1 INTRODUCTION
Concrete 3D printing (C3DP) has developed rapidly in recent years as an effective automation solution for the construction industry, enabling the direct fabrication of complex concrete components from digital models [1]. This technology significantly shortens construction time, reduces the need for formwork, and improves material efficiency [2]. At present, C3DP has been widely applied in residential construction, temporary and emergency shelters, as well as free-form architectural components [3]. Large-scale concrete 3D printing systems can generally be classified into three main configurations: robotic arm–based systems, crane- or cable-driven systems, and gantry-type systems. While robotic arm systems offer high flexibility, they are often limited in terms of workspace size and structural stiffness, whereas cable-based systems face challenges in achieving high printing accuracy and operational stability. In contrast, gantry-type configurations are characterized by high structural stiffness, good positioning accuracy, and scalable working envelopes, and they can be deployed for both indoor and outdoor printing applications [4]. Owing to these advantages, gantry-based concrete 3D printers are frequently adopted for large-scale printing applications [5,6], which in turn highlights the necessity of optimizing the gantry frame design to simultaneously satisfy requirements related to structural strength, stiffness, and overall operational performance [7,8].
Among the key components, the mechanical frame structure of a concrete 3D printer plays a critical role, as it directly influences structural stiffness, printing accuracy, and operational speed. However, designing a printer frame that is simultaneously lightweight, durable, and cost-effective remains a significant challenge, particularly under the pressure of shortened product development cycles. At present, most machine frame designs still rely heavily on engineering experience combined with conventional numerical simulation tools, such as finite element analysis (FEA). Two main design optimization approaches are commonly adopted. In the first approach, a factorial design is constructed to determine a limited number of design configurations to be evaluated. FEA is then performed for the selected parameter sets, followed by the development of surrogate models, such as regression model [9], response surface models (RSM) [10], or Kriging surrogate model [11], to approximate performance criteria based on simulation data. Subsequently, optimization is carried out using the established surrogate models. Although this approach is relatively straightforward and requires a limited number of design evaluations, its major drawback lies in the limited accuracy of the surrogate models, which may prevent the obtained solutions from being truly optimal. An alternative approach involves the direct integration of optimization algorithms with FEA software. For instance, Du et al. [12] proposed a design methodology for metro underframe structures based on a topology–size–shape co-optimization framework. In this approach, the optimization process is conducted within commercial FEA software (e.g., OptiStruct), where objective functions and constraints are evaluated using embedded finite element (FE) solvers in conjunction with gradient-based sensitivity analysis. While this strategy ensures high accuracy and strong physical consistency, it relies heavily on repeated high-fidelity simulations, leading to substantial computational cost [13]. Consequently, it becomes inefficient for complex optimization problems characterized by high-dimensional design spaces, multiple constraints, and competing performance objectives.
To reduce computational costs, many researchers have introduced artificial neural networks (ANNs) in mechanical engineering to model and predict the structural behavior of mechanical systems. ANNs have been demonstrated to be effective surrogate modeling techniques for approximating complex nonlinear relationships between design parameters and structural responses, particularly with respect to mechanical deformation, stress distribution, and modal characteristics. Numerous studies have successfully applied ANN-based models to a wide range of structural engineering problems. For example, Tran et al. proposed a practical ANN-based approach for estimating the punching shear strength of two-way reinforced concrete slabs [14]. Vu et al. [15] employed ANN models to predict the ultimate axial compressive capacity of concentrically loaded concrete-filled double-skin steel tube columns. In the context of stability and dynamic analysis, Papazafeiropoulos et al. [16] utilized deep learning techniques to determine buckling coefficients of stiffened plate girders under pure bending, and Wu et al. [17] developed a deep convolutional neural network to estimate structural dynamic responses. In addition, ANN-based and machine learning approaches have been applied to the modeling of composite structures, such as soft fiber-reinforced bending actuators [18], concrete-filled rectangular steel tube columns [19], and adhesively bonded joints with viscoelastic layers [20].
Building upon their strong predictive capability, ANN models have also been widely employed as surrogate models in design optimization problems. This approach effectively addresses two critical challenges: improving model accuracy while significantly reducing computational cost. By replacing repeated high-fidelity numerical simulations with accurate surrogate models, ANN-based optimization frameworks enable efficient exploration of complex design spaces while maintaining acceptable prediction accuracy. Consequently, the integration of ANN with metaheuristic optimization algorithms has gained increasing attention in recent years. Several studies have reported successful applications of hybrid ANN-based optimization frameworks. Jiang and Gao [21] proposed an optimization program for rail profile design based on a coupled ANN-genetic algorithm (GA) approach. Liu et al. [22] performed minimum-weight optimization of laminated composite structures using ANN-GA surrogate models. Zhang [23] presented an integrated ANN-particle swarm optimization (PSO)–FEM framework for the optimal design of planar irregular reinforced concrete structures, while Liu et al. [24] developed a hybrid GA for truss optimization based on deep neural networks. In addition, ANN-assisted optimization approaches have been successfully applied to practical mechanical systems, including composite running blade prosthetics [25] and rubber engine mounts [26].
Despite these advances, the application of ANN beyond predictive modelling, specifically for the design and optimization of complex real-world mechanical structures, remains relatively limited. Most existing studies focus either on purely predictive modelling [13-20] or on the optimization of structural components with design parameters defined in a continuous domain [21-26]. As a result, the optimized dimensional parameters may not comply with actual manufacturing constraints and must be rounded to the nearest available standard sizes. This adjustment reduces the effectiveness of the optimization results. A review of the literature reveals that the integration of ANN with optimization algorithms, such as GA or PSO, to form a surrogate-based optimization loop is still an emerging area, particularly in the design of large-scale machinery such as 3D concrete printers, large Computer Numerical Control (CNC) machines, or construction robots. These systems involve multiparameter with nonlinear constraints, making them ideal candidates for intelligent optimization approaches, yet real-world applications remain scarce. This gap presents an opportunity to advance the field by developing hybrid ANN-optimization frameworks tailored for the design of specific machine structures. Such frameworks could enable efficient exploration of large design spaces with reduced computational costs, while still accounting for the physical fidelity of real systems.
To address this gap, the present study proposes an integrated ANN-GA approach for optimizing the frame structure of a large-scale concrete 3D printer, representing a real-world complex mechanical system with multiple design parameters and constraints. A surrogate model based on ANN is constructed using simulation data generated from FEA via Ansys parametric design language (APDL) scripting, and a GA is employed to perform the optimization under multiple structural constraints. The proposed framework also considers design variables in a discrete domain consistent with standard steel sections, enabling practical manufacturability. The effectiveness of the proposed approach is evaluated through a systematic comparison with alternative optimization strategies.
The main contributions of this study can be summarized as follows:
1. A discrete design space formulation aligned with standard steel sections, ensuring direct manufacturability of optimized solutions;
2. Application to a real large-scale gantry-type 3D concrete printer frame with coupled static and dynamic constraints;
3. Development of an integrated dual optimization framework combining direct FE-based and ANN-based surrogate approaches, with systematic comparison and verification;
4. A clear quantitative demonstration of computational efficiency, showing a reduction in optimization time from approximately 38.5 hours to about 200 seconds while maintaining acceptable accuracy.
The remainder of this paper is organized as follows. Section 2 presents the materials and methods employed in this study. Section 3 presents the results and discussion. Finally, Section 4 summarizes the main conclusions of the study.
2 MATERIALS AND METHODS
2.1 Large-scale 3D Concrete Printer Frame
The printer frame is designed based on a space frame structure system [27]. A preliminary design of the printer is illustrated in Fig. 1. The Y-axis and Z-axis frames are assembled from steel box beams with standard square cross-sectional dimensions. The printer legs consist of a sliding rail system, with the rails directly fixed to the construction foundation and fabricated from I-beam steel structures.

Fig. 1. An experience-based design of a large-scale 3D concrete printer; a) 3D model of the printer; b) 3D model of the steel box beam; and c) cross-sectional view of the box beam
Some fundamental technical requirements of the large-scale 3D concrete printer are defined as follows [27]:
- Maximum printable structure dimensions: 6000 mm × 4000 mm × 3500 mm.
- Printhead travel speed V ranging from 0 m/min to 20 m/min.
- Permissible positioning error of the printhead: ±5 mm in the X and Y directions, and ±2 mm in the Z direction.
2.2 Structural Modeling
2.2.1 Governing Equations
The printer frame is analyzed using the finite element method (FEM). The static equilibrium equations for the structure are described by Eq. (1). From these, the nodal displacements u are calculated by solving the system of static equilibrium equations [28], as shown in Eq. (2):
\tag{1}$$
\tag{2}$$
where K is the global element stiffness matrix, u is the nodal displacement vector, and F is the external force vector.
The natural mode shapes and frequencies of the printer frame during free vibration are determined through modal analysis [29], based on Eq. (3):
\tag{3}$$
where, M is mass matrix, \(\ddot{\mathbf{u}}=\frac{d^2\mathbf{u}}{dt^2}\) and is the 2nd time derivative of the nodal displacement vector u.
To solve Eq. (3), it is assumed that the system undergoes harmonic vibration with a solution of the form Eq. (4):
\tag{4}$$
Substituting this expression into the equation of motion yields an eigenvalue or characteristic value problem, as expressed in Eq. (5):
\tag{5}$$
where, ω is the natural angular frequency and ϕ represents vector of the shape of the system (mode shape). Solving Eq. (5) allows the determination of the values of ωi (from which the natural frequencies fi = ωi / (2π) can be derived) and their corresponding mode shapes ϕi.
In this study, the global stiffness matrix K and mass matrix M are constructed from the finite element model of the printer frame (see the FE model description). The geometric design parameters of the frame, including cX, cY, a1, t1, a2, t2, a3, t3, a4, t4 (Fig. 2), directly influence the stiffness matrix K, thereby governing the nodal displacements u and, in particular, the printhead displacement, as defined in Eq. (2).
These design parameters also determine the mass matrix M, which subsequently governs the natural frequencies fi of the structure through the eigenvalue problem given in Eq. (5).
2.2.2 FE Model
The FE model of the printer frame was developed using Ansys APDL® software. The parameters of the preliminary design configuration are presented in Table 1. A total of ten dimensional parameters were parameterized to enable automated calculations across different sets of parameters. In particular, cX and cY represent the width of the Y-axis frame in the X and Y directions, respectively; a1×a1×t1 denotes the cross-sectional dimensions (vertical × horizontal × thickness) of the square steel box beam in the Y-axis frame; a2×a2×t2 denotes the cross-sectional dimensions of the square steel box beam in the Z-axis frame; a3×a3×t3 denotes the cross-sectional dimensions of the diagonal reinforcement members used in both the Y-axis and Z-axis frames; a4×a4×t4 denotes the cross-sectional dimensions of the steel box beam at the base of the Y-axis frame.

Fig. 2. FE model of printer frame
Table 1. The experience-based design parameters of the printer frame [mm]
| cX | cY | a1×a1×t1 | a2×a2×t2 | a3×a3×t3 | a4×a4×t4 |
|---|---|---|---|---|---|
| 460 | 460 | 60×60×3 | 50×50×2.5 | 25×25×1 | 60×60×3 |
The design problem is inherently discrete because the key parameters are selected from a finite set of commercially available profiles and standard manufacturing dimensions. Table 2 provides a detailed description of the feasible value sets for parameters cX, cY, as well as ai and ti.
The steel box beams of the printer frame are modeled using BEAM188 elements. The mass of the print head and the X-axis motor is m0 = mdi + mrx = 250 kg, and is represented by a concentrated mass element (MASS21). The total mass of the driving and guiding rails attached to the Y-axis frame is msy = 140 kg, which is assumed to be evenly distributed among the nodes of the Y-axis frame. The total mass of the driving and guiding rails attached to the Z-axis frame is msz = 100 kg, and is similarly distributed among the nodes of the Z-axis frame. The mass of each Y-axis motor is mry = 25 kg, while the mass of each Z-axis motor is mrz = 15 kg. These motors are modeled using concentrated mass elements (MASS21).
To simplify the analysis, the printer frame is assumed to be stationary (the base is fully fixed), and the dynamic loads acting on the frame during motion are converted into equivalent inertial forces. These inertial forces are calculated based on the maximum acceleration experienced during operation. According to the design requirements, the maximum horizontal speed of the print head is Vmax = 20 m/min = 0.333 m/s. Assuming the print head reaches this velocity within Δt = 0.1 s, the maximum acceleration is estimated to be amax = 3.33 m/s2 (in the X and Y directions).
Table 2. Parameter description of the frame of a large-scale 3D concrete printer
| Geometry parameters | The design parameter set [m] |
|---|---|
| cx, cy | {0.30, 0.32, 0.34, …, 0.54, 0.56, 0.58, 0.60} |
| a1, a2, a3, a4 | {0.03, 0.038, 0.04, 0.05, 0.06, 0.075} |
| t1, t2, t3, t4 | {0.001, 0.0011, 0.0012, 0.0014, 0.0016, 0.0018, 0.002, 0.0025, 0.0028, 0.003, 0.0032, 0.0035} |
The configuration of the frame under investigation corresponds to the structural state that may cause the greatest positioning error of the print head (i.e., when the Z-axis frame is at its highest vertical position and the print head is located at the center of the Z-axis frame, which may result in the largest deflection).
To reduce computation time, automatic analysis modules were developed using Ansys APDL scripting language, including modules for calculating the displacements of the print head in the X, Y, and Z directions, as well as the natural frequencies of the system [27]. These structural characteristics can therefore be evaluated automatically.
2.3 ANN Model Development
To construct the dataset, a total of 5000 samples were generated using the Ansys APDL-based FE model. Each sample corresponds to a unique combination of input design variables selected within their predefined bounds. The design points were generated using a Monte Carlo-based sampling strategy over the design space. This approach ensures a broad and representative coverage of the design domain while avoiding the combinatorial explosion associated with full factorial sampling.
The dataset generation process was implemented through an automated MATLAB–Ansys APDL script using an iterative loop, where each design variable was discretized within its lower and upper bounds. At each iteration, a set of input parameters was randomly sampled from the corresponding discrete value sets, and the associated structural responses were evaluated using the FE model. This procedure enables efficient exploration of the discrete design space while maintaining a manageable dataset size.
The complete dataset was randomly divided into three subsets, including 70 % for training, 15 % for validation, and 15 % for testing. The training set was used to update the network weights, the validation set was employed to monitor the training process and prevent overfitting, and the test set was used to evaluate the generalization capability of the trained model.
Prior to training, all input and output data were normalized using min–max scaling to eliminate discrepancies in magnitude and ensure stable convergence. Based on the normalized dataset, an ANN surrogate model was developed to efficiently approximate the structural responses required for optimization. Multilayer feed-forward neural networks (MLFFNNs) are widely used in nonlinear regression, classification, and system modeling due to their universal approximation capability [30,31]. In this section, the authors employ a MLFFNN to approximate the response of a 3D printer frame structure, including displacement values (uX, uY, uZ) and natural frequency (f1), as a substitute for the Ansys APDL computation module described in Section 2.2. The network consists of an input layer with 10 parameter variables cX, cY, a1, a2, a3, a4, t1, t2, t3, t4, two hidden layers, and output layer, where information flows unidirectionally from input to output without forming cycles. Each layer performs an affine transformation followed by a nonlinear activation function, enabling the network to learn complex nonlinear mappings between inputs and outputs.

Fig. 3. Architecture of the multilayer feed-forward neural network (MLFFNN)
The MLFFNN was initialized, and its architecture is illustrated in Fig. 3. There are some transfer functions that could be applied, such as log-sigmoid transfer function (logsig), linear transfer function (purelin), hyperbolic tangent sigmoid transfer function (tansig), and hard limit transfer function (hardlim). In this study, the hyperbolic tangent sigmoid function was employed as the activation function for the two hidden layers, while a linear function was used in the output layer. The tansig function was selected due to its strong capability in capturing complex nonlinear relationships and its output range of [−1 1], which is well suited for normalized input data and contributes to stable and efficient training. In contrast, the linear activation function in the output layer is appropriate for modeling continuous target variables, such as displacement components and natural frequency, enabling the network to produce unbounded outputs and improving regression accuracy [9,32].
The optimal number of neurons in the hidden layers was determined through a systematic trial-and-error procedure based on the evaluation of the mean squared error (MSE) on the validation dataset. The number of neurons was gradually varied within a reasonable range to balance model accuracy and generalization capability, while avoiding overfitting. Based on this analysis, the network architecture with 32 neurons in the first hidden layer and 10 neurons in the second hidden layer was selected.
2.4 Optimization Framework
2.4.1 Optimization problem formulation
The design space consists of 10 discrete design variables corresponding to commercially available structural profiles and standard geometric dimensions. To enable efficient genetic operations while preserving the discrete nature of the problem, each design variable is represented by an integer index mapped to a predefined discrete set. Specifically, for the ith design variable, an integer gene gi ∈ {1, 2, …, mi} is assigned, where mi denotes the number of admissible discrete options, and the actual design value is obtained through an inverse mapping function xi = f –1(gi). Consequently, the optimization is performed in a 10-dimensional integer-coded search space, while the physical design remains strictly discrete. For each individual, the decoded design variables are used to construct the structural model, from which the maximum displacement, and the first natural frequency are evaluated by the computational Ansys-APDL model (or surrogate ANN model).
The optimization objective is to minimize the total mass of the mechanical frame of the 3D concrete printer, denoted as M in Eq. (6):
M = \rho \Bigg[
&\sum_{i=1}^{m}4t_1(a_1-t_1)L_i
+\sum_{j=1}^{n}4t_2(a_2-t_2)L_j \\
&+\sum_{k=1}^{p}4t_3(a_3-t_3)L_k
+\sum_{l=1}^{q}4t_4(a_4-t_4)L_l
\Bigg]
\rightarrow \min,
\end{aligned}
\tag{6}$$
where ρ is the material density of the steel frame; m, n, p and q represent the number of structural members corresponding to different cross-section types; and Li, Lj, Lk, Ll denote the lengths of members with cross-sections a1×a1×t1, a2×a2×t2, a3×a3×t3 and a4×a4×t4, respectively.
The constraints require that the displacements in the X, Y, and Z directions (uX, uY, uZ) remain below specified allowable limits, while the first natural frequency ( f1) must exceed a prescribed minimum value, as defined in Eq. (7):
\begin{aligned}
u_X &= \left|g_X(c_X,c_Y,a_1,t_1,a_2,t_2,a_3,t_3,a_4,t_4)\right|
\le 2\,\text{(mm)};\\
u_Y &= \left|g_Y(c_X,c_Y,a_1,t_1,a_2,t_2,a_3,t_3,a_4,t_4)\right|
\le 2\,\text{(mm)};\\
u_Z &= \left|g_Z(c_X,c_Y,a_1,t_1,a_2,t_2,a_3,t_3,a_4,t_4)\right|
\le 1\,\text{(mm)};\\
f_1 &= g_f(c_X,c_Y,a_1,t_1,a_2,t_2,a_3,t_3,a_4,t_4)
\ge 6\,\text{(Hz)};
\end{aligned}
\right.
\tag{7}$$
where cx, cy, a1, t1, a2, t2, a3, t3, a4, t4 denote the geometric design parameters of the printer frame, as defined in Section 2.2 and illustrated in Fig. 2.
Constraint handling is implemented using an absolute penalty function approach, whereby violations of the displacement and natural frequency constraints are explicitly incorporated into the fitness function. Standard genetic operators, including selection, integer-based crossover, and mutation, are applied, with all offspring genes confined to their admissible index bounds. An elitism strategy is adopted to retain the best solutions across generations. This discrete index-mapping GA framework enables robust exploration of the combinatorial design space while ensuring that all candidate solutions correspond to manufacturable and structurally feasible configurations.
2.4.2 GA-Based Optimization Framework
A GA-based optimization framework was subsequently established to identify optimal design solutions under multiple constraints. In the domain of optimization, nature-inspired algorithms are frequently adopted owing to their versatility and robust performance across diverse problem classes. These algorithms can be broadly categorized into bio-inspired and physico-chemical-inspired approaches. Representative bio-inspired algorithms include the Cuckoo Search algorithm, the particle swarm optimization (PSO) algorithm [23], and the GA [33], among others. Physico-chemical-inspired algorithms encompass methods such as the harmony search algorithm and the simulated annealing (SA) algorithm [34]. In the present study, a discrete genetic algorithm (DGA) is adopted to minimize the total structural mass of a large-scale 3D concrete printer frame while satisfying both static and dynamic performance constraints. The DGA is selected due to its proven capability in handling discrete, combinatorial, and constrained optimization problems.
Two optimization approaches are considered for the structural design of the large-scale 3D concrete printer frame. The optimization is performed in both continuous and discrete design domains, with the discrete formulation ensuring direct manufacturability using commercially available steel sections.
The first approach follows a conventional finite element-based optimization strategy, in which the DGA is directly coupled with the computational model developed in Ansys APDL (Section 2.2). In this framework, the DGA iteratively updates the design variables, while each candidate solution is evaluated through finite element simulations. The structural responses obtained from the FE model are subsequently used to assess the objective function and design constraints, enabling the search for the optimal frame configuration.
The second approach employs a surrogate-based optimization strategy, in which the computationally expensive Ansys APDL model is replaced by the validated ANN surrogate model developed in Section 2.3. The ANN provides rapid predictions of structural responses, including printhead displacements and the first natural frequency, with high accuracy. Consequently, candidate solutions generated by the DGA can be evaluated efficiently without repeatedly performing FE simulations. The DGA then iteratively updates the design variables based on the ANN predictions to identify the optimal design. This approach significantly reduces computational cost while maintaining satisfactory optimization accuracy.
The optimization procedure based on the DGA is illustrated in Fig. 4. The process begins with the definition of the discrete design space, where 10 geometric parameters of the printer frame are encoded as integer indices within their feasible ranges. Next, the fitness of each individual is assessed according to its structural performance. The elitism strategy is applied to preserve the best-performing individuals, ensuring that superior solutions are carried over to the next generation. The selection operator (e.g., roulette wheel or tournament method) identifies parent chromosomes, which are then combined through crossover and slightly modified through mutation to produce a new population of candidate designs. This iterative evolutionary cycle – evaluation, selection, crossover, and mutation – continues until a termination criterion is met, such as reaching the maximum number of generations or achieving convergence of the objective function. The final output is the optimal design parameter set, representing the best balance between minimum structural displacement and sufficient stiffness, while satisfying the predefined constraint on natural frequency.

Fig. 4. Flowchart of the GA-based discrete optimization procedure for the 3D printer frame design
3 RESULTS AND DISCUSSION
3.1 Validation of the ANN Surrogate Model
ANN performance evaluation
Figure 5 presents the performance evaluation of the developed ANN model across the training, validation, and testing datasets. The regression plots indicate a very strong correlation between the predicted and target values, with correlation coefficients (R) exceeding 0.9997 for all subsets. This demonstrates the high predictive capability of the proposed model.
The distribution of prediction errors, as illustrated by the error histograms (Fig. 5c), shows that most errors are concentrated around zero with a relatively small dispersion, indicating low bias and good consistency of the model. In addition, the training process exhibits stable convergence behavior, with the MSE reaching a minimum value of 2.20×10⁻⁵ at epoch 216, suggesting effective learning of the underlying nonlinear relationships.
To quantitatively assess the model performance, several statistical metrics were employed, including the MSE, root mean squared error (RMSE), mean absolute error (MAE) and correlation coefficient R, as summarized in Table 3. These metrics were computed for the independent test dataset to ensure a comprehensive evaluation.
Table 3. Performance evaluation of the ANN model using statistical error metrics for the independent test dataset
| Error metric | MSE | RMSE | MAE | R |
|---|---|---|---|---|
| Independent test dataset | 1.053 × 10-4 | 1.026 × 10-2 | 3.42 × 10-3 | 0.9998 |
3.1.1 Investigation of the Computational Results
In this section, the effects of the input design parameters on the displacement responses and first natural frequency of the print head are investigated. Furthermore, to rigorously validate the predictive capability of the trained ANN, the ANN-based predictions are quantitatively compared with the corresponding results obtained from the high-fidelity Ansys APDL numerical model. This section defines the absolute errors and relative errors between the predictive performance and simulation performance (i.e., Ansys APDL simulated data) to compare the performance of ANN. The calculation formula for absolute error Eabs and relative error Erel is:
=
\left|y_{\mathrm{APDL}}-y_{\mathrm{ANN}}\right|,
\tag{8}$$
=
\frac{E_{\mathrm{abs}}}{y_{\mathrm{APDL}}},
\tag{9}$$
where, yAPDL is the output response of Ansys APDL module, yANN is the predicted output of ANN.
The comparison between the predicted displacements obtained from the ANN model and those computed by the finite element analysis in Ansys APDL demonstrates an excellent agreement across all components (uX, uY, uZ). As shown in Fig. 6a, an increase in the geometric variable cx leads to a noticeable reduction in uX and uZ, indicating an improvement in the global stiffness of the frame along the X-direction. The displacement component uY remains nearly constant, implying that the change in cx has limited influence on lateral stiffness along the Y-axis.
The relative error between ANN predictions and APDL results (Fig. 6b) remains generally below 3 %, with the smallest discrepancies observed in the uZ component (< 1 %). A slight increase in the error of uX is observed for cx > 450 mm, which may be attributed to nonlinear behavior or sparse sampling in the training dataset within that range. The overall results confirm that the ANN accurately captures the displacement responses.

Fig. 5. The training performance evaluation of MLFFNN; a) regression analysis; b) mean squared error evolution, and c) error distribution histogram

Fig. 6. Comparison of ANN-predicted and Ansys APDL-simulated displacements and their relative errors versus cX ; a) displacement; b) relative error
Figure 7a presents the variation of the first natural frequency f1 with respect to cx. Both ANN and APDL values exhibit similar trends, where f1 gradually increases as cx rises, reflecting enhanced global rigidity. The relative error (Fig. 7b) is below 0.6 %, confirming the high accuracy of ANN-based dynamic response prediction.

Fig. 7. Comparison of ANN-predicted and Ansys APDL-simulated displacements and their relative errors versus cx; a) displacement; b) relative error
The influence of parameter cy is shown in Fig. 8 and 9. The ANN predictions exhibit a strong correlation with APDL results for all displacement components. The dominant variation occurs in uY, which decreases markedly with increasing cY, signifying enhanced stiffness along the Y-direction. Meanwhile, uX and uZ remain nearly stable, as expected for this type of geometric modification.

Fig. 8. Comparison of ANN-predicted and Ansys APDL-simulated displacements and their relative errors versus cY ; a) displacement; b) relative error

Fig. 9. Comparison of ANN-predicted and Ansys APDL-simulated first natural frequency and the corresponding relative error versus cY; a) displacement; b) relative error
The relative error between ANN and APDL values remains within 3 %, with a minor increase in uY error at higher cY values. Such deviation can be explained by the stronger stiffness gradient and nonlinearities at larger dimensions. The corresponding natural frequency f1 increases monotonically with cY, confirming that the structural stiffness is markedly affected by this parameter. The ANN model accurately follows the APDL trend, and the maximum relative error remains below 1.2 %, demonstrating reliable generalization in dynamic analysis.
Figure 10 illustrates the displacement and error distributions corresponding to changes in a1. With increasing a1, all displacement components (uX, uY, uZ) decrease consistently, highlighting an improvement in vertical member stiffness. The ANN model replicates the APDL results with excellent accuracy, exhibiting maximum errors of less than 3 % across all components and below 1 % for uZ. These findings demonstrate that the ANN effectively captures the parametric relationships governing both the static and dynamic behaviors of the structure.

Fig. 10. Comparison of ANN-predicted and Ansys APDL-simulated displacements and their relative errors versus a1; a) displacement; b) relative error
Figure 11a demonstrates a strong agreement between the ANN-based predictions and the reference APDL results for the first natural frequency f1 as a function of a1. The first natural frequency f1 increases monotonically with a1, indicating that enlarging a1 enhances the global stiffness of the frame and consequently raises its fundamental vibration frequency. The ANN curve almost completely overlaps the APDL curve across the investigated range, confirming the high fidelity of the surrogate model in capturing the dynamic trend. The error plot in Fig. 11b further verifies this accuracy. The relative error remains consistently low (below approximately 0.7 %) and decreases as a1 increases, reaching nearly zero at larger values of a1. This behavior suggests that the ANN model provides a highly reliable approximation of the APDL-based frequency response, with improved prediction stability in the higher a1 region.

Fig. 11. Comparison of ANN-predicted and Ansys APDL-simulated first natural frequency f1 and relative errors versus a1; a) first natural frequency; b) relative error
Figures 12 and 13 illustrate the variation of displacement components, relative errors, and the first natural frequency of the 3D concrete printer frame with respect to the geometric parameter t1. An increase in the geometric parameter t1 leads to a gradual reduction in all displacement components (uX, uY, uZ), indicating improved structural stiffness. Among them, uY exhibits the most pronounced decrease, highlighting the strong influence of t1 on stiffness in the Y-direction. The ANN predictions show excellent agreement with the APDL results over the entire investigated range. The relative errors remain below 3 % for uX and uY, and below 1 % for uZ, confirming the reliability of the surrogate model. The first natural frequency f1 increases monotonically with increasing t1, reflecting enhanced global rigidity of the frame. The ANN accurately reproduces the APDL results, with a maximum relative error of approximately 0.35 %. These results demonstrate that the ANN model can efficiently and accurately predict both static and dynamic responses associated with variations in t1.

Fig. 12. Comparison of ANN-predicted and APDL-computed displacement components versus parameter t1; a) displacement; b) relative error

Fig. 13. Comparison of ANN-predicted and Ansys APDL-simulated first natural frequency and the corresponding relative error versus t1; a) first natural frequency; b) relative error
Within the limited scope of this paper, the authors do not present a comprehensive investigation of the effects of the remaining input variables on the static and dynamic characteristics. However, the obtained results are highly reliable and exhibit small errors, similar to those observed for the variables cX, cY, a1, t1. Overall, the ANN model trained using Matlab–Ansys APDL datasets exhibits high accuracy and stability in predicting both displacement and natural frequency responses of the 3D concrete printer frame. The relative error remains within 4 % for displacements and below 1 % for natural frequency, confirming the model’s robustness. These results validate the ANN’s ability to serve as a computationally efficient surrogate model, capable of replacing conventional finite element simulations in parametric optimization and design sensitivity analyses of large-scale additive manufacturing systems.
3.2 Optimization Results
3.2.1 Direct FE-based Optimization
The optimization results obtained using the DGA – Ansys APDL framework demonstrate reliable for the 10-variable discrete design problem (Fig. 14). The best fitness value decreases steadily from the initial level of approximately 900 to a final value of Mbest ≈ 627 kg after 224 generations. The close agreement between the best and best-so-far curves indicates stable elitism and consistent improvement throughout the evolutionary process. The mean fitness evolution remains higher than the best fitness and exhibits pronounced oscillations, reflecting the strong nonlinearity of the structural response evaluated directly through finite element analysis. This behavior is typical for DGA implementations relying on high-fidelity solvers, where evaluation noise and constraint sensitivity are more pronounced. The population diversity remains relatively high and stable throughout the optimization process, indicating that the GA maintains sufficient exploration capability and avoids premature convergence. The gene evolution map shows gradual stabilization of several variables, while others continue to fluctuate until the final generations, suggesting complex interactions between discrete design variables and structural performance metrics.

Fig. 14. Convergence characteristics of the discrete GA optimization for frame mass minimization; a) best and best-so-far fitness values, b) mean fitness value, c) population diversity, and d) evolution of the best individual.
Figure 15 illustrates the configuration of the current best individual obtained from the optimization process, where the design variables are represented by integer indices corresponding to feasible configuration options. The results indicate that several variables tend to converge toward lower or boundary values, reflecting the tendency to reduce the frame mass while still satisfying the displacement and natural frequency constraints. In contrast, other variables remain at moderate or higher levels, highlighting their critical role in maintaining structural stiffness and dynamic stability. Overall, the obtained solution demonstrates that the discrete GA-Ansys APDL approach effectively achieves a balanced trade-off between frame mass minimization and structural performance requirements, thereby confirming the efficiency of the proposed optimization framework for the design of large-scale 3D concrete printer frames.

Fig. 15. Integer-coded design variables of the current best individual identified by the discrete GA– Ansys APDL optimization process
Notably, the total optimization time of approximately 38.5 hours (138,479.4 s) highlights the substantial computational cost associated with direct APDL-based finite element evaluations. While the GA-APDL approach provides high-fidelity and physically accurate results, the obtained solution is less optimal in terms of objective value and substantially more time-consuming.
The best solution corresponding to the minimum frame mass, while satisfying the displacement and natural frequency constraints, is represented by the normalized design vector: xbest = [0.6000, 0.5600, 0.0750, 0.0011, 0.0300, 0.0020, 0.0300, 0.0011, 0.0600, 0.0011].
3.2.2 ANN-based Surrogate Optimization
In Figure 16, the optimization results demonstrate that the proposed ANN-GA framework achieves stable and effective convergence for the mass minimization of a 3D concrete printer subject to displacement and first natural frequency constraints in Eq. (8). The best fitness value decreases rapidly during the early generations, from an initial level exceeding 900 to approximately 700 within the first 50 generations, and then gradually improves until reaching an optimal value of Mbest ≈ 600 kg at generation 219. The best and best-so-far curves nearly coincide, indicating that the algorithm has identified a high-quality solution region and successfully preserved elite individuals through the elitism strategy.

Fig. 16. Convergence characteristics of the discrete ANN-GA optimization for frame mass minimization; a) best and best-so-far fitness values, b) mean fitness value, c) population diversity, and d) evolution of the best individual
The mean fitness evolution fluctuates around (6 to 7) × 103, remaining significantly higher than the best fitness value. This behavior is typical for constrained and highly nonlinear optimization problems and indicates that population diversity is intentionally maintained to enhance global exploration. Such behavior confirms that the algorithm does not suffer from premature convergence. The population diversity, quantified by the standard deviation across all genes, exhibits a sharp reduction in the initial generations, followed by a relatively stable level ranging from approximately 3.6 to 4.2. This trend reflects a well-balanced trade-off between exploitation and exploration, which is particularly important for discrete combinatorial design spaces involving multiple variables. The heatmap of the best individual gene evolution reveals that several design variables converge rapidly to their optimal discrete indices, whereas others continue to evolve gradually over subsequent generations. This observation suggests differing sensitivities of the design variables with respect to the objective function and indicates that the final optimal configuration is both stable and physically meaningful.
In terms of computational efficiency, the total optimization time of approximately 200 s for 219 generations with 10 design variables highlights the effectiveness of the surrogate ANN model in notably reducing the computational cost compared to direct finite element evaluations. Overall, the results confirm that the proposed ANN-GA framework provides a robust, efficient, and scalable solution for discrete structural optimization problems involving large-scale 3D printing systems with static and dynamic constraints. The best solution (Fig. 17) corresponding to the minimum frame mass is xbest_ANN = [0.58, 0.58, 0.075, 0.001, 0.06, 0.001, 0.03, 0.001, 0.04, 0.0018].

Fig. 17. Integer-coded design variables of the current best individual identified by the discrete ANN-GA optimization process
The optimal design obtained using the ANN-GA approach was further verified using ANSYS software, as presented in Table 4 and Fig. 18. It can be observed that the discrepancies between the results predicted by the ANN surrogate model and those obtained from the ANSYS finite element simulations are relatively small, with deviations of less than 5 %.
Table 4. Verification of the GA-ANN optimal design using ANSYS®
| Design option | uX | uY | uZ | f1 |
|---|---|---|---|---|
| GA-ANN | 1.4393 mm | 1.9987 mm | 0.9898 mm | 6.7287 Hz |
| APDL based | 1.3718 mm | 1.9963 mm | 0.9927 mm | 6.7152 Hz |
| Relative error | 4.9 % | 1.2 % | 2.9 % | 2.0 % |

Fig. 18. Verification results (uY) of the ANN-GA optimal design in ANSYS®
The performance of the two optimization approaches is systematically compared in terms of both solution quality and computational efficiency.
3.3 Comparison and Discussion
In addition, the authors solved the APDL-GA optimization problem over a continuous design space. The resulting optimum provides a theoretically favorable set of parameters; however, it is difficult to implement in practice, since several optimal dimensions do not comply with the available standard hollow steel sections used in fabrication. The total optimization time was approximately 180,919 s, highlighting the considerable computational cost of directly coupling GA with the finite element model. To improve manufacturability, the optimal continuous solution was subsequently mapped to a feasible design using a nearest-neighbor selection strategy, in which each continuous variable was adjusted to the closest admissible standard-section dimension while preserving proximity to the optimal solution. The final selected parameters are reported in Table 5.
Table 5. Comparison of structural performance and computational efficiency among different optimization approaches
| Design option | Design parameters [cX, cY, a1, t1, a2, t2, a3, t3, a4, t4] |
uX [mm] | uY [mm] | uZ [mm] | f1 [Hz] | M [kg] |
Compare to S–EXP [%] |
Time [s] |
|---|---|---|---|---|---|---|---|---|
| S-EXP (Experience-based selection) |
[0.46, 0.46, 0.06,0.003, 0.05,0.0025, 0.025,0.001, 0.06,0.003] |
1.1 | 1.9 | 0.99 | 7.01 | 974.5 | ||
| APDL-GA (continuous domain) |
[0.5843, 0.5338, 0.0660, 0.0014, 0.0364, 0.0016, 0.0303, 0.0010, 0.0441, 0.0018] |
1.2 | 2.0 | 1.0 | 6.73 | 633.7 | 27.98 | 180919 |
| APDL-GA (continuous domain) – reselected parameter |
[0.58, 0.54, 0.06, 0.0014, 0.038, 0.0016, 0.03, 0.001, 0.0500, 0.0018] |
1.2 | 2.0 | 1.0 | 6.69 | 626.9 | 35.67 | |
| APDL-GA (discrete domain) |
[0.60, 0.56, 0.075, 0.0011, 0.03, 0.002, 0.03, 0.0011, 0.06, 0.0011] |
1.2 | 2.0 | 0.998 | 6.76 | 627.4 | 35.62 | 138479 |
| ANN-GA (discrete domain) |
[0.58, 0.58, 0.075, 0.001, 0.06, 0.001, 0.03, 0.001, 0.04, 0.0018] |
1.4 | 2.0 | 0.992 | 6.72 | 600.2 | 38.4 | ~200 |
Table 5 provides a comprehensive comparison between the experience-based selection (S-EXP) and various optimization strategies, including APDL-GA and ANN-GA approaches under both continuous and discrete design domains. Compared with the baseline S–EXP design (M = 974.5 kg), all optimization methods achieve a significant reduction in structural mass while satisfying displacement and dynamic constraints.
The APDL-GA optimization in the continuous domain reduces the mass by approximately 28 %, whereas the reselected-parameter variant further improves the reduction to about 35.7 %, indicating the sensitivity of the optimization outcome to parameter selection. A comparable mass reduction (35.6 %) is obtained using the APDL-GA approach in the discrete design domain, confirming that discretizing the design variables preserves the overall effectiveness of the optimization process.
Clearly, the ANN-GA method yields the best performance, achieving the maximum mass reduction of 38.4 % while maintaining displacement responses and first natural frequency values close to those obtained by Ansys APDL-based solutions. More importantly, the computational time is dramatically reduced from several tens of hours for GA-APDL to approximately 200 s for the ANN-GA approach. This significant reduction highlights the advantage of the surrogate-based optimization in efficiently exploring the discrete design space while preserving structural performance.
The convergence behavior of the design variables provides important insight into the underlying mechanical mechanisms governing the optimization results. As shown in Table 5, with particular focus on the optimal ANN-GA solution, the global geometric parameters of the frame (cX, cY) tend to increase toward higher values compared to the experience-based design. This trend indicates that enlarging the overall frame dimensions significantly enhances the global bending stiffness, leading to a reduction in printhead displacements (Fig. 6, Fig. 8), which is consistent with classical structural mechanics principles. Similarly, the cross-sectional width of the primary load-bearing members (a1) converges to its upper bound, confirming that increasing section width is an effective strategy for improving structural stiffness (Fig. 10) with a relatively moderate increase in mass. In contrast, the thickness parameters (t1, t2) and the dimensions of secondary bracing members (a3, t3) tend to converge toward lower values. This behavior suggests that these variables have a limited contribution to global stiffness while significantly affecting the overall mass, and are therefore minimized during the optimization process. The parameters associated with the base frame (a4, t4) do not exhibit a clear tendency toward boundary values, indicating their relatively minor influence on both the global bending stiffness and overall mass. In terms of dynamic performance, the first natural frequency (f1) of the optimized designs shows a slight decrease compared to S–EXP solution but remains within the prescribed constraints. This reflects a rational trade-off between dynamic stiffness and mass reduction. These results confirm that the obtained optimal solutions are physically meaningful and governed by the fundamental balance between stiffness enhancement and mass minimization.
These results highlight the practical advantages of the proposed framework. In particular, the discrete design formulation ensures that all optimized solutions are directly manufacturable without post-processing. Furthermore, the ANN-GA approach significantly reduces computational time while maintaining prediction accuracy, making it highly suitable for large-scale engineering applications.
Overall, the results confirm that the integration of ANN surrogate models with GA optimization provides a robust and computationally efficient strategy for high-dimensional structural optimization, particularly for real-world systems involving discrete design constraints.
4 CONCLUSIONS
This study developed an integrated ANN-GA framework for the multi-parameter design optimization of a large-scale concrete 3D printer frame in a discrete design space consistent with practical manufacturing requirements. The proposed framework effectively combines high-fidelity finite element modeling, surrogate-based learning, and intelligent optimization to address the challenges associated with the design of complex large-scale machine structures.
First, a finite element model of the printer frame was established using APDL scripting, enabling automated evaluation of printhead displacements along the X, Y, and Z directions, as well as the natural frequencies of the frame. Based on the FE-generated dataset, an ANN surrogate model was constructed to predict printhead displacements and natural frequencies. With a network architecture of 10–32–10–4, the ANN model achieved high prediction accuracy, with deviations of less than 4 % compared to the FE results. Subsequently, a mathematical optimization model of the printer frame was formulated with ten design variables and four constraints, targeting minimum structural weight. Two optimization strategies were investigated: direct GA-based optimization coupled with APDL simulations and surrogate-based optimization using the ANN model. The developed GA optimization framework enables the identification of optimal design parameters in both continuous and discrete design domains. All optimal solutions were subsequently verified using ANSYS software. Several important findings were obtained. Using the direct GA-APDL approach, continuous-domain optimization reduced the frame weight from 974.5 kg (experience-based design) to 633.7 kg, corresponding to a reduction of 27.98 %, with a total computational time of approximately 50.2 hours. When optimization was performed in the discrete design domain, the optimal frame weight was further reduced to 627.4 kg, achieving a 35.62 % reduction within 38.4 hours. Notably, the GA-ANN surrogate-based optimization identified an optimal frame weight of 600.2 kg, representing a 38.4 % reduction, with a total computational time of only 200 seconds.
The proposed framework integrates discrete design optimization with surrogate-based techniques and has been successfully applied to a real large-scale structural system. The results demonstrate both practical manufacturability and substantial improvements in computational efficiency. Moreover, the proposed ANN-GA-based framework provides a general and scalable solution for the design optimization of complex mechanical systems. It can be effectively extended to applications such as large-scale CNC machines, gantry-based manufacturing equipment, and construction robots, where discrete design constraints and high computational cost are critical challenges.
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