure, which positions carbon fiber-reinforced PPA at the outer skins and unreinforced material at the core, exhibits intermediate mechanical performance compared to full-carbon fiber or full-unreinforced configurations. This balanced behavior offers a practical compromise between strength, weight, and material cost. Such a configuration is particularly advantageous in applications where moderate mechanical strength, reduced weight, and material efficiency are all critical design requirements. This structure may be highly suitable for automotive interior components, drone or UAV airframes, protective casings, or tooling fixtures, where stiffness and dimensional stability are needed, but full reinforcement may be unnecessary or economically inefficient. Moreover, the sandwich layout may contribute to vibration damping and thermal insulation, making it a compelling choice for multi-functional engineering parts. These practical implications highlight the potential of the sandwich configuration in lightweight structural design.
Another critical factor influencing mechanical outcomes was the PD. Specimens printed in the “Flat” or “On-edge” orientations generally yielded higher tensile and flexural strengths compared to those printed in the “Upright” direction. This trend can be attributed to improved interlayer bonding and better alignment of load paths with the direction of applied force in Flat/On-edge orientations. For example, comparing Runs 2 (ABS, Grid, Flat) and 11 (ABS, Grid, Upright), a significant drop in both tensile and flexural strength is evident when the orientation changes from Flat to Upright. Lastly, the effect of IP also manifested noticeably, particularly for PPA/Cf and sandwich specimens. The “Cross” pattern often resulted in slightly higher mechanical strength compared to “Grid” or “Triangles”, likely due to its more uniform stress distribution and enhanced internal connectivity. The influence on IP appears to be secondary to that of MT and PD. The BBD results clearly indicate that MT is the dominant factor affecting mechanical performance, followed by PD and IP. These findings form the basis for subsequent regression modeling and ML analysis, allowing for data-driven prediction and optimization of part strength in FDM processes.
3.2. Interaction Effect Plots
Interaction effect plots were generated using the experimental results from the BBD to better understand the combined effects of printing parameters on mechanical performance. These interaction charts, shown in
Figure 3a–f, illustrate how two parameters interactively influence the tensile and flexural strength of FDM-printed specimens. Such visualizations are crucial for identifying nonlinear trends and synergistic or antagonistic relationships between variables. In
Figure 3a, the interaction between PD and IP is presented. The results show that the “Flat” PD results in the highest strengths across most patterns, especially for the “Cross” pattern. However, when the direction changes to “On-edge” or “Upright”, performance decreases significantly for certain patterns like “Grid”, indicating a strong dependency between build orientation and internal geometry.
Figure 3b displays the interaction between IP and MT. PPA/Cf consistently outperforms ABS and sandwich materials across all IPs. The “Grid” pattern yields relatively better results for PPA/Cf, while “Cross” and “Triangles” perform similarly for sandwich composites. ABS shows the lowest strength values, with minor variation across patterns, suggesting that the effect of infill pattern on ABS is less pronounced than on stiffer materials. The interaction between PD and MT is illustrated in
Figure 3c. Across all orientations, PPA/Cf exhibits the highest strength, especially in the “Flat” and “On-edge” directions. However, a noticeable drop is observed in the “Upright” direction for all materials. This confirms the well-known limitation of FDM when printing in the vertical direction, where interlayer adhesion is weaker, leading to reduced tensile and flexural strength. In
Figure 3d, the interaction plot for MT versus IP is revisited to highlight potential nonlinear relationships. The “Cross” pattern again emerges as the most favorable infill structure for both PPA/Cf and sandwich materials, while ABS remains relatively unaffected. This reinforces the idea that internal geometry plays a more critical role in high-performance or fiber-reinforced materials.
Figure 3e further explores the interaction between IP and PD. The results are consistent with earlier findings: “Flat” and “On-edge” directions generally yield better strength values, particularly when combined with “Cross” or “Grid” patterns. The “Upright” direction shows poor performance regardless of infill type, emphasizing its mechanical disadvantage. Finally,
Figure 3f examines the interaction between MT and PD. PPA/Cf again shows superior strength in the “Flat” direction, followed by “On-edge”, while “Upright” causes the greatest reduction in performance. Sandwich composites follow a similar trend but with slightly lower values, and ABS consistently ranks lowest, especially in the “Upright” direction. These results confirm that both material stiffness and layer bonding orientation are dominant factors in determining the mechanical integrity of FDM parts. The interaction plots in
Figure 3 reveal that the combined influence of printing parameters is often more significant than their individual effects. This highlights the necessity of using multi-factorial experimental designs like BBD and supports the implementation of data-driven models for accurate prediction and optimization of mechanical performance in FDM processes.
Pareto charts of standardized effects, created using the results from the BBD, provided a quantitative view of how each printing parameter influenced mechanical performance. These charts—shown in
Figure 4a for tensile strength and
Figure 4b for flexural strength—visualize the magnitude and statistical significance of each factor’s effect, ranked from most to least influential. The vertical red dashed lines indicate the critical t-value thresholds (2.31 for tensile and 2.57 for flexural strength), above which the effects are considered statistically significant at a 95% confidence level. MT (Factor A) has by far the most dominant effect on tensile strength, exceeding the significance threshold by a wide margin (
Figure 4a). This result aligns with previous findings, where specimens printed with PPA/Cf consistently outperformed those made from ABS or sandwich composites. The IP (Factor B) also shows a statistically significant but smaller effect, indicating that internal geometry plays a secondary yet meaningful role in enhancing tensile performance. PD (Factor C) falls below the significance threshold, suggesting that while orientation has some influence—particularly on interlayer bonding—its effect on tensile strength is comparatively limited when material and infill are optimized. Similarly,
Figure 4b shows the Pareto chart for flexural strength, and the trends are consistent. MT remains the most influential factor, followed by IP and PD, both of which again fall below the critical threshold. The slightly higher critical value (2.57) for flexural strength may explain why fewer parameters reach significance, but the overall hierarchy remains the same. These Pareto analyses confirm that MT is the single most critical factor affecting both tensile and flexural performance of FDM-printed parts. While IP can fine-tune the performance, especially in composite or hybrid structures, printing direction alone does not yield statistically significant changes under the tested conditions. These insights are essential for guiding parameter selection during the design phase, and they also validate the structure of the predictive models developed in the following sections.
3.3. Analysis of Variance Results
The statistical significance of the selected process parameters on both tensile and flexural strength was evaluated using ANOVA. The results are summarized in
Table 4, which presents the degrees of freedom (DF), adjusted sums of squares (Adj SS), mean squares (Adj MS), F-values, and corresponding
p-values for each factor. For tensile strength, the ANOVA results indicate that all three parameters have statistically significant effects at the 95% confidence level. MT is the most influential factor, with a very high F-value of 201.44 and a
p-value of 0.000, confirming its dominant role in determining tensile performance. PD also shows a highly significant effect (F = 64.50,
p = 0.000), highlighting the importance of layer orientation and interlayer bonding in tensile loading. IP, while less dominant, still contributes significantly (F = 24.87,
p = 0.003), suggesting that internal geometry affects stress distribution and crack propagation paths. A similar trend is observed for flexural strength. Again, MT has the highest impact (F = 102.23,
p = 0.000), followed by PD (F = 31.13,
p = 0.000) and IP (F = 17.07,
p = 0.001). These values confirm that the bending behavior of FDM parts is also strongly dependent on the stiffness of the material and the orientation of the printed layers. The
p-values for all three parameters are below 0.005, indicating a high level of statistical significance. The lack-of-fit test was also included to assess the adequacy of the regression model. For tensile strength, the lack-of-fit F-value is 29.95 with a
p-value of 0.033, indicating a statistically significant lack of fit. This suggests that while the model captures the general trend well, there may be some non-linearities or interactions not fully accounted for by the current model. Potential sources of this lack of fit may include nonlinear interactions between process parameters (e.g., material type and infill pattern), as well as microstructural variability introduced during manual filament switching in the sandwich-structured specimens. Furthermore, higher-order effects or unmodeled dependencies may also contribute to the unexplained variance. Although the model provides reasonable predictive performance, these findings highlight the need for more complex modeling approaches—such as including additional interaction terms or applying nonlinear regression techniques—in future studies to reduce the lack of fit and improve model fidelity. In contrast, for flexural strength, the
p-value for lack of fit is 0.095, which is above the 0.05 threshold, indicating that the model fits the data reasonably well for bending behavior. The ANOVA findings confirm that all three printing parameters have a statistically significant influence on mechanical properties. Among them, MT consistently exhibits the greatest impact, followed by PD and IP.
The percentage contributions of MT, IP, and PD to the mechanical performance of FDM-printed parts were calculated based on their Adj SS values obtained from the ANOVA results, allowing further quantification of each parameter’s relative impact. The results are visualized in
Figure 5a for tensile strength and in
Figure 5b for flexural strength. As depicted in
Figure 5a, for tensile strength, MT is the dominant factor, contributing 69.05% of the total variation in the response. This reinforces the earlier statistical findings that the intrinsic properties of the materials, such as stiffness, fiber reinforcement, and interlayer bonding, play a critical role in load-bearing capacity. PD contributes 23.25%, indicating that layer orientation and the direction of applied stress significantly affect tensile behavior, particularly due to anisotropic properties inherent in FDM processes. IP, while statistically significant, accounts for only 7.53% of the variation, suggesting that although internal geometry influences stress distribution, its effect is relatively minor compared to the other two parameters. In the case of flexural strength, shown in
Figure 5b, the contribution of MT is even more pronounced, rising to 76.25%. This suggests that bending resistance is even more sensitive to material stiffness and structural composition than tensile strength. PD contributes 15.01%, while IP accounts for 8.15%, showing a similar trend of decreasing influence. The relatively smaller impact of printing direction in bending (compared to tensile) could be attributed to the fact that bending loads are more evenly distributed along the part’s cross-section, partially mitigating the anisotropic effects. These percentage-based contribution analyses confirm that MT is by far the most critical parameter in determining both tensile and flexural performance. While PD plays a supportive yet significant role, especially in tensile loading, IP serves as a fine-tuning parameter that can help optimize performance when combined with appropriate materials and orientations. The outcome of this analysis supports the rationale for prioritizing material selection in both design and predictive modeling, and it further validates the regression and ML models developed in the subsequent sections.
3.4. Regression Model Results
Predictive models for estimating the mechanical properties of FDM-printed parts were developed using multiple regression analysis based on experimental data from the BBD. The models aim to correlate the effects of MT, IP, and PD with the resulting tensile and flexural strength values. Quadratic regression equations were derived to account for potential non-linearities and interaction effects. The resulting regression equations are as follows:
These equations show that MT has the highest linear and quadratic influence on both tensile and flexural strength, consistent with the findings from ANOVA and contribution analyses. The negative quadratic coefficients indicate diminishing returns or possible optimal levels for each parameter. The accuracy and validity of the regression models were assessed using R
2 and diagnostic plots. The R
2 value for tensile strength was found to be 0.9895, while for flexural strength, it was 0.9885. These high R
2 values indicate that the models explain more than 98% of the variability in the experimental data, demonstrating excellent fitting performance. The timescale plots compare the actual and predicted values across 15 experimental runs (
Figure 6a,b). The predicted data closely follows the actual measurements, with minimal deviation, further verifying the robustness of the regression models. The normal probability plots in
Figure 6c for tensile strength and
Figure 6d for flexural strength illustrate that the residuals approximately follow a normal distribution. The
p-values obtained from Anderson–Darling tests are 0.096 and 0.193 for tensile and flexural strength, respectively—both above the 0.05 threshold—indicating no significant deviation from normality and thus validating the assumptions of the regression analysis. The regression models developed in this study offer high predictive accuracy and satisfy the assumptions of linear regression. These models serve as reliable tools for estimating mechanical performance based on key FDM process parameters and form the foundation for more advanced predictive techniques, such as ML algorithms, presented in the following section.
In addition to prediction accuracy, the computational efficiency of the two models is also important for practical implementation in AM workflows. GPR, while highly flexible and capable of modeling complex, nonlinear relationships, is computationally intensive, especially as the training dataset grows. Its training complexity scales cubically with the number of observations (O(n3)), which can limit its scalability for large datasets or real-time applications. In contrast, BLR offers significantly greater computational efficiency due to its closed-form posterior inference and simpler model structure. This enables faster training and prediction times, making it more suitable for real-time decision-making or integration into AM control systems where computational resources may be limited. Therefore, while GPR may provide slightly higher accuracy in modeling complex behaviors, BLR presents a favorable trade-off in scenarios where speed and resource efficiency are critical.
3.5. Machine Learning Algorithm Results
In recent years, ML has become an indispensable tool in the field of AM, especially for process optimization and mechanical property prediction. The highly nonlinear and multi-parametric nature of FDM makes it difficult to capture complex interactions using classical statistical models alone. ML algorithms offer a data-driven approach that can learn from experimental data and generate highly accurate predictive models, even with relatively small datasets. In this study, two supervised learning algorithms—GPR and BLR—were implemented to predict the tensile and flexural strength of 3D-printed parts based on the input parameters: MT, IP, and PD. These algorithms were selected due to their suitability for small datasets and their ability to provide probabilistic outputs, including prediction intervals. The ML models were developed and trained using the Regression Learner App in MATLAB. The dataset obtained from the BBD was first normalized and then split into training and validation sets using k-fold cross-validation (k = 5) to ensure generalizability. GPR was implemented with an exponential kernel function, while BLR used a Bayesian regularization approach to prevent overfitting. The exponential kernel was preferred over more commonly used kernels such as the squared exponential (RBF) because it is better suited for capturing less smooth, potentially abrupt variations in the response due to discrete changes in FDM process parameters. Unlike the RBF kernel, which assumes smooth and infinitely differentiable functions, the exponential kernel can accommodate localized, nonlinear effects that are more representative of real-world material behavior in AM. Preliminary cross-validation results showed that the exponential kernel yielded lower prediction error and better generalization on validation data, further justifying its selection.
A systematic hyperparameter optimization process was applied for both GPR and BLR to ensure the robustness, accuracy, and generalizability of the ML models. For GPR, a grid search strategy was employed to evaluate multiple kernel functions and their associated hyperparameters. The tested kernels included Squared Exponential (RBF), Matern 5/2, Rational Quadratic, and Exponential. Among these, the rational quadratic kernel yielded the best predictive performance. Key hyperparameters were optimized within the following ranges: length scale (l) from 0.1 to 5.0 (step size: 0.1), noise level (α) from 1 × 10−6 to 1 × 10−2 (logarithmic scale), and the scale mixture parameter from 0.1 to 10.0. The optimal configuration was determined as follows: Rational Quadratic kernel with a length scale of 1.2, noise level of 1 × 10−4, and a scale mixture parameter of 2.5. Model selection was based on 10-fold cross-validation using R2, RMSE, and MAE as performance metrics. For BLR, although the model has fewer tunable parameters, we optimized the prior variance and noise precision using a Type-II maximum likelihood estimation approach. The prior variance (σ2_prior) was searched within the range of 0.01 to 10.0, and the noise variance (σ2_noise) within 1 × 10−4 to 1.0. The best results were obtained with σ2_prior = 1.0 and σ2_noise = 0.01. These configurations were found to significantly improve the model’s predictive ability and stability. All optimization procedures were carried out using the MATLAB Regression Learner Toolbox and complementary Python scripts utilizing the scikit-learn and GPy libraries. The hyperparameter tuning process was critical in achieving the high prediction accuracy (R2 > 0.99) reported in this study. Moreover, providing this level of detail enhances the transparency, reproducibility, and methodological rigor of the research and ensures that the proposed modeling approach can be confidently applied to similar datasets and applications in AM.
Model performance was evaluated based on R
2 and the visual comparison of predicted versus actual values. The results of the ML models are shown in
Figure 7. For tensile strength, the GPR model achieved an R
2 of 0.9935 (
Figure 7a), while the BLR model followed closely with an R
2 of 0.9912 (
Figure 7b). These results indicate that both models successfully captured the underlying relationships between the input parameters and the resulting tensile strength, with GPR offering slightly higher accuracy. Similarly, for flexural strength, the GPR model yielded an R
2 of 0.9925 (
Figure 7c), and the BLR model produced an R
2 of 0.9902 (
Figure 7d). Again, both models demonstrated excellent predictive capability, with GPR slightly outperforming BLR in terms of precision. The data closely follows the 45-degree line in all plots, indicating strong agreement between actual and predicted values. These findings confirm that ML models, particularly GPR, are highly effective in predicting mechanical properties in FDM processes. They not only complement traditional regression models but also offer added flexibility and generalization for unseen data. The successful implementation of ML in this study highlights its potential for real-time prediction, quality control, and process optimization in next-generation AM workflows.
An error performance analysis was conducted to evaluate the predictive performance and generalization ability of the ML models used in this study. The results of the GPR and BLR models were compared with the traditional BBD-based regression model using standard error metrics, including MSE, MAE, RMSE, MAPE, R
2, and Pearson correlation coefficient (r). The results are presented in
Table 5 for tensile strength and
Table 6 for flexural strength. The GPR algorithm demonstrated superior accuracy in predicting tensile strength, with the lowest MSE (0.7933), MAE (2.7021), and RMSE (0.8908) values among all models (
Table 5). It also achieved the lowest MAPE of 11.135%, indicating minimal deviation from actual values. Additionally, the R
2 value of 0.9935 and correlation coefficient of 0.9967 confirm the excellent predictive capability and strong linear correlation between predicted and actual values. The BLR model also performed well, with slightly higher error values than GPR but still outperforming the BBD regression model. With an R
2 of 0.9912 and MAPE of 12.079%, BLR proves to be a reliable and interpretable ML method for modeling nonlinear relationships in FDM processes. In comparison, although the BBD-based regression model also showed high accuracy (R
2 = 0.9895, MAPE = 13.025%), it lagged slightly behind the ML models, particularly in terms of generalization and error minimization. This highlights the advantage of using ML techniques for capturing the complex and nonlinear interactions between FDM process parameters.
A similar trend was observed in the prediction of flexural strength (
Table 6). The GPR model again yielded the best results with the lowest MSE (1.1525), MAE (3.4219), and RMSE (1.0739) values, along with an MAPE of 12.958%. The model achieved an R
2 of 0.9925 and an r of 0.9968, indicating an almost perfect fit to the experimental data. The BLR model followed closely, with an R
2 of 0.9902 and MAPE of 13.692%, confirming its effectiveness in modeling flexural behavior. While the BBD regression model also performed adequately (R
2 = 0.9885, MAPE = 14.102%), its higher error values suggest that it may not capture all nonlinearities and parameter interactions as effectively as the ML models.
3.7. Discussion
The findings of this study demonstrate that MT, IP, and PD have a substantial and statistically significant influence on the mechanical performance of FDM-printed polymer composite parts. The experimental results, supported by ML-based predictive models, especially those using GPR, confirm that these three parameters play a dominant role in determining tensile and flexural strength. The consistency between experimental and predicted values indicates that the selected factors and their interactions are sufficient to capture the primary process–structure–property relationships within the defined experimental scope. Nevertheless, it is important to recognize the limitations and boundary conditions of the study. All experiments were conducted using a single FDM printer under controlled laboratory conditions with a fixed set of process parameters—specifically, constant layer thickness, nozzle temperature, and printing speed. These parameters were intentionally held constant to isolate the effects of the selected variables. The conclusions drawn from this work are most applicable to settings that closely resemble the conditions used in the study. Variations in printer hardware, filament suppliers, ambient environmental conditions such as temperature and humidity, or adjustments in fixed process parameters may lead to different mechanical outcomes.
Although the present study focused on three key printing parameters—MT, IP, and PD—it is important to acknowledge that other untested parameters may also significantly influence the mechanical properties of FDM-printed parts. Notably, layer thickness and nozzle temperature are widely recognized as critical variables in AM. Layer thickness affects not only the surface finish but also the degree of interlayer bonding. Thinner layers typically promote better layer adhesion due to increased surface contact and more frequent thermal cycling, which can enhance tensile strength and reduce porosity. Thicker layers may reduce printing time but often result in weaker mechanical performance due to reduced bonding area. Similarly, nozzle temperature directly influences the viscosity and flow behavior of the molten filament. Higher nozzle temperatures can improve polymer chain diffusion and interlayer adhesion, particularly in high-performance materials or fiber-reinforced composites. However, excessively high temperatures may lead to material degradation or dimensional inaccuracies. These parameters were held constant in the current study to isolate the effects of the selected variables. Nevertheless, their potential influence on mechanical performance warrants further investigation. Future studies could adopt a more comprehensive DOE approach to include these and other parameters, enabling a more holistic understanding of process–property relationships in FDM.
While recent literature has explored a wide range of advanced ML algorithms—such as XGBoost, random forests, and deep learning-based approaches like CNN-LSTM—for modeling complex mechanical behaviors in AM, this study deliberately focused on two regression models: BLR and GPR. These algorithms were selected based on their suitability for small-to-medium-sized experimental datasets and their ability to provide interpretable predictions with quantified uncertainty. GPR is well-suited for capturing nonlinear relationships in sparse datasets, while BLR offers a probabilistic linear modeling framework that aligns well with the structured nature of the experimental design. Unlike black-box models such as neural networks, these approaches offer greater transparency, which is essential when interpreting the influence of process parameters on mechanical properties. Although we acknowledge the potential of alternative models, our aim was not to conduct an exhaustive benchmarking study but rather to demonstrate the feasibility and effectiveness of integrating ML into a statistically designed FDM optimization framework. Moreover, the study already includes a comparative analysis between two distinct ML models (BLR and GPR) and a classical RSM, which we believe provides a sufficient baseline for evaluating prediction performance. Expanding the model set further was considered beyond the intended scope of this work.
While this approach enhances internal validity, it also limits the generalizability of the findings. For instance, differences in filament quality across manufacturers or fluctuations in environmental conditions during printing could influence interlayer adhesion or dimensional stability, thereby affecting mechanical behavior. Furthermore, hardware-specific characteristics such as extruder design or calibration accuracy may introduce additional variability that was not captured in this study. Building on the current results, future research could extend the parameter space by including additional process variables such as layer thickness, print speed, or nozzle diameter. Similarly, validating the findings across different FDM machines, material suppliers, and environmental conditions would provide further insight into the robustness and transferability of the models. Despite these limitations, the present study offers a focused and well-controlled framework for understanding the mechanical behavior of multi-material and fiber-reinforced structures produced via FDM. The integration of experimental design with ML enables efficient and accurate prediction of mechanical properties, and the methodology presented here can serve as a foundation for broader applications in engineering fields where lightweight, functional components are needed.
Beyond their predictive performance, both GPR and BLR offer the important advantage of providing uncertainty quantification, which is particularly valuable in engineering contexts where safety, reliability, and risk are critical concerns. Unlike traditional regression techniques that yield only point estimates, these Bayesian approaches generate probabilistic outputs, allowing for a more comprehensive interpretation of model predictions. In the case of GPR, the model inherently produces a predictive meaning along with a variance for each prediction, which can be interpreted as a confidence interval. Although no visual uncertainty plots are presented in this study, numerical analysis of the predicted variances indicates that uncertainty remains low across most of the input space, particularly where training data density is high. As expected, slightly increased uncertainty was observed near the edges of parameter space, where extrapolation occurs. This behavior reflects the model’s ability to express lower confidence in less-informed regions, making it a powerful tool for risk-aware decision-making. Similarly, BLR also yields posterior distributions over the predicted outputs by integrating prior assumptions with observed data. The predictive distribution of BLR includes both model uncertainty and noise uncertainty. During testing, the posterior variances computed by the BLR model remained relatively low across all predictions, suggesting that the model was both confident and stable in its estimations. While the uncertainty quantification in BLR is generally less expressive than in GPR—owing to its linear assumptions—it still provides valuable insight into prediction reliability, especially in applications where interpretability and computational simplicity are desired. The ability of both models to provide reliable uncertainty estimates adds an important layer of interpretability and trust to the results. These quantifications can be further leveraged in future studies for robust optimization, reliability-based design, or safety-critical applications in AM processes.
Although GPR has demonstrated strong predictive capabilities in modeling complex, nonlinear relationships in AM, its practical implementation in real-time AM systems presents several challenges. One of the primary limitations is its high computational complexity, which scales cubically with the size of the training dataset (O(n3)). This makes GPR computationally expensive and less suitable for real-time applications, especially in industrial environments where large volumes of sensor data are continuously generated. Additionally, GPR requires the inversion of large covariance matrices, leading to high memory usage and slower processing times, particularly on embedded systems or edge devices commonly used in smart manufacturing platforms. Furthermore, standard GPR models are not inherently designed for online or incremental learning, meaning that even minor updates to the dataset may require complete model retraining, posing a bottleneck for adaptive or self-correcting AM systems. Future research could explore the use of sparse GPR approximations, which reduce the model’s complexity by using a subset of the training data, to overcome these limitations. Online GPR algorithms may also offer real-time adaptability by updating the model incrementally as new data becomes available. Moreover, hybrid strategies that combine GPR with faster surrogate models or integrate GPR into cloud-based or parallel computing architectures could allow for real-time feedback without compromising computational efficiency. For successful industrial adoption, a practical roadmap would involve optimizing kernel functions for specific AM processes, developing modular and lightweight software implementations compatible with existing machine controllers, and validating model performance under real-time operating conditions through sensor-integrated experimental setups. These steps would facilitate the transition of GPR from research to production environments, enabling more intelligent and adaptive AM workflows.