Published at : 07 Dec 2023
Volume : IJtech
Vol 14, No 7 (2023)
DOI : https://doi.org/10.14716/ijtech.v14i7.6660
Ahmad Kholil | Department of Mechanical Engineering, Faculty of Engineering, Universitas Indonesia, Kampus UI Depok, 16424, Indonesia |
Gandjar Kiswanto | Department of Mechanical Engineering, Faculty of Engineering, Universitas Indonesia, Kampus UI Depok, 16424, Indonesia |
Adnan Al Farisi | Department of Mechanical Engineering, Faculty of Engineering, Universitas Indonesia, Kampus UI Depok, 16424, Indonesia |
Jos Istiyanto | Department of Mechanical Engineering, Faculty of Engineering, Universitas Indonesia, Kampus UI Depok, 16424, Indonesia |
This study aimed to optimize lattice structure design by changing the size of
unit cell at a constant volume. It
was observed that the changes in unit cell affected the
strength of lattice structure, posing a challenge for additive
manufacturing. To evaluate these effects, Finite Element Analysis
(FEA) was conducted by applying
static loading at one end of the surface from x, y, z-axis, and combination
of model, using Inconel 625 additive manufacturing. Furthermore,
the model was analyzed by plotting graphs of changes in
cell size to deformation and stress. The
addition of outer skin to deformation and stress behavior was
also investigated. Printed parts were manufactured
through additive manufacturing using PLA to
assess how changes in lattice size affected
overhang surface
quality. The results showed that
deformation and stress behavior were influenced by the smallest cross-sectional area and
shape of the unit cell, as shown by the relationships within lattice
structure models. The addition of
compression loads also increased deformation and stress behavior, while high outer
skin thickness reduced these parameters in lattice
model. The results from the printed part of model showed poor
surface quality, particularly on the
overhanging part.
Additive manufacturing; Control volume; Design optimization; Lattice structure; Unit cell
The
topic of lattice structure design is one of the most active areas in additive manufacturing
(AM) study. AM has the ability to produce complex lattice structure while
maintaining geometry, optimizing the manufacturing of parts by the
reduction in material without compromising the
strength and deformation aspects. According to ASTM52900-21, AM is
the process of joining materials to create parts from 3D model data, typically
one layer after another, compared
to subtractive manufacturing and formative
manufacturing methodologies (Kiswanto, Kholil, and Istiyanto, 2023; ASTM-52900, 2021). Furthermore, it is a 3D printing technology with
significant potential for revolutionizing various industries. This innovative
manufacturing enables the production of complex and intricate structures that
were previously unattainable through conventional processes such
as casting, forging, and machining (Zhong et al., 2019). The method allows 3D models drawn with
computer-aided designs to be presented as functional products estimated during
the early design phase quickly and efficiently (Saptaji et al., 2022; Budiono, Kiswanto, and Soemardi, 2014).
Filament based-Material Extrusion
Additive Manufacturing (FMEAM) is increasingly used as one of the prominent AM
methods. In this method, polymeric materials are commonly preferred due to the
low cost. However, metal filaments have been used, such as Atomic Diffusion
Additive Manufacturing (ADAM) technology by Markforged. FMEAM with metal
filaments is the mixing of metal powder particles with polymer binders to
create a product applicable as a continuous feed in a 3D printer. This process
is usually followed by a chemical and temperature treatment (Kiswanto, Kholil, and Istiyanto,
2023; Nurhudan
et al., 2021). In 3D printing, support
structures are often needed to prevent the collapse of taller or smaller parts
of the object during printing. Meanwhile, the removal of these structures after
completion often requires a significant amount of material and time, leading to
increased waste and higher production costs (Panesar
et al., 2018). One of the attractive
applications of FMEAM is the fabrication of lattice structure, offering
exceptional lightweight, high-strength, and energy-absorbing properties.
Therefore, the importance of lattice structure design that can minimize the
need for support structures becomes crucial in reducing material waste and
conserving energy during the manufacturing process (He et al., 2022;
Nurhudan et al., 2021;
Haghshenas and Khonsari, 2018; Tang et
al., 2018).
Lattice structure is
characterized by periodic arrangements of interconnected struts, creating a
network of voids in the solid material. The structure has significant
mechanical properties, such as high stiffness-to-weight ratio and enhanced
energy absorption capabilities, allowing the suitability for various
engineering applications (Benedetti
et al., 2021;
Cheng, Bai, and To, 2019;
Tang et al., 2018). However, the intricate geometry
and internal complexity pose significant challenges when analyzing mechanical
behavior. Lattice structure also offers several advantages, including the
provision of specific strength and stiffness to an object while significantly
reducing material usage (Zhong et al., 2019; Du et
al., 2020; Yap et al., 2015;
Wang et al., 2020). These properties are essential
in the design of objects in industries such as aerospace, automotive, medical,
and other manufacturing fields (Dong et al., 2020). A previous study on the
triangular lattice structure of Inconel 625 observed a 57.6% reduction in
impact toughness compared to the solid infill pattern (Kiswanto, Kholil, and Istiyanto,
2023). During the analysis,
compressive test was conducted on SC, HC, BCC, and PG80 lattice structures (Seek et al., 2022), while functionally graded
lattice, including BCC and hexagonal HC structures, used photo-curable
polyurethane resin (Park
and Park, 2020). Despite the difference in
volume, there is an insignificant comparison between models, as this approach
is not apples-to-apples and profitable based on the volume of materials used.
Consequently, this study presents a novel approach to controlling lattice
volume.
In AM process, Computer-Aided
Design (CAD) is crucial for designing the objects to be printed. However,
creating effective lattice structure design using CAD software can be a
challenge, particularly when there is a need for adaptation to specific AM
technology such as MEAM. One of the main challenges includes the availability of
free software that aids in designing product to create structure with the
desired shape, size, and volume, in a short period (Barclift
et al., 2017). To address these issues, this
study presents CAD module capable of automatically generating lattice structure
based on Application Programming Interface (API). CAD API is an application
programming interface that allows users to access and manipulate data in CAD
software. CAD API tool has been developed using the Visual Basic programming
language in SolidWorks software (Zhang et al., 2019; Nguyen et al., 2018) to facilitate the modification of unit cell and lattice structure
parameters.
Finite Element Analysis (FEA) is
a powerful tool for investigating the mechanical response of complex
structures, providing valuable insights into the behavior under different
loading conditions (Hamza et al., 2023). This tool enables the
prediction and optimization of lattice structure performance before their
physical realization (Cheng, Bai, and To, 2019; Tang et al., 2018). Consequently, this study focuses on FEA application to analyze
lattice structure models using Inconel 625 material additive manufacturing.
This study
aimed to
develop
lattice structure model and perform FEA using the same unit
cell, different sizes, and a
constant volume.
FEA was
conducted on lattice structure models by providing static loading at one end of
the model surface
from x, y, z, and combination directions. Specifically, the material
selected for FEA was
Inconel 625 additive manufacturing. The effect of different sizes of unit cell
on deformation and stress, including the addition of outer skin was investigated. Printed parts produced
through FMEAM with
PLA were verified
to assess the quality
of the overhang surface. This method was expected to reduce material,
improve efficiency in the manufacturing process, and
maintain
high strength as well as
low deformation. The consideration was used to optimize the
manufacturing of parts in reducing material without minimizing the strength and deformation
aspects. By comparing
models with a constant
volume,
this study determined how changes in unit cell dimensions correspond
to variations
in strength and deformation.
Figure 1 Unit cell design of lattice structure
Where V is the volume (mm3),
and to achieve a constant volume, the parameters a, b, c, z, and y (mm) are
fixed, while z and x are varied. The value of y is obtained from Equation 2 and
x is derived from Equation 4.
Where the parametric value of ranges from 0.1 to 0.9, but in this study, a value of = 0.5 is used. This value is selected as half the width of the unit cell and a fixed parameter in generating lattice models.
The results of unit cells with varying sizes z and x, are shown in Figure 2. All unit cells have a constant volume of 1200 mm3, while the dimensions vary in z value from 8.8 mm to 6 mm with a change of 0.2 mm to obtain 15-unit cells. The value of x is taken from equation 4, while the values a, b, c, and y are constant.
Figure 2 Size parameters of the unit cell
The design of lattice structure model with the same unit cell, different sizes, and a constant volume requires tools created in CAD software. API service was developed based on the Visual Basic programming through Solidworks. Figure 3a shows the interface of API service, which is used to input the parameter values of a, b, c, z, y, and V, where the value of x will be generated according to Equation 4. Subsequently, the input of the upper and lower base parameter values is followed by determining the number of unit cells in directions a, b, and c. Figure 3b shows lattice model generated from API service.
Figure 3 (a) The interface of parameters lattice structure, (b) model of lattice
structure generated by API service
Figure 4 shows CAD model of
lattice structure model generated through API service, using the data obtained
from Figure 2. The number of unit cells in directions a, b, and c are 6, 5, and
8, respectively, resulting in a total of 240 unit cells forming lattice
structure. The top and bottom bases are created with a size of 10 mm each. Each
lattice model has a constant volume of 360,000 mm3
with a total dimension of 60 mm x 60 mm x 132 mm. All lattice models have a
constant mass of 3,038.4 g for each model. The unit
cell of each lattice structure varies in z value from 8.8 mm to 6 mm with a
change of 0.2 mm. In this study, 15 lattice structure models are obtained, as
presented in Figure 4 for analysis.
Figure 4 Lattice structure model generated by API service
FEA was conducted using ANSYS 2023 student version. Figures 5a-e show the boundary conditions of the simulation. One of the final surfaces of the models was given a fixed constraint, while the other in the front was given a force. The first simulation in Figure 5a applied forces in x-axis with a magnitude of 100 kN. The simulation was performed on 15 lattice structure models and 1 solid model. The material used was Inconel 625 Additive Manufacturing. The same boundary conditions were applied for all models in the second simulation, as shown in Figure 5b, with forces in y-axis at a magnitude of 100 kN. Similarly, the third simulation presented in Figure 5c applied forces in the z-axis with a magnitude of -100 kN. The fourth simulation in Figure 5d applied forces in xyz-axis with a magnitude of 100 kN. All simulations were performed on 15 lattice structure models and 1 solid model. Additionally, FEA was conducted with varying compression loads ranging from 100 kN to 1500 kN on lattice structure model, solid model, and lattice structure model with outer skin thicknesses of 1 mm, 3 mm, and 5 mm, as shown in Figure 5e.
Figure 5 Boundary
condition of FEA for lattice structure models with (a-d) loads in x, y, z-axis, and
combination, (e)
100 – 1500 kN compression loads in the z-axis
The final step is printing pf all models through
Flashforged with PLA material. Parameter settings are defined by layer
thickness of 0.1 mm, extruder temperature 210oC, platform
temperature 50oC, travel speed 80 mm/s, and without support.
FEA results of deformation for 15 lattice structure models and 1 solid model are shown in Figure 6. In x-axis and y-axis, the deformation curves showed the same pattern, obtaining the lowest values obtained by model 15 at 0.889 mm and 0.999 mm. For the z-axis, the lowest deformation was observed in lattice model 15, at 0.039 mm. In the combined xyz deformation, there was a significant decrease in deformation values from model 1 to 7, followed by a continuous reduction trend. Comparing the deformation results between the solid and lattice structure in the combined xyz, the solid model showed a value of 0.779 mm, while the smallest value was observed in lattice structure model 15, at 1.61 mm.
Figure 6 Deformation behavior was
affected change dimension of unit cell under x, y, z, and combination loading
Figure 7 shows the results of stress behavior for the model. The maximum stress values in x, y, z-axis, and combination were obtained by model 1, at 771 MPa, 770 MPa, 102 MPa, and 1,315 MPa, respectively. These values decrease as the shape of the unit cell changes. In x-axis, the smallest stress was obtained by model 12, at 677 MPa, while y-axis had the smallest stress of 674 MPa obtained by model 13. For the z-axis compression, model 15 had the lowest stress, with a stress of 69.9 MPa. Regarding the combined xyz, the lowest stress value was found in model 12, at 702 MPa, while the solid model had 487 MPa on x-axis and y-axis, of 47 MPa on the z-axis, and 677 MPa in combination loads.
Figure 7 Stress behavior was affected
change dimension of unit cell under x, y, z, and combination loading
The deformation and stress values were
influenced by the smallest cross-sectional area of the unit cell, as shown in
Figure 2. Model 1 has the smallest unit cell cross-sectional area, increasing
to the maximum in Model 13, followed by a decrease in Model 15. The shape
factor could also be influenced, particularly the load in x-axis or y-axis, and
the combination, causing bending in lattice structure.
Figures 8 and 9 are FEA images of
deformation and stress behaviors of model 1 under x, y, z, and combination
loading.
Figure 8 FEA result of deformation behaviors for
loads: (a) Fx = 100 kN, (b) Fy = 100 kN, (c) Fz = -100 kN, (d) Fxyz =100 kN,
and (e) Fxyz =100 kN of the solid model
Figure 9 FEA result of stress behaviors for loads:
(a) Fx = 100 kN, (b) Fy = 100 kN, (c) Fz = -100 kN, (d) Fxyz =100 kN, and (e)
Fxyz =100 kN of the solid model
Figure 10a shows the results of maximum deformation for the solid model, lattice Model 5, and lattice Model 5 with an outer skin of 1 mm, 3 mm, and 5 mm, respectively. Under compression loads ranging from 100 kN to 800 kN, the five models did not show significant differences in deformation. However, as the compression load increased from 900 kN to 1500 kN, substantial differences were observed, showing an increasing trend with the addition of load for each model. At a compression load of 1500 kN, model 5 showed the highest deformation at 8.6 mm, followed by lattice models with outer skin thicknesses of 1.0 mm, 3.0 mm, and 5.0 mm, and the solid model, at 5.01 mm, 2.02 mm, 1.25 mm, and 0.34 mm, respectively. The results showed that increasing the applied compression load led to a rise in deformation, while higher thickness caused a significant reduction (Kumar et al., 2020). Figure 10b shows the results of maximum stress for the solid model, model 5, and model 5 with outer skin of 1 mm, 3 mm, and 5 mm. As the applied load varied from 100 kN to 1500 kN, there was a trend of increasing stress for each model. Among the five models, at a load of 1500 kN, Model 5 has the highest stress, with a value of 1130 MPa. This was followed by lattice models with outer skin thicknesses of 1 mm, 3 mm, and 5 mm, and the solid model, showing maximum stress values of 941 MPa, 754 MPa, 738 MPa, and 699 MPa, respectively. The results showed that increasing the applied compression load improved maximum stress and energy absorption capability, while additional thickness in the outer skin caused a significant (Seek et al., 2022; Kumar et al., 2020).
Figure 10 (a) Deformation, and (b) stress
behavior of lattice model with outer skin under press loads of 100-1500 kN
Figure 11a-b shows the printed
part of models 1-15 built through FMEAM. Verification of printing results with
FMEAM using PLA was carried out to determine how changes in lattice size
affected the quality of the overhang surface. As shown in Figure 11c, the
overhang structure did not collapse, although support was not added. However,
the surface quality is good compared to the structure that does not overhang.
Figure 11 (a-b) model 1-15 built by FMEAM, (c) lattice models with overhang structure.
In conclusion, this
study aimed to develop
lattice model optimization method using the
same basic unit cell shape with different sizes and a constant volume created by API service. This method was expected to reduce material usage and improve efficiency in the
manufacturing process while maintaining high strength and low deformation. The results suggested that changing
the size of lattice cells at a constant volume affected the strength of the structure. Furthermore, changes in the dimensions of cell lattice models with x, y,
z axis, and
combined loading directly
influenced deformation
and stress. Lattice Model 15 had the smallest deformation and stress compared
to the others. FEA results showed a
considerable increase in deformation and stress, particularly in comparison to
the solid. Increasing the
thickness of the outer skin caused a
reduction in the values of these
variables. The
printed models with FMEAM showed
poor surface quality, specifically
on the overhanging parts, but can
be fixed through
post-processing. Further studies should focus on establishing the optimal lattice models and thickness of the outer skin for a part such as a
turbine blade.
The authors are grateful for the financial
support from RIIM BRIN grant number: 97/IV/KS/11/2022. The authors are
also grateful to the Engineering
Faculty of Universitas Indonesia for
providing Seed Funding Grant of 2022.
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