Fiber reinforced unsaturated polyester resin with a laminated structure, manufactured in the form of a square pipe by the pultrusion process was used in this study. Details on the square pipe geometry and dimensions are presented in Figure 1. Experimental tests were performed on small specimens cut out from the flat sections of the laminated square pipe. As shown in the figure, the laminated structure consists of the following 5 layers: a combination of a chopped strand mat and screen type mat on the two outside layers, followed by a screen-type mat on the second layers, and unidirectional (UD) fibers oriented along the longitudinal axis of the pipe (0˚ direction) in the inner-most layer.

The bending test pieces were cut out from the square pipe as strips 2.4 mm in thickness, 90 mm in length, and 25 mm in width as shown in Figure 2. Three-point bending tests were performed using an Instron Universal Testing Machine (model 55R4206) at a displacement speed of 2.0 mm/min, span length of 60 mm, at room temperature. For measurement of strain, a strain gauge with a gauge length of 10 mm (KFGS-10-120-C1-11) was used. During the bending tests, the initial damage was also evaluated using the AE method. Using an AE sensor (Nihon Physical Acoustics, Inc., micro-30), the AE measurement threshold was set to 55 dB.

For the observation of fracture in the specimen, a small metallurgical microscope (Olympus, Inc., GX41) was used. In addition, in order to observe the fracture progression, the test was interrupted at displacement intervals of 0.5 mm, and cross-sectional observation at each displacement was conducted.

Tensile specimens were also cut out from the square pipe, with dimensions of 2.4 mm in thickness, 250 mm in length, and 15 mm in width as shown in Figure 3. The tensile tests were performed at a displacement speed of 2.0 mm/min, a grip distance of 150 mm, and at room temperature. The tests were performed using strain gauges and AE sensors, and the initial damage of the material during tensile testing was evaluated. In addition, in order to observe the fracture progression, cross-sectional observations were conducted.

The shape and dimensions of the specimens used for the tensile fatigue tests were the exact same as those for the static tensile tests as shown in the previous section. A Shimadzu Corporation Servo Pulser fatigue testing machine was used (model EHF-ED10) at a frequency of 5 Hz which this value is commonly used in the composite material field [16] [17] . The load waveform was a sine wave, and testing was conducted at room temperature. The load conditions were determined from the tensile test results to investigate the relationship between tensile stress level and fatigue limit tensile stress level. The testing conditions were shown in Table 1. The fatigue properties were evaluated according to the S-N diagram, and the value of cyclic stress that was repeated over 10⁷ times was taken as the fatigue limit.

After the bending tests, final failure occurred on the tensile side and signs of failure on the compression side could not be observed. The bending test results are presented in Table 2, the relationship between the AE amplitude and displacement is shown in Figure 4, the AE energy and displacement are shown in Figure 5, and the relationship between the cumulative AE count number and displacement is shown in Figure 6. Part (a) in each figure shows the corresponding stress-strain diagram taken from a specimen. In the stress-strain diagram shown in (a), stress-strain data from other samples are not included due to broken strain gauges during testing. In (b), the stress-displacement diagram is shown.

From the stress-displacement diagram, a linear relation is observed up to a displacement of 3.0 mm, after which it becomes non-linear until a final fracture occurs. Also, Figure 6(b) shows that in the linear region, as the displacement is increased, the number of AE counts increases only slightly. However, in the non-linear region, the number of AE counts increases significantly. Figure 4 shows amplitude values as high as 95 dB, however, near the end of the test at final failure, the amplitude is as low as 75 dB and does not exceed this value. The resulting energy in Figure 5(b) shows relatively high energy values of 500 μV * sec/count or more immediately after transitioning from the linear region to the non-linear region of the stress-displacement curve. In addition, the maximum energy value occurs at a displacement of 3.5 mm (≒strain 0.011) and stress

value of approximately 265 MPa, regardless of the test piece. It is suggested that at this displacement, a fracture with relatively high energy release such as fiber breakage occurs in the specimen [18] .

Figure 7(a) shows the relationship between amplitude and displacement in the interrupted tests, and Figure 7(b) shows the relationship between energy and displacement. In the previous bending test results, a high energy value of 500 μV * sec/count or more was shown near a displacement of 3.0 mm. In Figure 7, the individual bending stress lines and AE amplitude and energy plots were shown in a different color which indicates the test was performed with each displacement 0.5 mm.

Figure 8 shows the results of cross-sectional observation accompanied by schematic diagrams at displacements of 0 mm, 2.5 mm, 4.0 mm and 6.5 mm. A transverse crack is observed in the fiber bundle oriented in the 90˚ layer at a

displacement of 0 mm. It is considered that this is caused by the difference in curing and shrinkage parameters during the pultrusion process [19] . At a displacement of 2.5 mm, debonding of the mat layer is observed, and transverse cracks can be seen in the fiber bundles oriented at 90˚ in the screen type mat layer.

At a displacement of 4.0 mm, beyond the linear to non-linear transition at a displacement of 3.0 mm, a fracture that resulted in high released energy occurred, as seen by transverse cracking in the 90˚ layers as well as fiber fracture of UD layers. After that, at a displacement of 6.5 mm prior to final failure, both types of fractures developed until the final fracture of fibers in the UD layer bundles.

Since the final breakage was caused by the fracture of fibers in the UD layer, the fiber breakage in the UD layer generated at a displacement of 3.5 mm is considered to be the cause of final destruction. From the above observations, the failure with a high energy value of AE is regarded as the initial fracture in the UD layer. The initial fracture of the UD layer in the bending test occurs at approximately 3.5 mm (a strain of 0.011) at the corresponding stress of approximately 265 MPa. In this case, the initial fracture stress is about 60% of the ultimate strength of the material.

As failure occurred on the tension side of the samples during the bending tests, it is considered that tensile failure contributes to the final failure, therefore tensile properties were examined carefully. Upon observing the fracture appearance following the tensile tests, final fracture of all specimens was characterized by fiber breakage of the UD layer. Tension test results are presented in Table 3, the relationship between the AE amplitude and displacement is shown in Figure 9, the AE energy and displacement are shown in Figure 10, and the relationship between the accumulated AE counts and the displacement is shown in Figure 11.

Part (a) in each figure also shows the corresponding stress-strain diagram. In the stress-strain diagram, linear behavior can be seen until the final fracture. According to Figure 11(b), the cumulative AE count number increases rapidly when the displacement reaches 1.0 mm. Beyond that point, the cumulative number increases gradually, and then the AE count increases at approximately 3.0 mm of displacement. With respect to the sudden increase of the AE count,

Figure 10(b) also shows high energy values over 700 μV * sec/count at 1.0 mm of displacement. At this displacement (a strain of 0.0027) and stress of approximately 100 MPa, the maximum energy values are observed. As in the bending tests, it is suggested that fracture is caused by relatively high energy release events such as fiber breakage that occurred in the test piece at this displacement [18] .

In addition, in order to observe the progress and development of the fracture, cross-sectional observation of the test piece at a displacement of 1.8 mm was conducted. The results of cross-sectional observation of Sample A (before the test) and Sample B (displacement of 1.8 mm) along with a schematic view are presented in Figure 12. According to Figure 12(a), no fracture is observed in the fiber bundles of the UD layer and 90˚ layer before the test. However, at a displacement of 1.8 mm in Figure 12(b), multiple transverse cracks are observed in the fiber bundle oriented at 90˚, and cracks are further observed in the UD layer. This is similar to the bending test observations since the final failure was

caused by the failure of the UD layer. The fiber breakage of the fibers from the UD layer generated at a displacement of 1.0 mm is considered to be the cause of final failure. From this, it is considered that the initial fracture of the UD layer during tensile testing occurred at a displacement of 1.0 mm (strain of 0.0027), at a stress of approximately 100 MPa, with the initial fracture stress being 26% of the ultimate strength.

As a result of observing the progress of the fracture, it was suggested that the initial fracture of the UD layer was the cause of final fracture in both the bending tests and the tension tests. The ratio of the initial fracture stress to final strength was 60% in the bending test, and 26% in the tension test. There is a significant difference between the two values. To further investigate, the strain value during the bending tests was considered.

The strain gauge attachment position of the bending test piece was on the outermost layer of the specimen, on the chopped strand mat layer. Reported strains during testing were measured on this outermost layer. Therefore, using

Equation (1), the corresponding strain on the tensile side of the UD layer on the bending test piece was determined, that is, at the interface between the screen type mat layer and the UD layer. According to the cross-section observation results, the distance from the outermost layer to the interface between the 90˚ layer and the UD layer is approximately 0.62 mm from the intermediate surface.

ε = y / ρ (1)

ε: Strain;

y: displacement from neutral axis;

ρ: curvature radius.

From this result, the radius of curvature at a strain of 0.011 corresponding to high AE energy generation is 108 mm, and the corresponding stress value at this time is approximately 32% of the bending strength. From this, it can be concluded that the initial rupture stress in the UD layer shows similar values in both the bending test and the tension test.

The results of tensile fatigue tests are presented in Table 4 and Figure 13. The S-N diagram shows a linear tendency, and when the cyclic stress is 25% of the tensile strength, the number of cycles exceeds 10⁷ times. From this point, 25% of the maximum strength can be regarded as the fatigue limit. The initial fracture stress during the tension test was 26% of the maximum strength and thus matches with the fatigue limit. This suggests that the fatigue limit obtained from the results of the tensile fatigue test and the initial fracture stress obtained from the tensile test are equivalent. In other words, it is possible to predict the fatigue limit by examining the stress at initial fracture which is the cause of the final failure by the AE method.