Characterization of the Dimensional Precision, Physical Bonding, and Tensile Performance of 3D-Printed PLA Parts with Different Printing Temperature

: In this study, tensile test specimens were fabricated using a material extrusion 3D-printer at various printing temperatures to evaluate the development of physical bonds within the same layer as well as in between previous layers. The tensile test specimens were fabricated using PLA material, with printing temperatures ranging from 180 ◦ C to 260 ◦ C. Experimental investigations were conducted to investigate the dimensional accuracy and physical appearance of the parts across printing temperatures. Uniaxial tensile tests were conducted at a strain rate of 1 mm/min and repeated five times for each variable in accordance with the ASTM D638-14 standard. Results showed that increasing the printing temperatures yielded parts with better tensile properties. An approximate difference of 40% in tensile strength was observed between specimens fabricated under the two most extreme conditions (180 ◦ C and 260 ◦ C). The changes in tensile properties were attributed to bonding mechanisms related to interlayer bonding strength and a reduction in voids within the internal geometry. Analysis of the fracture surface using scanning electron microscopy (SEM) revealed fewer and smaller voids within the internal geometry for parts printed at higher temperature. The percentage area of voids reduced significantly when the printing temperature was increased from 180 ◦ C to 220 ◦ C. The tensile properties continuously improved with the printing temperature, with parts printed at 220 ◦ C exhibiting the highest dimensional accuracy. The findings offer insight into the impact of the printing temperature on both the external physical bonds between printed roads, affecting the physical appearance and dimensional accuracy, and the internal bonds, affecting the tensile properties of the fabricated parts.


Introduction
Over the past 25 years, additive manufacturing (AM) has seen a mass increase in adaptation for manufacturing processes in the industry.The technology was commonly used to produce proof-of-concept prototypes in its pioneering stages but has matured as an alternative method to produce complex-shaped products.Therefore, AM technologies have since grown to become a manufacturing technology that is able to compensate for the shortcomings of traditional manufacturing methods such as subtractive, formative, and molding technologies [1].Intensive research in these technologies has aided in the development of materials, software, equipment, and processing capabilities such as speed, resolution, and dimensional accuracy related to additive manufacturing.Through these advancements, increasing interest has been drawn to adopt AM technologies in the manufacturing industry [2].The direct fabrication of fully functional parts is the current trend that dictates the advancement of additive manufacturing technologies.In recent years, AM technologies have been rapidly developed for the automotive industry due to their ability to shorten the time needed for product design and development as well as the production of highly customized parts for optimized performance [3,4].
The AM process begins with the generation of a 3D model, which is then sliced into 2D cross-sections containing information on each layer.The 2D-data are then transferred to the AM machine and built in a layer-by-layer manner [5].Therefore, these complex 3D-models can be fabricated directly without the requirement of specific fixtures or tools [6].AM technologies can be subdivided into several categories: material extrusion, VAT photopolymerization, powder bed fusion, binder jetting, material jetting, sheet lamination, and direct energy deposition [7].Fused deposition modeling (FDM), which falls under the category of material extrusion, was originally developed by Scott Crump in the late 1980s and patented by Stratasys Inc. [8].The equivalent technology, which utilizes the same principle, is known as fused filament fabrication (FFF).Since the expiration of the patent in 2009, the possibilities for low-cost FDM printers have gained more attention and paved the way for accessible 3D-printing.Due to its simplicity and low cost, numerous brands and variations of printers based on this technology have been developed in the past decade.FFF is an AM technology that is commonly used to fabricate polymer and composite materials as it is low-cost, simple to use, and has the ability to print large parts compared to other AM technologies [9,10].The mechanical properties, accuracy, roughness, speed, and material cost of parts manufactured by various AM techniques (stereolithography, FFF, material jetting, powder bed fusion, 3D printing (3DP), and sheet lamination) have been compared in a previous study.FFF is able to produce parts with a high impart strength but exhibited disadvantages in term of accuracy, roughness, speed, and compressive strength [11].Among the two most popular AM techniques for polymers (FFF, VAT photopolymerization), FFF is more user friendly and requires less production time than VAT photopolymerization.However, the print quality of an FFF printed part is not as good as the print quality of VAT photopolymerization [12].Most commercial polymers are petrochemical-based and made from non-renewable sources.Popular materials commonly used with FDM are acrylonitrile butadiene styrene (ABS), polyethylene-terephthalate-glycol (PETG), and polyether-etherketone (PEEK) due to their enhanced mechanical properties, reliability, and durability [13].Polylactic acid (PLA) is a type of biodegradable plastic made from renewable sources such as sugar cane and corn [14,15].Its low printing temperature, ease of use, and biodegradability makes this one of the most popular materials used with FFF.Furthermore, PLA is also increasingly utilized in the biomedical field to produce patient specific implants and prostheses due to its material properties such as biocompatibility, sterilizability, low weight, and cost [16][17][18][19][20].Finally, PLA is able to degrade into the surrounding environment without harm at the end of its life cycle [21].
The process of model fabrication in FFF begins by feeding a filament made from thermoplastic polymers through an extruder head.The liquefier in the extruder head heats the filament material into its molten or semi-molten state and systematically deposits it in the form of roads onto the build platform.As soon the molten material is deposited, it cools down and solidifies, forming a layer based on the computer-generated file.The process repeats, and a new layer is built upon the previous layer until the 3D-model is formed [22].The strength and quality of FFF fabricated parts are often compared with their traditionally manufactured injection molded counterparts as they are made of the same material.However, it should be noted that FFF fabricated parts are weaker compared to injection molded parts, even if they are printed at 100% infill [23].One major drawback of FFF fabricated parts is their poor mechanical properties due to weak physical bonding between the deposited roads [24].The development of bonds is highly dependent on the temperature development during printing as the core principle is derived from extrusion and relies on the heating and cooling of thermoplastic material.Additionally, the strength of the parts is also compromised by the weak interlaminar bonding and the presence of voids due to the nature of the layer-by-layer deposition process [25].Void formation within the parts can be associated with the incomplete neck growth between deposited roads where they solidify before polymer coalescence with adjacent and preceding layers is complete [26,27].Previous studies have concluded that inter-filament bonding improves when the printing temperature is higher due to the reheating effect on the previously deposited roads by increasing the time window available for bond development.However, a reduced dimensional accuracy was observed when an excessively high printing temperature was used [8][9][10].
FFF 3D-printing has established itself as a favored additive manufacturing technology used to process thermoplastic materials due to its ease of use and low cost over the years.As a result, numerous researchers worldwide have contributed to the advancement of FFF processes in terms of performance and explored the influence of process parameters on the quality and properties of the fabricated parts [28].The quality of the FFF fabricated parts depends on the combination of a variety of process parameters such as printing temperature, build plate temperature, print speed, layer thickness, build orientation, and infill pattern [29][30][31][32][33].Most of the research that has been carried out investigated the effect of optimizing a variety of process parameters to produce parts with better mechanical performance [34][35][36][37].Furthermore, the implementation of fiber reinforcements [38], particles, compatibilizers, nanomaterials, and other techniques into the final product has also been explored to improve the mechanical properties of the fabricated parts [39][40][41][42].Domingo-Espin et al. [43] confirmed that the mechanical properties of parts fabricated by FFF were affected by part orientation and build direction, and suggested that tensile loading should not be applied perpendicular to the layer planes to avoid fragile fracture due to the weak bonding between layers.Kaveh et al. [44] investigated the possibility of optimizing process parameters such as feed and flow rate, filament width, and printing temperature to improve the internal cavity and precision of FFF fabricated parts.It was concluded that the interlayer mechanical properties are affected by the formation of bonds between the deposited roads, which depends on the diffusion bonding of the polymer across the interface.The above-mentioned studies also focused on the effect of different process parameters and the resulting mechanical properties (tensile, flexural, and impact) of the FFF fabricated parts.
Specific to printing temperature, researchers have found that increasing the printing temperature has a positive effect on the mechanical properties, but that an excessive increase results in more brittle parts [45].Vanaei et al. [46] studied the effect of extrusion and platform temperature as well as the cooling factors that affected the bonding between the materials and concluded that the effect of the extruder temperature was more significant compared to other process parameters.Benwood et al. [47] and Alafaghani et al. [48] investigated the mechanical properties of parts fabricated using PLA material and observed that the maximum strength for the material was around 200 • C to 220 • C.They concluded that the extrusion temperature-strength relationship is not linear.This is likely due to the rheological property of the material where it loses viscosity, resulting in the formation of constant voids within the material [49].Based on the literature, the printing temperature is an important printing parameter as it is the main heat source provided to the material and dictates the successful extrusion of material, while at the same time, it induces changes in the material properties.
The physical bonding between adjacent and preceding roads within the internal cavity greatly affects the resulting mechanical properties of the FFF fabricated parts and are commonly attributed to bond development during the printing process.During the printing process, a stream of semi-molten filament material is extruded next to another existing filament; viscous flow of the polymer causes a neck formation as they are in a molten state.Molecular diffusion at the interface and randomization can be explained using the reptation theory.De-Gennes [50] developed a reptation model to explain the concept of the diffusion bonding of polymeric materials.In later research conducted by Kim et al. [51], the motion of chains across the interface was presented in five stages, which included surface arrangement, surface approach, wetting, diffusion, and randomization.Sun et al. [52] further extended the concept and reorganized bond formation into surface contact, neck growth and molecular diffusion, and randomization across the interface.The time required for diffusion and randomization can be approximated by the reptation time of the polymer chain [53].Coogan et al. [54] presented a method utilizing a diffusioncontrolled healing model to predict the bond formation strength of FFF fabricated parts.The researchers also concluded that air gaps/porosity had the most influential effect on the mechanical properties and attributed the mechanical anisotropy of the FFF fabricated parts to porosity ratio present inside the parts [55][56][57][58].In a study conducted by Abbott et al. [59], it was reported that the infill angle and air gap had the largest influence on the mechanical properties.The coalescence of adjacent roads at different printing temperatures and different printing strategies (unidirectional and bidirectional) was numerically modeled in a recent work [60] that reported that increasing the printing temperature increased the coalescence between roads.
Based on the literature review, it can be seen that many similar studies have been conducted to investigate the effect of various process parameters on the resulting mechanical properties as well as statistical approaches to yield the best mechanical properties [61,62].However, the underlying relationship between PLA printing temperature and the resulting physical bonding within the internal cavity as well as its subsequent impact on the tensile properties of PLA have not been investigated in detail.Furthermore, to the best of our knowledge, the correlation between printing temperature, voids, and tensile strength has not been previously systematically reported and quantified.Thus, this study aimed to assess the quality of the bonds by quantifying the average size and percentage area of voids present between the deposited roads that result in measurable changes in tensile strength over a range of printing temperatures.It is believed that the formation of voids is a result of incomplete physical bonding between adjacent and preceding roads that can be related to neck formation and molecular diffusion across the interfaces.Furthermore, the physical appearance and dimensional accuracy of the fabricated parts were also investigated with reference to different printing temperatures.The outcome of this paper provides a better understanding on how optimizing the printing temperature affects the quality of the bonds formed within the internal cavity and its implication in the tensile properties of FFF fabricated parts.

Materials and Sample Preparation
Tensile test specimens were fabricated using an FFF 3D-printer (Creality Ender 3v2, Shenzhen, China) with a print precision of ±0.1 mm, X-Y axis precision of 0.012 mm and Zaxis precision of 0.004 mm [63] using a 0.4 mm nozzle.The study was conducted by varying the printing temperatures from 180 • C to 260 • C at intervals of 10 • C. All of the samples were printed using yellow-colored PLA material (Polymaker Polylite, Shanghai, China) with a diameter of 1.75 mm at 100% infill density.The printing temperature was chosen based on the recommended values in the technical data sheet provided by the manufacturer, which was between 180 • C and 240 • C. The range of printing temperature was further expanded up to 260 • C to investigate the behavior of the material above the recommended settings, but kept slightly below the degradation temperature of PLA, which is around 280 • C [64].Attempts to print the PLA specimens below 180 • C were unsuccessful and resulted in clogging of the nozzle, but printing above the recommended peak temperature of 240 • C did not result in any difficulties.According to the PLA material data sheet, the material has an elastic modulus of 2.6 GPa, and an ultimate tensile strength (UTS) of 46.6 MPa for use under standard processing conditions.The material was stored in a humiditycontrolled container (AIPO AS-31, Zhuhai, China) prior to the fabrication process.To mitigate external factors affecting the investigation, other process parameters were fixed, as shown in Table 1.The samples were printed flat on the build platform as shown in Figure 1a.A raster orientation of [0 • /90 • ] was selected for this study to allow brittle fracture to occur.The orientation was selected to produce fracture surfaces with clear boundaries between preceding layers at the fracture surface based on previous studies [65].The micrographs of the fracture surfaces were then used to quantify the percentage porosity within the internal cavity.The arrangement of the raster is presented in Figure 1b, and the methods used to assess the FFF fabricated specimens in this investigation were: (i) dimensional accuracy and physical appearance, (ii) tensile properties and behavior, and (iii) physical bonding and the formation of voids.
Table 1.Process parameters and settings used in the investigation.

Process Parameter Setting
Nozzle printing temperature 180 • C to 260 • C (at intervals of 10 with clear boundaries between preceding layers at the fracture surface based on previous studies [65].The micrographs of the fracture surfaces were then used to quantify the percentage porosity within the internal cavity.The arrangement of the raster is presented in Figure 1b, and the methods used to assess the FFF fabricated specimens in this investigation were: (i) dimensional accuracy and physical appearance, (ii) tensile properties and behavior, and (iii) physical bonding and the formation of voids.

Measurement of Dimensional Accuracy
A total of six specimens were fabricated for each printing temperature according to ASTM D638-14 Type I and measured 165 mm long, 19 mm wide, and 7 mm thick.The gauge cross-sectional area of the specimens was 13 mm × 7 mm (width × thickness) with a 50 mm gauge length thickness, as presented in Figure 1b.The length, width, and thickness of the specimens were measured at three different locations, as presented in Figure 2, using digital calipers (Mitutoyo, Japan) with an accuracy of ±0.01 mm, and the average values were compared with the designed specifications to determine the dimensional accuracy.The physical appearances of three specimens were selected from each printing temperature and observed using a digital microscope (CoolingTech, ShenZhen, China).

Measurement of Dimensional Accuracy
A total of six specimens were fabricated for each printing temperature according to ASTM D638-14 Type I and measured 165 mm long, 19 mm wide, and 7 mm thick.The gauge cross-sectional area of the specimens was 13 mm × 7 mm (width × thickness) with a 50 mm gauge length thickness, as presented in Figure 1b.The length, width, and thickness of the specimens were measured at three different locations, as presented in Figure 2, using digital calipers (Mitutoyo, Japan) with an accuracy of ±0.01 mm, and the average values were compared with the designed specifications to determine the dimensional accuracy.The physical appearances of three specimens were selected from each printing temperature and observed using a digital microscope (CoolingTech, ShenZhen, China).The dimensional accuracy of the parts fabricated at different printing temperatures was examined by comparing the measured length, width, and thickness with the designed specifications.The absolute and dimensional error were calculated as:

Tensile Testing
Tensile testing was conducted using a universal testing machine (Galdabini Quasar 25, Cardano al Campo, Italy) at a strain rate of 1 mm/min until failure occurred in the form of fracture.The extension of the specimens was measured and recorded using an axial extensometer (Reliant EAG, Colorado Springs, CO, USA).A minimum of five specimens from each printing temperature was tested according to the ASTM test procedures and only the results from specimens that fractured within the gauge length were included for analysis.The corresponding results were plotted into a stress-strain curve based on the average values from five tests.

Fracture Surface Observation and Analysis
Quantitative analysis and imaging are methods used to analyze the formation of voids in FFF fabricated parts [26].The cross-section of the fracture surface from the specimens was observed under scanning electron microscope (LEO 1455VP, Germany) at 20× and 50× magnification to determine the physical bonding between filaments at selected printing temperatures (extreme temperature and budget constraints).The SEM micrographs were imported to an image processing software, ImageJ (v1.54g), and analyzed to see whether changes in the printing temperature affected the physical bonding between the printed roads, which is influenced by neck formation and molecular diffusion.A method utilized by Abbott et al. [59] to quantify the contact length between extruded roads of the specimens was initially considered, but the results were not beneficial as it was difficult to distinguish the boundaries between the adjacent roads at printing temperatures above 220 • C. Consequently, a method of quantifying the average size of the voids and the percentage area of void spaces was used in this study.It should be noted that the measurements are highly dependent on the region where the measurements are conducted.Therefore, the analysis was conducted at four different regions of the cross-sectional fracture surface to obtain an average, as shown in Figure 3. Using the image processing software (ImageJ), the average size and percentage area of void spaces from the micrographs were identified by adjusting the threshold level, which were converted to a binarized form.Figure 4 shows an example of the conversion of the SEM micrographs into the binary form to calculate the average size and percentage area of the voids using the particle analysis tool available in the software [67].The average size and percentage area of voids from the binarized images were then complied and re- Using the image processing software (ImageJ), the average size and percentage area of void spaces from the micrographs were identified by adjusting the threshold level, which were converted to a binarized form.Figure 4 shows an example of the conversion of the SEM micrographs into the binary form to calculate the average size and percentage area of the voids using the particle analysis tool available in the software [67].The average size and percentage area of voids from the binarized images were then complied and related to the recorded tensile strength at different printing temperatures.Using the image processing software (ImageJ), the average size and percentage area of void spaces from the micrographs were identified by adjusting the threshold level, which were converted to a binarized form.Figure 4 shows an example of the conversion of the SEM micrographs into the binary form to calculate the average size and percentage area of the voids using the particle analysis tool available in the software [67].The average size and percentage area of voids from the binarized images were then complied and related to the recorded tensile strength at different printing temperatures.

Physical Appearance of Specimens
Figure 5 illustrates the fractured tensile specimens fabricated at different temperatures.It can be observed that the surface finish of the specimens differed at different printing temperatures, as shown in Figure 5a-i.The deposited molten filament is known as a 'road' and takes the shape of the nozzle.At low printing temperatures, there is a clear division of boundaries between the deposited roads.The physical appearance of the surface also becomes shinier as the printing temperature is increased, as illustrated in Figure 5e-i.This is likely due to the higher percentage of crystallinity as a longer time is available for the molecular chains to rearrange into its crystallized form.PLA is a semi-crystalline polymer where the polymer chains are arranged in either a random amorphous phase or a highly organized crystalline phase [68].PLA is known to have a slow crystallization time, which means that the polymer needs to be cooled slowly to allow sufficient time for recrystallization to occur.At lower printing temperatures, the cooling process is rapid, therefore, the majority of the polymer chains remain in an amorphous arrangement, leading to a low percentage of crystallinity [69].

Physical Appearance of Specimens
Figure 5 illustrates the fractured tensile specimens fabricated at different temperatures.It can be observed that the surface finish of the specimens differed at different printing temperatures, as shown in Figure 5a-i.The deposited molten filament is known as a 'road' and takes the shape of the nozzle.At low printing temperatures, there is a clear division of boundaries between the deposited roads.The physical appearance of the surface also becomes shinier as the printing temperature is increased, as illustrated in Figure 5e-i.This is likely due to the higher percentage of crystallinity as a longer time is available for the molecular chains to rearrange into its crystallized form.PLA is a semi-crystalline polymer where the polymer chains are arranged in either a random amorphous phase or a highly organized crystalline phase [68].PLA is known to have a slow crystallization time, which means that the polymer needs to be cooled slowly to allow sufficient time for recrystallization to occur.At lower printing temperatures, the cooling process is rapid, therefore, the majority of the polymer chains remain in an amorphous arrangement, leading to a low percentage of crystallinity [69].

Dimensional Accuracy
From the results obtained, it can be observed that all of the measured values of width, length, and thickness showed the same trend, whereby the values increased with increasing printing temperature until reaching an optimum printing temperature.From the re-

Dimensional Accuracy
From the results obtained, it can be observed that all of the measured values of width, length, and thickness showed the same trend, whereby the values increased with increasing printing temperature until reaching an optimum printing temperature.From the results, the optimum printing temperature for the PLA material used in this study was 220 • C*, where the specimens had the least dimensional error.
Table 2 summarizes the measured values and dimensional error of the specimens fabricated at different printing temperatures.Specimens fabricated below 220 • C measured smaller, while those above 220 • C measured larger than the designed specifications.The deposition of material at different printing temperatures is highly dependent on the rheological properties of the polymer.This leads to a difference between the intended deposition volume and actual deposition volume, which affects the dimensional accuracy [70].The processing temperature has a significant effect on the viscosity of PLA, which affects the formation of bonds between the deposited roads.Based on the results in Table 2, specimens printed at low temperatures measured smaller than their designed specifications.This can be related to the low fluidity and high viscosity behavior at low temperatures, which leads to the non-uniform and incomplete deposition of PLA material.In contrast, the viscosity of PLA decreases as the working temperature increases, which results in a higher flow capacity.A higher flow capacity results in road spreading and also enhances the die-swell effect, resulting in greater extrudate expansion after the material leaves the nozzle [71,72].Therefore, specimens printed at higher temperatures measured larger than their designed specifications.

Tensile Properties
Based on the results shown in Figure 6, it can be observed that the tensile strength and elastic modulus increased with printing temperature.The stress-strain curve from Figure 7 shows that specimens printed at different printing temperatures exhibited different ultimate tensile strengths, implying a difference in maximum holding capacity.A drastic 23% increase in tensile strength was observed for specimens printed at 180 • C to 200 • C.This can be attributed to the quality of bonds formed within the specimens, which will be discussed in Section 3.5.Increasing the printing temperature after 200 • C to 260 • C contributed to a further 17% improvement in tensile strength.
Figure 7 shows that specimens printed at different printing temperatures exhibited different ultimate tensile strengths, implying a difference in maximum holding capacity.A drastic 23% increase in tensile strength was observed for specimens printed at 180 °C to 200 °C.This can be attributed to the quality of bonds formed within the specimens, which will be discussed in Section 3.5.Increasing the printing temperature after 200 °C to 260 °C contributed to a further 17% improvement in tensile strength.Overall, a 38% difference in tensile strength was recorded for specimens printed at the two most extreme conditions.The strain at break, as shown in Figure 7, showed an increasing trend up to 210 °C, then a gradual decrease was observed after.The fracture mechanism can be described as brittle as the plastic deformation was low, which can be identified as the region between the yield point and rupture point on the stress-strain curve.The results show that PLA exhibits an elastic-plastic response as there is no evidence of strain hardening beyond the yield strength [68].

Void Formation
Quantitative analysis was conducted using the SEM micrographs at 50x magnification.Figure 8 shows the relationship between the percentage and average size of voids with the printing temperature.The trend of the results illustrates a significant decrease in the percentage area of voids when the printing temperature increased from 180 °C to 220 °C, while a further increase in printing temperature had a lesser effect on reducing the percentage area of voids.In contrast, the average void size showed a steady decrease from 180 °C up to 260 °C.The improvement in physical bonding can be attributed to the improved neck formation and molecular diffusion, where greater overlap between deposited roads was observed.Therefore, increasing the printing temperature leads to a reduced percentage of voids.Figure 9 shows the relationship between the ultimate tensile strength and percentage of solid region within the internal geometry with printing temperature.Based on the results, it is clear that a higher tensile strength is a result of parts with a higher density within their internal geometry.Overall, a 38% difference in tensile strength was recorded for specimens printed at the two most extreme conditions.The strain at break, as shown in Figure 7, showed an increasing trend up to 210 • C, then a gradual decrease was observed after.The fracture mechanism can be described as brittle as the plastic deformation was low, which can be identified as the region between the yield point and rupture point on the stress-strain curve.The results show that PLA exhibits an elastic-plastic response as there is no evidence of strain hardening beyond the yield strength [68].

Void Formation
Quantitative analysis was conducted using the SEM micrographs at 50x magnification.Figure 8 shows the relationship between the percentage and average size of voids with the printing temperature.The trend of the results illustrates a significant decrease in the percentage area of voids when the printing temperature increased from 180 • C to 220 • C, while a further increase in printing temperature had a lesser effect on reducing the percentage area of voids.In contrast, the average void size showed a steady decrease from 180 • C up to 260 • C. The improvement in physical bonding can be attributed to the improved neck formation and molecular diffusion, where greater overlap between deposited roads was observed.Therefore, increasing the printing temperature leads to a reduced percentage of voids.Figure 9 shows the relationship between the ultimate tensile strength and percentage of solid region within the internal geometry with printing temperature.Based on the results, it is clear that a higher tensile strength is a result of parts with a higher density within their internal geometry.
Figure 8 shows the relationship between the percentage and average size of voids with the printing temperature.The trend of the results illustrates a significant decrease in the percentage area of voids when the printing temperature increased from 180 °C to 220 °C, while a further increase in printing temperature had a lesser effect on reducing the percentage area of voids.In contrast, the average void size showed a steady decrease from 180 °C up to 260 °C.The improvement in physical bonding can be attributed to the improved neck formation and molecular diffusion, where greater overlap between deposited roads was observed.Therefore, increasing the printing temperature leads to a reduced percentage of voids.Figure 9 shows the relationship between the ultimate tensile strength and percentage of solid region within the internal geometry with printing temperature.Based on the results, it is clear that a higher tensile strength is a result of parts with a higher density within their internal geometry.Based on the SEM micrographs in Figure 10, a lack of bond overlap is clear at low printing temperatures.A significant reduction in the size and percentage area of voids was observed as the printing temperature increased, which improved the physical bonding between the roads.The influential factors affecting the fracture dynamics and plastic deformation of the specimens are the physical bonding between roads and the voids that form within the internal geometry.A larger and higher percentage of voids could be observed for specimens printed at lower temperatures based on the SEM micrographs of the failure crosssection, as shown in Figure 10a,b.The strength degradation can be attributed to the greater residual porosity within the internal geometry contributing to weaker tensile strength and quicker failure.A reasonable assumption is that the voids undergo high-stress concentration upon loading and act as failure points where crack initiation begins [73].The propagation of failure in brittle polymers can be associated with crazing and molecular void formation [74].In terms of the failure mechanism, the presence of voids creates an initiation point for failure that triggers layer delamination upon loading.This effect is more profound when the infill is printed at certain orientations such as those printed at a raster angle of [45°] [65,75].Therefore, controlling the process parameters is an effective way to reduce these effects as well as the porosity related defects that result in failure.Based on the SEM micrographs in Figure 10, a lack of bond overlap is clear at low printing temperatures.A significant reduction in the size and percentage area of voids was observed as the printing temperature increased, which improved the physical bonding between the roads.The influential factors affecting the fracture dynamics and plastic deformation of the specimens are the physical bonding between roads and the voids that form within the internal geometry.A larger and higher percentage of voids could be observed for specimens printed at lower temperatures based on the SEM micrographs of the failure cross-section, as shown in Figure 10a,b.The strength degradation can be attributed to the greater residual porosity within the internal geometry contributing to weaker tensile strength and quicker failure.A reasonable assumption is that the voids undergo high-stress concentration upon loading and act as failure points where crack initiation begins [73].The propagation of failure in brittle polymers can be associated with crazing and molecular void formation [74].In terms of the failure mechanism, the presence of voids creates an initiation point for failure that triggers layer delamination upon loading.This effect is more profound when the infill is printed at certain orientations such as those printed at a raster angle of [45 • ] [65,75].Therefore, controlling the process parameters is an effective way to reduce these effects as well as the porosity related defects that result in failure.
specimens printed at lower temperatures based on the SEM micrographs of the failure crosssection, as shown in Figure 10a,b.The strength degradation can be attributed to the greater residual porosity within the internal geometry contributing to weaker tensile strength and quicker failure.A reasonable assumption is that the voids undergo high-stress concentration upon loading and act as failure points where crack initiation begins [73].The propagation of failure in brittle polymers can be associated with crazing and molecular void formation [74].In terms of the failure mechanism, the presence of voids creates an initiation point for failure that triggers layer delamination upon loading.This effect is more profound when the infill is printed at certain orientations such as those printed at a raster angle of [45°] [65,75].Therefore, controlling the process parameters is an effective way to reduce these effects as well as the porosity related defects that result in failure.

Bond Development Based on Fracture Analysis
During printing, the deposited roads solidify and form cross-bonding with adjacent and preceding roads that were previously deposited through polymer sintering.This phenomenon can be related to the concept of diffusion bonding, which includes surface contact, neck growth, molecular diffusion, and randomization across the interface [52].The mechanical properties of FFF fabricated parts are dictated by the quality of bonds between adjacent and underlying roads.The bonds formed between adjacent roads within the same layer are known as 'intralayer bonds', while bonds formed with preceding roads from previous layers are known as 'interlayer bonds', which is illustrated in Figure 11.A greater overlap between roads is categorized as better physical bonding as less voids are formed within the internal geometry.From the micrographs of the cross-sectional fracture surfaces, it can be confirmed that the printing temperature affects the formation of bonds between roads.The bonds developed are highly dependent on the local temperature at which bonding occurs, which is known as the coalescence temperature.The formation of bonds through polymer diffusion is highly dependent on heating and cooling factors.Therefore, it is important to optimize process parameters such as printing temperature and speed to enhance the strength of bonds.

Bond Development Based on Fracture Analysis
During printing, the deposited roads solidify and form cross-bonding with adjacent and preceding roads that were previously deposited through polymer sintering.This phenomenon can be related to the concept of diffusion bonding, which includes surface contact, neck growth, molecular diffusion, and randomization across the interface [52].The mechanical properties of FFF fabricated parts are dictated by the quality of bonds between adjacent and underlying roads.The bonds formed between adjacent roads within the same layer are known as 'intralayer bonds', while bonds formed with preceding roads from previous layers are known as 'interlayer bonds', which is illustrated in Figure 11.A greater overlap between roads is categorized as better physical bonding as less voids are formed within the internal geometry.From the micrographs of the cross-sectional fracture surfaces, it can be confirmed that the printing temperature affects the formation of bonds between roads.The bonds developed are highly dependent on the local temperature at which bonding occurs, which is known as the coalescence temperature.The formation of bonds through polymer diffusion is highly dependent on heating and cooling factors.Therefore, it is important to optimize process parameters such as printing temperature and speed to enhance the strength of bonds.The schematic diagram shown in Figure 12a,b was reconstructed to illustrate the necking and molecular diffusion between roads within the same layer (intralayer bonds).At higher coalescence temperatures, the time window where the roads are above the polymer glass transition temperature is longer and allows more time for neck growth and molecular diffusion across the interface [53].The strength of the bonds is higher as the roads fuse more closely together, which also results in the reduction in the size and percentage area of voids.Therefore, a longer time window is preferable as it results in the formation of stronger bonds.Figure 12c,d illustrates the development of interlayer bonds with previous layers as The schematic diagram shown in Figure 12a,b was reconstructed to illustrate the necking and molecular diffusion between roads within the same layer (intralayer bonds).At higher coalescence temperatures, the time window where the roads are above the polymer glass transition temperature is longer and allows more time for neck growth and molecular diffusion across the interface [53].The strength of the bonds is higher as the roads fuse more closely together, which also results in the reduction in the size and percentage area of voids.Therefore, a longer time window is preferable as it results in the formation of stronger bonds.Figure 12c,d illustrates the development of interlayer bonds with previous layers as the printing temperature increases.As the printing temperature increases, a stronger and more compact structure is formed as a result of greater overlap with roads from the previous layers.This reduces the tendency for delamination between the layers to occur upon loading, which increases the tensile strength.Besides forming stronger bonds between roads, the deposition of molten filament is also expected to have a reheating effect on adjacent and preceding roads, which promotes polymer diffusion and entanglement.Heat from the freshly deposited road is transferred through heat conduction to the previously deposited roads [77].This reheats the previously deposited roads above their glass transition temperature, allowing for neck formation and polymer diffusion to reoccur [78].Therefore, a higher printing temperature results in a greater reheating effect as more heat can be transferred [79].Based on the results obtained, it can be concluded that a higher printing temperature provides a longer time window for bond development, which results in better neck formation and an increased tensile strength similar to the research by Abbott et al. [59]. is high at lower working temperatures [81].The viscosity material decreases with increasing temperature and flows more easily, allowing better fusion between the roads, thus decreasing the size of the voids.Similar results were reported in a recent numerical simulation, where the kinetics of coalescence increased at higher temperature [60].Based on the SEM micrographs in Figure 12, it can be observed that the majority of the voids formed on the bottom side of the roads.This was identified as all of the samples were placed and viewed using the same orientation during SEM imaging.This phenomenon can be attributed to the printing path taken during the fabrication process which is illustrated in Figure 13a.For the layers printed with an infill orientation of 90 degrees, the deposited roads take a shorter printing path compared to layers of 0 degrees.Due to the shorter path, the adjacent roads are of higher temperature when new roads are deposited, thus increasing the time window available for diffusion bonding.At a high printing temperature, the low viscosity molten PLA quickly fills the gaps from previous layers due to gravitational force.The presence of voids within the part can be associated with inadequate neck formation and molecular diffusion and is more profound at lower printing temperatures.The voids act as a point for crack initiation where upon loading results in failure [80].The formation of voids can be attributed to the rheological behavior of PLA, where viscosity is high at lower working temperatures [81].The viscosity material decreases with increasing temperature and flows more easily, allowing better fusion between the roads, thus decreasing the size of the voids.Similar results were reported in a recent numerical simulation, where the kinetics of coalescence increased at higher temperature [60].
Based on the SEM micrographs in Figure 12, it can be observed that the majority of the voids formed on the bottom side of the roads.This was identified as all of the samples were placed and viewed using the same orientation during SEM imaging.This phenomenon can be attributed to the printing path taken during the fabrication process which is illustrated in Figure 13a.For the layers printed with an infill orientation of 90 degrees, the deposited roads take a shorter printing path compared to layers of 0 degrees.Due to the shorter path, the adjacent roads are of higher temperature when new roads are deposited, thus increasing the time window available for diffusion bonding.At a high printing temperature, the low viscosity molten PLA quickly fills the gaps from previous layers due to gravitational force.Based on the SEM micrographs in Figure 12, it can be observed that the majority of the voids formed on the bottom side of the roads.This was identified as all of the samples were placed and viewed using the same orientation during SEM imaging.This phenomenon can be attributed to the printing path taken during the fabrication process which is illustrated in Figure 13a.For the layers printed with an infill orientation of 90 degrees, the deposited roads take a shorter printing path compared to layers of 0 degrees.Due to the shorter path, the adjacent roads are of higher temperature when new roads are deposited, thus increasing the time window available for diffusion bonding.At a high printing temperature, the low viscosity molten PLA quickly fills the gaps from previous layers due to gravitational force.The shorter path taken for roads printed at 90 degrees results in a greater overlap with roads from the preceding layer, forming smaller voids.This is illustrated between The shorter path taken for roads printed at 90 degrees results in a greater overlap with roads from the preceding layer, forming smaller voids.This is illustrated between layers 2 and 3 in Figure 13b.Furthermore, the higher coalescence temperature also results in a greater reheating effect, which provides a secondary chance for molecular diffusion and randomization across the interface.In contrast, the previous roads would have already cooled down when new roads are deposited for roads printed at 0 degrees.This significantly reduces the time window available for neck growth and molecular diffusion, which causes the roads to fuse less closely together.The formation of voids on the bottom side of the layers is a result of the lack of bonding with preceding layers and is illustrated between layers 1 and 2 in Figure 13b.

Conclusions
This study provides knowledge on how varying the printing temperatures affects FFF fabricated parts both externally and internally.The relationship between printing temperature with dimensional accuracy and tensile properties was established.From the results, it can be concluded that the notable increase in tensile strength is due to better developed physical bonds within the internal geometry.A steady decrease in the average size of voids was observed when the printing temperature was increased.The percentage area of voids reduced by approximately 86% as the printing temperature was increased from 180 • C to 220 • C. On the other hand, T = 220 • C was the optimum printing temperature that yielded the best dimensional accuracy.It was observed that specimens printed below T = 220 • C were smaller than the designed specification while those above T = 220 • C were larger.Based on the results, it is clear that the development of bonds between adjacent and preceding roads is highly dependent on the rheological behavior of PLA, which is a function of temperature.A longer time window for neck growth and polymer diffusion between deposited roads formed stronger bonds.Next, it should also be noted that the tool path taken during printing has a profound effect on the formation of voids.The shorter printing path for layers printed at 90 degrees showed more overlap with roads from adjacent and preceding layers as the coalescence temperature was higher.From this study, it is evident that varying the printing temperature has a profound effect on the quality of bonds formed between the deposited roads.This affects the tensile properties due to the internal geometry of the printed parts and externally in the form of dimensional accuracy and surface finish.The findings from this paper provide a method to alter the mechanical properties by optimizing the printing temperature.

Figure 1 .
Figure 1.(a) Print orientation and (b) dimensions of the specimen according to the ASTM D638-14 Type 1 Standard [66].

Figure 1 .
Figure 1.(a) Print orientation and (b) dimensions of the specimen according to the ASTM D638-14 Type 1 Standard [66].

Figure 2 .
Figure 2. Different locations of measurement for the width (blue marking), length (red marking), and thickness (green marking); dotted lines indicate measured ends.The dimensional accuracy of the parts fabricated at different printing temperatures was examined by comparing the measured length, width, and thickness with the designed specifications.The absolute and dimensional error were calculated as:   (mm) = (  −  )

Figure 2 .
Figure 2. Different locations of measurement for the width (blue marking), length (red marking), and thickness (green marking); dotted lines indicate measured ends.

Figure 3 .
Figure 3. Example of selected regions used to conduct analysis to determine the formation of voids.

Figure 3 .
Figure 3. Example of selected regions used to conduct analysis to determine the formation of voids.

Figure 3 .
Figure 3. Example of selected regions used to conduct analysis to determine the formation of voids.

Figure 4 .
Figure 4. (a) Adjustment of threshold to determine the average size and percentage of void.(b) Binarized form of micrograph.

Figure 4 .
Figure 4. (a) Adjustment of threshold to determine the average size and percentage of void.(b) Binarized form of micrograph.

Figure 7 .
Figure 7. Stress-strain curve at different printing temperatures; values at the end of each curve represent the strain at break.

Figure 8 .
Figure 8. Percentage area of voids and average void size plotted against printing temperature.Figure 8. Percentage area of voids and average void size plotted against printing temperature.

Figure 8 .Figure 9 .
Figure 8. Percentage area of voids and average void size plotted against printing temperature.Figure 8. Percentage area of voids and average void size plotted against printing temperature.J. Manuf.Mater.Process.2024, 8, x FOR PEER REVIEW 11 of 18

Figure 9 .
Figure 9. Ultimate tensile strength and percentage of solid region against printing temperature.

Figure 13 .
Figure 13.(a) Printing path (orange) during the fabrication of specimens.(b) Overlap of deposited roads with the previous layer (circled in red).

Figure 13 .
Figure 13.(a) Printing path (orange) during the fabrication of specimens.(b) Overlap of deposited roads with the previous layer (circled in red).

Table 1 .
Process parameters and settings used in the investigation.
Process ParameterSetting Nozzle printing temperature 180 °C to 260 °C (at intervals of 10 °C)

Table 2 .
Average measured width, length, and thickness of the specimens at different printing temperatures.Optimum printing temperature is labelled with (*).