Interaction Mechanism of Cementitious Composites Containing Different Twisted PVA Fiber Bundles

However, there are few studies in the literature on twisted PVA fiber-reinforced silicate cement-based composites. To implement the fiber-twisting process conveniently and to explore this concept, the reinforcement of through-length twisted fiber bundles is proposed, instead of uniformly distributed short fibers. The flexural properties of construction materials, which include the ability to absorb energy and maintain structural performance during bending behaviors, are of great importance to the ductile properties of structural members [ 20 35 ]. Drawing on these considerations and previous research [ 36 37 ], this paper examines the impact of various twist factors (0, 50, 100, 150 twists per meter) and fiber bundle quantities (1, 2, 3) on the flexural performance of through-length twisted PVA fiber-reinforced cementitious composites (TLTP-FRCCs). To account for the draping effect of PVA fibers and the size requirements of the flexural specimen, a specimen size of 160 × 40 × 15 mm was adopted [ 38 ]. To reduce the test variability, three specimens were fabricated for each test case. Therefore, three-point bending tests were conducted on 36 rectangular specimens to investigate the influence of fiber twisting on the flexural behavior of an FRCC [ 38 ]. Through macroscopic mechanical tests, microscopic observations, and relevant analysis, this study investigates the impact of four twist factors and three bundle numbers on the interaction mechanism of cementitious composites containing different twisted PVA fiber bundles. Additionally, the toughening mechanisms of twisting are revealed. This study recommends the optimal match of these two factors for ductile precast concrete components, among other applications.

Many styles of short steel fibers have been developed to toughen cementitious materials due to their good processability, including fibers with roughened surfaces, round fibers with end paddles/buttons, hooked fibers, and twisted fibers [ 16 30 ]. Karalar et al. discovered a substantial enhancement in bending performance through the incorporation of waste lather scarps, akin to twisted steel fibers, into concrete, as demonstrated in a two-point bending test [ 30 ]. However, PVA fibers are only available in powder form or processed into filament or band form due to their poor processability [ 21 ]. Therefore, it may be possible to use twisted PVA fibers to address the limitations of flat fibers. Twisted fiber-based materials have been widely studied in fields such as textiles, robotics, and medicine for their high efficiency, fast response, scalability, long life, and improved tensile and bending capacity [ 31 33 ]. Haines et al. demonstrated an artificial muscle made of twisted PA6 fiber that can lift over 100 times the weight of human muscle at the same length and weight, owing to its improved tensile and flexural properties [ 32 ].

Due to their high aspect ratio, high ultimate tensile strength, relatively high modulus of elasticity, good chemical compatibility with silicate cement, and lack of health risks, PVA fibers have been widely used in reinforcing cementitious composites [ 21 23 ]. To achieve homogeneous toughening of the specimen, long PVA fibers are typically cut into short bundles of 6–24 mm and uniformly dispersed throughout the matrix [ 24 ]. Noushini et al. examined the dynamic and material properties of an FRCC with varying lengths of short-cut PVA fibers, finding improved mechanical properties but minimal impact on the damping characteristics [ 21 ]. The irregular arrangement of short-cut fibers limits harnessing their high tensile strength, while bundled fibers struggle to form effective bonds with the concrete surface, posing a challenge to exploring material modifications [ 25 ]. As a result, increasing attention has been paid to developing chemical additives to enhance the bonding performance between PVA fibers and the matrix [ 26 27 ]. Cao et al. used calcium carbonate whiskers as chemical additives with PVA and steel fibers to form a new cementitious composite for a bending test [ 26 ]. The CaCOwhiskers were shown to enhance the bonding performance between the fibers and the matrix, providing a crack resistance effect at the microscale. Due to the potential for complex chemical reactions to occur between additives and the cement matrix, resulting in the uncontrollable performance of specimens reinforced with fibers with relevant additives, improving the bonding of PVA fibers to the cement-based matrix from the fibers themselves is a sensible approach.

Silicate cementitious composites are currently the most extensively employed materials in concrete structures, owing to their widespread availability, straightforward preparation, and superior mechanical properties [ 1 2 ]. However, these composites are frequently blended with other materials instead of being utilized independently due to their constrained mechanical properties for practical applications [ 3 5 ]. Fibers such as glass fiber, basalt fiber, forta-ferro fiber, coconut fiber, sisal fiber, steel fiber, and polyvinyl alcohol (PVA) fiber have been effectively used to reinforce silicate cement-based concrete [ 6 13 ]. Ozkilic et al. discovered that incorporating dispersed reinforcement of lightweight expanded clay concrete with coconut fiber and sisal fiber yielded a favorable impact on its mechanical properties, including the compressive strength and bending strength [ 7 ]. Prakash et al. noted that the inclusion of steel fibers in eco-concrete led to a decrease in slump, as well as improvements in the compressive strength, modulus of elasticity, split tensile strength, and flexural strength [ 12 ]. In general, an extensive body of research indicates that fiber-reinforced cementitious composites (FRCCs) showcase enhanced mechanical properties, pseudo-strain hardening behavior, elevated damage tolerance, and heightened cracking resistance [ 14 18 ]. Armed with these superior material properties, there is a growing adoption of FRCCs for application in ductile components [ 19 20 ].

The macroscopic morphology of the fiber bundles at different twist factors is shown in Figure 5 a, where it can be observed that the fiber bundles gradually transformed from flat sheets into spiral shapes with decreasing diameters as the twist factor increased. To examine the morphology of the PVA fiber bundles after the specimens were formed, MXCT was performed using the Nikon XTH320 MXCT facility at Zhejiang University, Hangzhou, China, as shown in Figure 5 b. The scanning parameters used included an exposure time of 500 ms, a voltage of 200 kV, a current of 100 μA, and a scanning accuracy of approximately 30 μm [ 40 ]. Image processing was performed using VGStudio MAX 3.0 software, and 2D slices and 3D solid images were obtained by reconstructing the data from the original MXCT data. To capture the twisted fiber bundle morphology more accurately, specimen B-3-4-2 was selected, which contained three bundles of fibers and a twist factor of 150, for MXCT imaging in this study. The corresponding 3D reconstruction results are shown in Figure 5 c, where it can be seen that the twisted fiber bundles were uniformly tensed in the specimen, and the twisted pattern, even the bubbles, is clearly visible.

To investigate the impact of through-length twisted PVA fiber on the bending capacity of concrete, various types of specimens were prepared for comparison, as outlined in Table 3 . For the purpose of minimizing the test variability, three specimens were produced for each test case. The specimen number indicates the type, for instance, for B-2-1-3, 2 denotes two through-length fiber bundles, 1 denotes the first twisting condition, and 3 denotes the third parallel specimen for that case. The specially designed mold for the test is displayed in Figure 3 ; it could create 12 specimens at once, each measuring 160 × 40 × 15 (mm), and accommodate the arrangement of 0–3 through-length fibers. Additionally, the mold was constructed from nylon and assembled to facilitate mold removal, while also preventing any potential impact of the lubricants on the performance of the specimen. The empty slot in the center of the mold aided in securing and twisting the fibers. The specimen preparation procedure is depicted in Figure 4 . First, the PVA fibers were arranged in the mold according to the working conditions indicated in Table 3 . Second, the dry materials (silicate cement, fly ash, silica fume, and medium sand) were mixed with water in a mixer for five minutes to ensure thorough dispersion. Third, the well-mixed composites were poured into each mold along the edge to avoid altering the position and tension of the fibers. After vibration and smoothing, the surface was covered with cling film to prevent surface cracking caused by moisture evaporation. The specimens were left to cure for two days, after which they had attained the required strength for demolding and could be removed from the mold and placed in the maintenance room for steam curing for 26 days.

To examine the microscopic morphology of the PVA fiber bundle, a bundle of PVA fiber was immobilized using epoxy resin and outer tape and observed with ESEM. The resulting images at two magnification levels are shown in Figure 2 . In Figure 2 a, it can be observed that the diameter of a bundle of the PVA fiber with epoxy resin was approximately 1600 μm. Figure 2 b shows that the cross-section of a single PVA filament was a flat oval shape, and the gaps between the filaments were easily produced. However, a large number of fiber filaments can be coalesced into a whole under the action of epoxy resin.

The main matrix components used in this study, encompassing silicate cement, fly ash, silica fume, and medium sand, were pre-mixed, as illustrated in Figure 1 a. The silicate cement had weight percentages of approximately 2.59%, 1.46%, and 0.019% for SO, MgO, and Cl, respectively, and demonstrated 3-day bending and compressive strengths of around 6.5 MPa and 37 MPa, respectively. The fly ash had a density of about 1.3 g/cmand a total weight percentage of approximately 77% for SiO, Al, and Fe. The silica fume had a weight percentage of roughly 94% for SiO. The medium sand aggregate used had a particle size of 40–70 mesh and a weight percentage of approximately 93.0% for SiO. The long PVA fiber bundles used in this research were manufactured by Sinopec Chongqing SVW Chemical Co., Ltd., Chongqing, China, as depicted in Figure 1 b. Table 1 presents the mechanical properties of the PVA fiber bundle with a slenderness of 2000 dtex/1000f.

This study investigates four twist factors (0, 50, 100, 150) and three bundle numbers (1, 2, 3) to comprehensively analyze the effect of twist factors and fiber bundle numbers on the interaction mechanism of TLTP-FRCC. To examine the PVA fiber bundle used, environmental scanning electron microscopy (ESEM) [ 34 ] was utilized to observe the bundle at a microscopic level. A removable mold made of nylon was designed and produced to meet the requirement for twisting and the size of the flexural specimen. After fabricating the specimens using the aforementioned mold, micro-X-ray computed tomography (MXCT) [ 39 ] was employed to observe the twisted PVA fiber bundle inside the unbent specimen at a micro level, which serves as a reference for comparing with the bent specimens.

The INSTRON-8802 Electron-hydraulic Servo Fatigue Testing Machine (with a maximum applied load of 250 kN) was used to conduct the three-point flexural test on the rectangular specimens under displacement control, with a loading speed of 0.2 mm/min [ 41 ], as depicted in Figure 6 a. To improve the clarity, both the enlarged view of the test setup enclosed in the red box of Figure 6 a and its wireframe diagram are presented in Figure 6 c, revealing that the test specimen dimensions were 160 × 40 × 15 mm, and the clear span was 120 mm. Carbon fiber fabrics and aluminum plates to reinforce the ends of the specimens in this study were used to avoid damage to the ends of the specimens, which would affect the test results, as illustrated in Figure 6 b. The MLONT-F10 Linear Variable Displacement Transducer (LVDT) was utilized to measure the span deflection value of the specimen during the test, with a maximum range of 10 mm and a measurement accuracy of 1‰.

In addition to analyzing the macroscopic tests, this section presents the results of observing the specimens that failed in bending using MXCT as described in Section 2.3 . Due to spatial limitations, this paper presents the MXCT results for the most representative B-3-4-2 specimen, as illustrated in Figure 11 . The top and bottom surfaces of the 3D specimen, obtained through 3D reconstruction of the original MXCT figures, are depicted in Figure 11 a,b. By comparing Figure 11 b with the middle figure in Figure 7 d, it can be observed that the 3D reconstruction accurately reproduced the cracks on the bottom surface of the specimen. In Figure 11 c, it can be observed that the specimen remained intact and the fibers were still under tension even after the specimen failed in bending. To better observe the damage of the PVA fibers, three fibers from the top to bottom were analyzed by increasing the display magnification one by one, and the resulting damage morphology diagrams are shown in Figure 11 d–f. Upon examination of the aforementioned figures, it is apparent that the location of the fiber damage is situated at the cracks in the cementitious composites. This was due to the tensile stress at this location exceeding the allowable tensile stress value of the TLTP-FRCC-based specimen. Additionally, along with the cracking of the concrete, the fiber filaments in the fiber bundle were also pulled off. The fiber damage segment in the yellow box reveals that the fiber damage at the crack was the most significant, and the residual fiber filaments were the least. The fiber filaments gradually increased towards the two longitudinal extensions of the fiber bundle and show a spatially uneven increase mode. The damage to the three fibers shows a gradual increase from bottom to top, which corresponds to the higher shear stress in the upper part of the specimen shown in Figure 11 b, which led to the tilting of the crack.

At the/1000 point, the average load force, equivalent bending stress, and energy consumption of B1, B2, and B3 initially increased, followed by a decrease, and then another increase with the increasing twist factor. At the/600 point, the same trend was observed for B1, B2, and B3, except for the average load force and equivalent bending stress of B3, which increased continually with the increasing twist factor. At the LOP point, the average load force, equivalent bending stress, and energy consumption of B1 and B2 increased as the twist factor increased from 0 to 100, but then decreased as the twist factor increased further. In contrast, for B3, these values continuously increased with the increasing twist factor. The specific values for each index are provided in Table 4 Table 5 and Table 6

Regarding the LOP, deflection tolerance is a crucial evaluation index. As the fiber bundles increased, the T1, T2, and T3 deflection tolerance values at the LOP point decreased, while that of T4 remained constant. The average load force (equivalent bending stress) of the T1 specimens decreased from 0.46 kN (6.10 MPa) to 0.38 kN (5.13 MPa), and T2 and T3 decreased from 0.70 kN (9.37 MPa) and 0.77 kN (10.25 MPa) to 0.46 kN (6.10 MPa) and 0.57 kN (7.59 MPa), respectively. Conversely, the average load force (equivalent bending stress) of T4 increased from 0.60 kN (8.06 MPa) to 0.73 kN (9.77 MPa) as the fiber bundles increased. For the LOP point, the average energy consumption of T1, T2, and T3 decreased with the increase in the fiber bundles, while for T4, the energy consumption capacity increased, as shown in Table 4 Table 5 and Table 6

At the/600 point, the T1 specimens showed a sequential increase in the average load force (equivalent bending stress), ranging from 0.32 kN (4.33 MPa) to 0.33 kN (4.34 MPa) and 0.37 kN (4.88 MPa) with increasing fiber bundles. The average load force (equivalent bending stress) of T2 specimens increased from 0.33 kN (4.40 MPa) to 0.45 kN (6.03 MPa) with increasing fiber bundles before decreasing to 0.41 kN (5.51 MPa). For T3 and T4, the average load force (equivalent bending stress) of the specimens also increased sequentially with increasing fiber bundles, ranging from 0.33 kN (4.39 MPa) to 0.44 kN (5.82 MPa), 0.56 kN (7.49 MPa) to 0.63 kN (8.39 MPa), respectively. Similarly, the average energy consumption of T1, T2, T3, and T4 increased with the increase in the number of fiber bundles at the/600 point, and the specific energy consumption values are shown in Table 4 Table 5 and Table 6

At the/1000 point, the average load force (equivalent bending stress) of the T1 specimens remained almost constant, ranging from 0.15 kN (2.04 MPa) to 0.15 kN (1.99 MPa) as the number of fiber bundles increased, before finally increasing to 0.16 kN (2.20 MPa). The average load force (equivalent bending stress) of the T2, T3, and T4 specimens sequentially increased with the increase in fiber bundles, ranging from 0.20 kN (2.65 MPa) to 0.26 kN (3.47 MPa), 0.15 kN (2.04 MPa) to 0.23 kN (3.07 MPa), and 0.31 kN (4.08 MPa) to 0.32 kN (4.25 MPa), respectively. Additionally, at the/1000 point, the average energy consumption of the T1, T2, T3, and T4 specimens increased with the increase in fiber bundles, with specific energy consumption values shown in Table 4 Table 5 and Table 6

The average load–deflection curves of 1 to 3 fiber bundles at twist factors of 0, 50, 100, and 150 are presented in Figure 9 . The vertical axis represents both the load value and the equivalent bending stress, which was calculated using Equation (1) and is displayed on the right vertical axis. To enhance visibility, Figure 9 includes two vertical reference lines corresponding to/1000 and/600. The specimens could generally withstand deflections ranging from 0.21 to 0.34 mm and loads ranging from 0.38 to 0.77 kN. Due to the low volume fraction of PVA fibers and the absence of coarse aggregates in the TLTP-FRCC-based specimens, bending failure occurred in a manner similar to that of the plain concrete specimens, resulting in load–deflection curves that lack an obvious toughness segment. Instantaneous bending failure to specimen rupture means that only the state change prior to bending failure requires consideration in this paper. To simplify the notation, the twist factors of 0, 50, 100, and 150 are abbreviated as T1, T2, T3, and T4, respectively, while the fiber bundle numbers of 1, 2, and 3 are abbreviated as B1, B2, and B3. The average deflection, load, equivalent bending stress, and energy consumptionof the specimens at the three characteristic points (/1000,/600, and LOP) for the 12 working conditions are presented in Table 4 Table 5 and Table 6 for a better quantitative comparison.

Due to the low fiber volume fraction of fiber-reinforced concrete, its damage mode is similar to that of plain concrete, exhibiting no obvious plastic segment and brittle failure. Based on the load–deflection curves presented in Section 4.2.2 , the critical points for analysis were chosen according to ASTM C1609/C1609M-19a [ 42 ], which included/1000 (0.12 mm),/600 (0.20 mm), and the peak point of each curve. Among these, the point of the maximum load is referred to as the limit of proportionality (LOP) [ 43 ]. The load values at/1000 and/600, as well as at the LOP, are denoted as, and, respectively, while the corresponding deflection values are denoted as, and. According to ASTM C1609/C1609M-19a, the equivalent bending stress at the LOP was calculated using Equation (1) and denoted as. Additionally, the energy consumption up to a certain point on the load–deflection curve is defined as the area under the curve up to that point. When the point is the LOP, the energy consumption is denoted as, and can be calculated using Equation (2). This definition is consistent with the ASTM standard definition for toughness at various points on the load–deflection curve [ 42 ].whererepresents the clear span length,denotes the width of the specimen,represents the height of the specimen, and () denotes a point on the load–deflection curve.

When examining the cross-sections of the specimens without twisting, as shown in Figure 7 a, it is apparent that a majority of the fiber filaments within the fiber bundles were broken at this location, leading to flat fiber bundle sections. However, when the fiber bundles were twisted, the rupture caused the fiber bundle to deconvolute, resulting in an uneven section with fiber filaments of different lengths. This phenomenon is clearly visible in the bending rupture of B-3-4-2, as shown in Figure 8 . As the twist factor increased, there was an increase in the number of filaments with different fiber positions within the same section of a single fiber bundle, as well as an increase in the variation among different fiber positions. This can lead to unevenness in the broken section of the fiber bundle, and longer, more fragmented broken filaments, as depicted in Figure 7 b–d. For specimens containing more than one fiber bundle, the fiber damage pattern was different due to variations in the twist pattern and concrete fracture surface. For instance, in Figure 7 a, B-3-1-1 exhibited an inclined fracture surface, indicating the presence of not only tensile stress but also shear stress. As a result, the lower fiber bundle was not fractured as cleanly as the upper bundle, and some fibers broke at the non-fracture surface. Therefore, the long-broken filaments on the fracture surface are primarily attributable to two factors: the displacement of different filaments within the fiber bundle due to fiber twisting, and the fracture of filaments on the non-fracture surface, often resulting from significant shear stresses. The filament breakage of different fiber bundles within the same specimen is not consistently on one side. As shown in Figure 7 b,d, the filament breakage occurred on one side of the specimen cross-section, while in Figure 7 c, the filament breakage appeared on both sides. Notably, in Figure 7 c, the three fiber bundles exhibited three distinct cases of filament breakage. Specifically, the upper-side fiber bundle experienced partial breakage on the left side of the specimen, the middle-side fiber bundle broke almost completely at the fracture surface, and the lower-side fiber bundle experienced partial breakage on the right side of the specimen.

This type of cement-based specimen, which lacks coarse aggregate and has a low PVA fiber volume fraction, exhibited brittle rupture during the bending tests similar to plain concrete. Due to limited space, Figure 7 presents the bending damage of typical specimens in 12 working conditions. As the load on the top surface of the specimen increased, so did the tensile stress on the cross-section below the neutral axis. Eventually, small cracks began to appear on the bottom surface, indicating that the specimen was losing its bending capacity, as shown in the left figure of Figure 7 . Subsequently, as the loading displacement further increased, the specimen experienced rupture, as depicted in the middle figure of Figure 7 . Moreover, the cross-sectional view resulting from the rupture is presented in the right figure of Figure 7 . The cross-sections of the specimens were highly irregular due to the presence of the through-length PVA fibers, despite the brittle nature of the rupture.

In accordance with the aforementioned treatment, three-point flexural tests were conducted on the specimens sequentially to investigate the impact of the fiber bundle number and the twist factor on the flexural properties of TLTP-FRCC. This study not only examined the macroscopic test phenomena and load–deflection curves for various working conditions but also calculated the equivalent bending stress and flexural failure toughness according to ASTM C1609/C1609M-19a [ 42 ] for a more quantitative comparison. Furthermore, to investigate the toughening mechanism of the through-length twisted PVA fibers during bending failure, MXCT observations were conducted on the bent specimens, and the corresponding analysis is presented in this paper.

5. Discussion

Upon conducting the bending test, it became apparent that this TLTP-FRCC, which lacks coarse aggregates and has a low fiber volume fraction, developed only a single prominent fine crack on the specimen surface at the moment of bending failure. As loading displacement increased, the specimen subsequently fractured directly. Nevertheless, based on the unevenness of the cross-section resulting from the rupture, it can be inferred that the through-length twisted fibers contributed to toughening the composite during the bending test, as the concrete experienced both tensile and shear stresses.

L

/1000 and

L

/600), owing to the increased stiffness of the FRCC and its consequent increased modulus of elasticity [

L

/600 point is very close to the LOP point of a specimen, the effect of the fiber defects caused by insufficient twists will start to affect the

L

/600 state of the specimen. For example, the average load (equivalent bending stress) of B-3-2 was smaller than that of B-2-2 at the

L

/600 point. The LOP point is a key point used to measure the flexural toughness of the specimen, and the absolute values of deflection, equivalent bending stress, and bending energy consumption at the LOP point for the specimens under different working conditions are given in

When the same twist factor was applied to the fibers, and more fiber bundles were introduced, the vertical load and energy consumption increased at relatively small deflections of the specimen (such as the control points at/1000 and/600), owing to the increased stiffness of the FRCC and its consequent increased modulus of elasticity [ 44 ]. However, as the deflection continued to increase and the LOP point of the specimen was reached, the thick fiber bundles (up to 0.8 mm in cross-sectional width without twisting) played a similar role as the initial defect and led to a decrease in the elastic modulus of the specimen, because the relatively smooth fiber bundles did not have a strong enough bond with the cementitious matrix [ 45 ]. As the fiber twist factor increased, the fiber bundle slowly transformed into a spiral, resulting in a decrease in the radius and an increase in the contacted fiber with the cementitious matrix. Simultaneously, the roughness of the contact surface increased. These factors operated in tandem to enhance the bond between the fiber and the matrix, effectively mitigating the slippage effect. After applying the toughening mechanism discussed above, the bending test produced the following results. When the deflection was relatively small, the bonding performance between the fiber and the matrix was not a critical factor, and the specimens with four different twist factors generally exhibited an increasing trend in toughness and modulus of elasticity as the fiber bundle increased. As the deflection value gradually approached the bending tolerance, the requirement for bonding performance significantly increased, and specimens with twist factors of 0, 50, and 100 tended to exhibit decreased toughness and elastic modulus as the fiber bundle increased due to inadequate bonding performance and the fiber resembling the initial defect. However, when the twist factor was increased to 150, this trend was accompanied by an increase in the fiber and matrix bond strength, resulting in a favorable trend of increasing toughness and elastic modulus as the fiber bundle increased. With regard to the deflection values of bending failure, the test results are consistent with the above description, where the value decreased with an increasing number of fiber bundles at low twist factors (0, 50, 100), and at high twist factor equal to 150, the twisting could largely counteract the effect of the defects caused by the fiber bundles. It is worth noting that when the/600 point is very close to the LOP point of a specimen, the effect of the fiber defects caused by insufficient twists will start to affect the/600 state of the specimen. For example, the average load (equivalent bending stress) of B-3-2 was smaller than that of B-2-2 at the/600 point. The LOP point is a key point used to measure the flexural toughness of the specimen, and the absolute values of deflection, equivalent bending stress, and bending energy consumption at the LOP point for the specimens under different working conditions are given in Figure 12 , along with their relative proportions compared to the average values of B-1-1.

To put it in another perspective, the effects of different twist factors with the same number of fiber bundles are discussed further. As mentioned previously, twisted fibers increased the toughness and elastic modulus of the TLTP-FRCC specimens based on the larger contact area and rougher contact surface between the fiber and the matrix. However, since the thickness of a flexural beam is much smaller than its width, a twisted fiber bundle with a large height will instead lead to a significant loss of toughness and elastic modulus. Hence, at the LOP point, specimens with the same number of fiber bundles exhibited an augmentation in the bending capacity and energy consumption capacity as the fiber twist factor increased from 0 to 100. This increase can be attributed to the gradual reduction of the slippage effect. However, when the twist factor reached 150, there was a sharp decrease in the bending and energy consumption capacity of the B1 specimens due to their excessive fiber bundle height. Fortunately, this issue can be solved by increasing the fiber bundles, as cross rows of multiple fibers can enhance the cross-sectional stiffness despite the fiber bundle defects and also consume more energy through filament pulled-off, as shown in Figure 11 . Therefore, as the twist factor reached 150, the decrease in the bending and energy consumption capacity of the B2 specimens slowed down significantly, and the corresponding capacity of the B3 specimens increased even more.

For the cementitious composites used, PVA fiber bundles with 1000 filaments per bundle, oriented along the length of the specimens, had a significant impact on the results due to defects in the transverse and vertical directions caused by their placement in the matrix or by excessive twisting. By considering these negative effects along with the toughening effect of the TLTP fiber bundles, this paper concludes that the best flexural behaviors were obtained for the B-1-3 specimens, considering various factors in general. In the upcoming research, the impact of different filament quantities within a PVA fiber bundle on flexural performance will be examined. These investigations will be tailored to the height of the specimens to accurately determine their influence. Moreover, beam, column, wall, and joint members made of TLTP-FRCC with the best-performing match will be designed to further verify their performance at the structural member level.