The Inﬂuences of Projectile Material and Environmental Temperature on the High Velocity Impact Behavior of Triaxial Braided Composites

: Two-dimensional (2D) triaxial braided composites with braiding angle ( ± 60 ◦ /0 ◦ ) have been used as aero-engine containing casing material. In the current paper, three types of projectile with the same mass and equivalent diameter, including cylinder gelatin projectile, carbon ﬁber-reinforced plastics (CFRP), and titanium alloy blade-like projectile, were employed to impact on triaxial braided composites panels with thickness of 4.3 mm at room temperature (20 ◦ C) to ﬁgure out the inﬂuences of projectile materials on the damage pattern and energy absorption behavior. Furthermore, the inﬂuences of environmental temperature were also discussed considering the aviation service condition by conducting ballistic impact tests using CFRP projectile at cryogenic temperature ( − 50 ◦ C) and high temperature (150 ◦ C). The triaxial braided target panel were pre-heated or cooled in a low-temperature chamber before mounted. It is found that soft gelatin project mainly causes global deformation of the target and therefore absorb much more energy. The triaxial braided composite absorb 77.59% more energy when impacted with CFRP projectile than that with titanium alloy projectile, which mainly results in shear fracture. The environmental temperature has inﬂuences on the damage pattern and energy absorption of triaxial braided composites. The cryogenic temperature deteriorates the impact resistance of the triaxial braided composite material with matrix cracking damage pattern, while high temperature condition improves its impact resistance with shearing fracture damage pattern. the energy absorbed as a function of impact velocity for various temperatures and the average energy absorbed at three temperatures, respectively. Signiﬁcantly less energy is absorbed by the triaxial braided composite plate at cryogenic temperatures than at room temperature or high temperature. At cryogenic temperatures, the average energy absorbed in cases of target perforation is 189.3 J, which is 22.4% less than at room temperature. The average energy absorbed at high temperature, on the contrary, increases by 13.4% with respect to that at room temperature. These results indicate that low temperature degrades the impact resistance of the two-dimensional triaxial braided composite material, whereas high temperature improves its impact resistance.


Introduction
The fan-containment casings of commercial aero-engines, which is a typical thinwalled structure [1], are typically made of two-dimensional (2D) triaxial braided composite materials [2]. To be certified as airworthy, the fan casing must demonstrate that it can resist the impact due to a blade-out event [3]. The application of braided composite materials in aviation thus requires an in-depth investigation of the failure mechanism of these materials under impact loading [4,5].
Verification in the final stages of structural design usually requires full-scale tests and component-level rig tests, which are extremely expensive and require specialized testing equipment [6,7]. Alternatively, ballistic-impact tests on subscale and full-scale components allow designers to optimize the design of composite structures. Numerous ballistic-impact results have demonstrated that target-panel failure is related to the characteristics of both target and projectile, as well as the impact conditions, including the impact velocity and attitude of the projectile. Previous studies [8] also suggest that, under impact loads, sulfide laminates at 95 and 125 • C. The results reveal that increasing the temperature decreases the stiffness and delamination area and amplifies permanent indentations. Upon increasing the temperature, the failure mechanism transforms from a brittle to a ductile manner. Temperature is closely associated with plastic deformation of the matrix and its coupling with the resin-rich regions and the fiber-bridging mechanism that stems from the specific weave architecture. Khashaba et al. [44] reported that the reduced stiffness and strength is due to softening and plastification of the epoxy matrix, debonding at the fibermatrix interface, and increased interfacial stress in the re-solidified matrix. Amaro [45] investigated how temperature affects the multi-impact performance and reported that the number of impacts to failure depends strongly on the temperature because of the global properties of the matrix.
The effect of low temperature on triaxial braided composites is another rarely studied subject. Sreekantha et al. [46] carried out low-velocity impact experiments on E-glassepoxy composite laminates at both sub-zero and elevated temperatures, and the results indicate that temperature more strongly affects the perforation threshold energy of thicker laminates because of increased laminate rigidity at low temperature. Ma et al. [47] investigated how glass-fiber-reinforced polymer composites respond to low-velocity impact under cryogenic conditions. Finally, Shimamoto et al. [48] performed high-speed impact experiments on CFRP at cryogenic temperatures. However, no studies have yet reported how environmental temperature affects the impact response of triaxial braided composites, which poses a threat to the safety of aero-engines.
From the above analysis, it can be seen that there are still two challenges in the safety research of aero-engine 2D triaxial braided composite casing. First of all, the fly-off blades may be made of composite materials or titanium alloys, and there is no corresponding testing data or analysis on the containment capability of the casing to blades made of completely different materials. Second, the influence of the service environment temperature of the 2D triaxial braided composite casing on its containment capability is still unclear, which threaten the aviation flight safety. The present work uses three types of projectiles, cylindrical gelatin projectiles, CFRP blade-like projectiles, and titanium alloy blade-like projectiles, in ballistic-impact tests to identify the damage pattern and failure modes of 2D triaxial braided composites. These ballistic-impact tests were conducted at both low and high temperatures. We study how projectile material and environmental temperature affects the damage pattern and energy absorption of the composites, which should provide the basic concept to design impact-resistant fan components for aero-engines.

Test Specimen
The composite target was braided with 12k T700 carbon fiber in the form angle of (±60 • /0 • ). Figure 1 shows the process for manufacturing triaxial braid composites: First, a triaxial braider, mounted with the axis horizontal, created a braid tube using 12k flat tow fibers in both the ±60 • (bias) and 0 • (axial) directions (Figure 1a). The tube was then flattened into a double-walled tape ( Figure 1b). Next, the three layers of flattened tapes were piled up with the 0 • fibers aligned. Triaxial braided composite panel was fabricated using the resin-transfer molding technique, whereby epoxy resin was infused into multiple layers of dry braided preform. This transfer molding method has the advantages of good surface finish, dimensional stability, and good mechanical properties [49]. The fiber volume was the same in each direction so that both the individual plies and the entire lay-up were quasi-isotropic. From a large panel, 250 mm × 250 mm composite targets were cut out, each 4.3 mm thick.
As mentioned in the Introduction part, there are three types of projectiles which are commonly used or have potential application for fan blade out events of aero-engine, i.e., cylindrical gelatin projectiles, rectangular titanium alloy projectiles, and composite blade-like projectiles. In the current study, these three projectiles were designed with the same mass. The geometry and dimensions of three types of projectile were shown in Figure 2. The gelatin projectiles were shaped as flat-ended cylinders with 30 mm diameter and 52 mm height. The cylindrical gelatin projectile has a density of 950 kg/m 3 and a porosity of 10%. The CFRP and titanium-alloy projectiles were both rectangular, 70 mm long, and 40 mm wide. Considering the differences in density, the CFRP projectile was 6 mm thick while the titanium-alloy projectile was 2 mm thick. Because the current research is aimed at a specific engine containing casing as the research object, the design of the projectile is based on the engine rotor blades, which is usually a thin sheet with a threedimensional twisted blade shape. Therefore, the thickness of 2 mm of the titanium alloy blade herein is a suitable thickness. The thickness of the CFRP material body is determined based on the density difference between the titanium alloy material and the carbon fiber composite material. The CFRP projectile is a 12-layered woven fabric-reinforced laminate. The rectangular projectiles have the same equivalent diameter as the gelatin cylinder.
were quasi-isotropic. From a large panel, 250 mm × 250 mm composite targets were cut out, each 4.3 mm thick.
As mentioned in the Introduction part, there are three types of projectiles which are commonly used or have potential application for fan blade out events of aero-engine, i.e., cylindrical gelatin projectiles, rectangular titanium alloy projectiles, and composite bladelike projectiles. In the current study, these three projectiles were designed with the same mass. The geometry and dimensions of three types of projectile were shown in Figure 2. The gelatin projectiles were shaped as flat-ended cylinders with 30 mm diameter and 52 mm height. The cylindrical gelatin projectile has a density of 950 kg/m 3 and a porosity of 10%. The CFRP and titanium-alloy projectiles were both rectangular, 70 mm long, and 40 mm wide. Considering the differences in density, the CFRP projectile was 6 mm thick while the titanium-alloy projectile was 2 mm thick. Because the current research is aimed at a specific engine containing casing as the research object, the design of the projectile is based on the engine rotor blades, which is usually a thin sheet with a three-dimensional twisted blade shape. Therefore, the thickness of 2 mm of the titanium alloy blade herein is a suitable thickness. The thickness of the CFRP material body is determined based on the density difference between the titanium alloy material and the carbon fiber composite material. The CFRP projectile is a 12-layered woven fabric-reinforced laminate. The rectangular projectiles have the same equivalent diameter as the gelatin cylinder.

Testing Device
The 65-mm-caliber gas gun used in the ballistic tests accelerated the projectile to a maximum velocity of 200 m/s. Figure 3 shows the principle diagram and structural drawing of this single-stage gas gun. The projectile is supported by foam in an aluminum sabot. The sabot and projectile are pushed and accelerated by compressive air in the gun barrel. The projectile launch velocity is varied by changing the air pressure. The sabot is captured at the exit of the gun barrel by a sabot separator while the projectile moves forward and mass. The geometry and dimensions of three types of projectile were shown in Figure 2. The gelatin projectiles were shaped as flat-ended cylinders with 30 mm diameter and 52 mm height. The cylindrical gelatin projectile has a density of 950 kg/m 3 and a porosity of 10%. The CFRP and titanium-alloy projectiles were both rectangular, 70 mm long, and 40 mm wide. Considering the differences in density, the CFRP projectile was 6 mm thick while the titanium-alloy projectile was 2 mm thick. Because the current research is aimed at a specific engine containing casing as the research object, the design of the projectile is based on the engine rotor blades, which is usually a thin sheet with a three-dimensional twisted blade shape. Therefore, the thickness of 2 mm of the titanium alloy blade herein is a suitable thickness. The thickness of the CFRP material body is determined based on the density difference between the titanium alloy material and the carbon fiber composite material. The CFRP projectile is a 12-layered woven fabric-reinforced laminate. The rectangular projectiles have the same equivalent diameter as the gelatin cylinder.

Testing Device
The 65-mm-caliber gas gun used in the ballistic tests accelerated the projectile to a maximum velocity of 200 m/s. Figure 3 shows the principle diagram and structural drawing of this single-stage gas gun. The projectile is supported by foam in an aluminum sabot. The sabot and projectile are pushed and accelerated by compressive air in the gun barrel. The projectile launch velocity is varied by changing the air pressure. The sabot is captured at the exit of the gun barrel by a sabot separator while the projectile moves forward and

Testing Device
The 65-mm-caliber gas gun used in the ballistic tests accelerated the projectile to a maximum velocity of 200 m/s. Figure 3 shows the principle diagram and structural drawing of this single-stage gas gun. The projectile is supported by foam in an aluminum sabot. The sabot and projectile are pushed and accelerated by compressive air in the gun barrel. The projectile launch velocity is varied by changing the air pressure. The sabot is captured at the exit of the gun barrel by a sabot separator while the projectile moves forward and impacts the target directly. The spallation fragments from the target, projectile with residual velocity, and foam fragments are arrested by the fragment collector mounted on the back of the target. impacts the target directly. The spallation fragments from the target, projectile with residual velocity, and foam fragments are arrested by the fragment collector mounted on the back of the target.
(a) Schematic diagram (b) Gas gun (c) Target Chamber

Testing Methods
The actual projectile impact velocity was measured by a velocimetry system installed between the gun muzzle and the target because it runs independently and has high accuracy. As a projectile passes through the velocimetry system, successive laser beams are obstructed, generating corresponding voltage signals. Given the time interval between two trigger signals and the distance between laser beams in the velocimeter, the velocity is determined. In the actual process, fragments such as foam in the sabot may interfere with the measurement of the velocimeter, so the speed of each test was checked by highspeed photography. Furthermore, the muzzle is very close to the target to reduce the flight distance of the projectile, thereby reducing the speed change and attitude change during the flight of the projectile, so as to improve the test accuracy. Figure 4 shows how the specimens were mounted. Unlike the usual axisymmetric projectile, the blade-like projectile is shaped, making it difficult to control its impact posture. In the present research, the projectile was fixed in an aluminum alloy sabot with four V-shaped grooves at the front edge. When the sabot was captured by the sabot separator, a petal-shaped tear forms and dissipates the kinetic energy of the sabot. The triaxial braided composite plate is fixed along both the short edges using four bolts, leaving the upper and lower edges free. A high-speed camera, MEMRECAM HX-7 (NAC cooperation) is fixed through the bracket above the impact plane to take photos at a frame rate of 3000 frames per second. These high-speed photos are designed to image the target during projectile trajectory and deformation. They also serve to estimate the residual velocity of the projectile for the given perforation conditions.

Testing Methods
The actual projectile impact velocity was measured by a velocimetry system installed between the gun muzzle and the target because it runs independently and has high accuracy. As a projectile passes through the velocimetry system, successive laser beams are obstructed, generating corresponding voltage signals. Given the time interval between two trigger signals and the distance between laser beams in the velocimeter, the velocity is determined. In the actual process, fragments such as foam in the sabot may interfere with the measurement of the velocimeter, so the speed of each test was checked by high-speed photography. Furthermore, the muzzle is very close to the target to reduce the flight distance of the projectile, thereby reducing the speed change and attitude change during the flight of the projectile, so as to improve the test accuracy. Figure 4 shows how the specimens were mounted. Unlike the usual axisymmetric projectile, the blade-like projectile is shaped, making it difficult to control its impact posture. In the present research, the projectile was fixed in an aluminum alloy sabot with four Vshaped grooves at the front edge. When the sabot was captured by the sabot separator, a petal-shaped tear forms and dissipates the kinetic energy of the sabot. The triaxial braided composite plate is fixed along both the short edges using four bolts, leaving the upper and lower edges free. A high-speed camera, MEMRECAM HX-7 (NAC cooperation) is fixed through the bracket above the impact plane to take photos at a frame rate of 3000 frames per second. These high-speed photos are designed to image the target during projectile trajectory and deformation. They also serve to estimate the residual velocity of the projectile for the given perforation conditions.

Testing Methods
The actual projectile impact velocity was measured by a velocimetry system installed between the gun muzzle and the target because it runs independently and has high accuracy. As a projectile passes through the velocimetry system, successive laser beams are obstructed, generating corresponding voltage signals. Given the time interval between two trigger signals and the distance between laser beams in the velocimeter, the velocity is determined. In the actual process, fragments such as foam in the sabot may interfere with the measurement of the velocimeter, so the speed of each test was checked by highspeed photography. Furthermore, the muzzle is very close to the target to reduce the flight distance of the projectile, thereby reducing the speed change and attitude change during the flight of the projectile, so as to improve the test accuracy. Figure 4 shows how the specimens were mounted. Unlike the usual axisymmetric projectile, the blade-like projectile is shaped, making it difficult to control its impact posture. In the present research, the projectile was fixed in an aluminum alloy sabot with four V-shaped grooves at the front edge. When the sabot was captured by the sabot separator, a petal-shaped tear forms and dissipates the kinetic energy of the sabot. The triaxial braided composite plate is fixed along both the short edges using four bolts, leaving the upper and lower edges free. A high-speed camera, MEMRECAM HX-7 (NAC cooperation) is fixed through the bracket above the impact plane to take photos at a frame rate of 3000 frames per second. These high-speed photos are designed to image the target during projectile trajectory and deformation. They also serve to estimate the residual velocity of the projectile for the given perforation conditions. Considering that the triaxial braided composite casing using in aero-engine could be subjected to different ambient temperatures, varying from as high as 100~150 °C to as low Considering that the triaxial braided composite casing using in aero-engine could be subjected to different ambient temperatures, varying from as high as 100~150 • C to as low as −50 • C. To figure out the influences of environmental temperature during service, we also conducted a series of impact tests of a 2D triaxial braided composite target plate at high temperature (150 • C) and cryogenic temperature (−50 • C). For the high-temperature tests, the composite target was heated at 2 • C/min to a predetermined temperature (155 • C) in an electric blast oven, following which the target was thermally insulated for half an hour to allow the homogenization of the internal temperature of the composite target. The heated target was removed from the insulation and immediately installed in the target holder. For the tests at cryogenic temperature, the target was cooled in a low-temperature chamber filled with dry ice (a solid form of carbon dioxide with a sublimation point of −78.5 • C). Dry ice sublimates at normal temperature and pressure, absorbing a large amount of heat from the environment and thereby decreasing the surrounding temperature. The composite target was placed in the cryogenic chamber for 2~3 h and then immediately installed in the target holder. When installing, the bolts are installed with a constant torque wrench with a constant value. Compared with directly on the target plate clamping system, the design of this heating and cooling method could make the clamping pressure of the target plate not change at room temperature, high temperature, and low temperature, thereby exert no interfere with the results. The actual temperature of the target was measured using an infrared thermometer. For both high-and low-temperature tests, the projectile was launched immediately after installing the target in the target holder, and the high-speed camera was triggered to capture images. Table 1 shows the results of high-speed impact tests on 2D triaxial braided composites using different types of projectiles at room temperature (20 • C). In the impact analysis, the ballistic performance is normally measured by energy absorption. Energy absorption of composites is defined as the consumption of kinetic energy of the projectile. For cases that projectiles rebound, it is considered as the total kinetic energy of the projectile is absorbed by fabric targets. According to the initial velocity and residual velocity, the energy absorption of fabrics can be calculated as:

Influence of Projectile Material
in which m denotes the projectile mass, V i denotes the initial velocity of the projectile, and V r denotes the residual velocity of the projectile. Two sets of impact tests were performed with cylindrical gelatin projectiles: one with a projectile velocity of 169 m/s and another with a projectile velocity of 213 m/s. However, even with an impact velocity as high as 213 m/s, the triaxial braided composites were not perforated by the gelatin projectile. On the contrary, the gelatin projectile flows and fragments during impact. We thus deduce that the ballistic-limit velocity is greater than 213 m/s. As the gelatin projectile flow away after impact, the residual velocity could not be obtained, therefore the energy absorption is not available.
Three sets of impact tests were carried out using titanium-alloy blade projectiles and impact velocities ranging from 105 to 160 m/s. In all three sets of tests, the titanium-alloy projectile perforated the target plate, indicating that the ballistic-limit velocity is below 105 m/s for a titanium-alloy projectile.
Six sets of tests were carried out using the CFRP projectiles. In two sets of tests, the projectile rebounded, whereas the projectile perforated the target in the four remaining sets of tests. At impact velocities of 118 and 131 m/s, the target was not perforated, and the CFRP projectile rebounded. At higher impact velocities, 157~172 m/s, the 2D triaxial braided composite targets suffered damages of a similar pattern. The triaxial target is perforated by the CFRP projectile at 157 m/s, but not at 131 m/s, so the ballistic limit is between these two velocities.
Based on this analysis, the triaxial braided composite target plate has significantly different ballistic-limit velocities for the three types of projectiles made of different materials but of similar mass and equivalent diameter. The ballistic-limit velocity of the CFRP, gelatin, and titanium-alloy projectile is between 131 and 157 m/s, above 213 m/s, and below 105 m/s, respectively. The target has the highest ballistic limit for the gelatin projectile, followed by the composite material blade-like projectile, and then by the titanium-alloy metal projectile with the lowest ballistic-limit velocity. Figure 5 shows the energy absorbed by 2D triaxial braided composites as a function of impact velocity, and Figure 6 shows the energy absorbed by the composite target when impacted by projectiles made of various materials. The composite target absorbs the most energy (>612.5 J) when impacted by the gelatin projectile. Because the composite target was not perforated by this projectile at any of the velocities tested, still more energy can be absorbed by this material. When the composite target was impacted with CFRP and titanium-alloy blade-like projectiles, the energy absorption of the composite target first increases and then decreases with increasing impact velocity. When the triaxial braided composite was perforated by a CFRP projectile, the average energy absorbed is 267.1 J, which is 77.59% greater than the maximum average energy absorbed of 150.4 J for a titanium-alloy projectile. According to the study by Anderson Jr. et al. [50], the ballistic limit velocity decreases significantly with the increase in projectile hardness after the projectile hardness exceeds that of the target. In the current study, the composite target and CFRP projectile has moderate hardness while the titanium projectile has obviously greater hardness than the target panel. Therefore, the ballistic limit velocity as well as energy absorption decreases when used titanium alloy projectile. It is worth noting that the previous research on the hardness of the projectile was generally in the field of metal materials. The projectile studied in the current research has a larger material span, ranging from soft gelatin to resin-based composite materials to metal alloy materials.

Impact Process
High-speed cameras were used to record the impact by various types of projectiles on a braided composite target. Figure 7 shows the impact of a gelatin projectile in the Gelatin-2 test. As the impact velocity is extremely high in the tests using gelatin projectile, the gelatin projectile deformed and failed to maintain its original cylindrical geometry. The deformation phenomenon of gelatin projectile was investigated in our recent study [51] and corresponding internally supported gelatin bird projectile were used to improve this undesirable deformation. It is found that the deformed gelatin projectile mainly affects the load characteristic. Considering the flow characteristic of gelatin projectile during impact, the deformation of the gelatin projectile before impact has limited influence on the damage features of the composite target. Therefore, the gelatin projectile could be comparable with other projectile.
The cylindrical gelatin projectile first contacts the target at 1.32 ms and undergoes a significant flow during the impact, which is fully consistent with reports in the literature. The triaxial braided composite target undergoes a large bending deformation under the impact of the gelatin projectile, which absorbs the impact energy to a large extent. Finally, the composite target plate is not perforated by the gelatin projectile, and the target plate recovers completely from the bending deformation. The large bending deformation of the target during impact results in delamination and matrix cracking of the target. Since the gelatin projectile is less hard than the carbon-fiber composite target, the target suffers no significant fiber breakage. For both titanium-alloy and CFRP projectiles, first, the energy absorption increases with the incident velocity, and then, it decreases when the incident velocity exceeds a critical value. This phenomenon is widely observed in ballistic impact, whether it is a metal target plate or a composite material target plate.

Impact Process
High-speed cameras were used to record the impact by various types of projectiles on a braided composite target. Figure 7 shows the impact of a gelatin projectile in the Gelatin-2 test. As the impact velocity is extremely high in the tests using gelatin projectile, the gelatin projectile deformed and failed to maintain its original cylindrical geometry. The deformation phenomenon of gelatin projectile was investigated in our recent study [51] and corresponding internally supported gelatin bird projectile were used to improve this undesirable deformation. It is found that the deformed gelatin projectile mainly affects the load characteristic. Considering the flow characteristic of gelatin projectile during impact, the deformation of the gelatin projectile before impact has limited influence on the damage features of the composite target. Therefore, the gelatin projectile could be comparable with other projectile.  Figure 8 shows the impact of the titanium-alloy projectile perforating a 2D triaxial braided composite target in the Ti-1 test. The projectile is in an ideal posture before hitting the target plate. The contact with the target plate begins at 5.28 ms. At 12.21 ms, about 2/5 of the length of the blade projectile has passed through the target, and, at 21.12 ms, the titanium-alloy projectile completely passes through the target. During the entire impact of the titanium-alloy blade projectile, the target plate undergoes limited bending deformation, which differs significantly from the case for impact by the gelatin projectile. This also explains the concentrated damage inflicted on the target plate and the low energy absorbed. The cylindrical gelatin projectile first contacts the target at 1.32 ms and undergoes a significant flow during the impact, which is fully consistent with reports in the literature. The triaxial braided composite target undergoes a large bending deformation under the impact of the gelatin projectile, which absorbs the impact energy to a large extent. Finally, the composite target plate is not perforated by the gelatin projectile, and the target plate recovers completely from the bending deformation. The large bending deformation of the target during impact results in delamination and matrix cracking of the target. Since the gelatin projectile is less hard than the carbon-fiber composite target, the target suffers no significant fiber breakage. Figure 8 shows the impact of the titanium-alloy projectile perforating a 2D triaxial braided composite target in the Ti-1 test. The projectile is in an ideal posture before hitting the target plate. The contact with the target plate begins at 5.28 ms. At 12.21 ms, about 2/5 of the length of the blade projectile has passed through the target, and, at 21.12 ms, the titanium-alloy projectile completely passes through the target. During the entire impact of the titanium-alloy blade projectile, the target plate undergoes limited bending deformation, which differs significantly from the case for impact by the gelatin projectile. This also explains the concentrated damage inflicted on the target plate and the low energy absorbed.  Figure 8 shows the impact of the titanium-alloy projectile perforating a 2D triaxial braided composite target in the Ti-1 test. The projectile is in an ideal posture before hitting the target plate. The contact with the target plate begins at 5.28 ms. At 12.21 ms, about 2/5 of the length of the blade projectile has passed through the target, and, at 21.12 ms, the titanium-alloy projectile completely passes through the target. During the entire impact of the titanium-alloy blade projectile, the target plate undergoes limited bending deformation, which differs significantly from the case for impact by the gelatin projectile. This also explains the concentrated damage inflicted on the target plate and the low energy absorbed.   Figure 9 shows the process of CFRP projectiles perforating a 2D triaxial braided target in a CFRP-3 test. At 0.42 ms, the CFRP projectile makes initial contact with the target plate, and, at 1.05 ms, it has almost passed through the target plate. The target plate undergoes no obvious bending deformation during the impact, and material is ejected from the back of the target plate due to matrix fragmentation.  Figure 9 shows the process of CFRP projectiles perforating a 2D triaxial braided target in a CFRP-3 test. At 0.42 ms, the CFRP projectile makes initial contact with the target plate, and, at 1.05 ms, it has almost passed through the target plate. The target plate undergoes no obvious bending deformation during the impact, and material is ejected from the back of the target plate due to matrix fragmentation.  Figure 8 shows the impact of the titanium-alloy projectile perforating a 2D triaxial braided composite target in the Ti-1 test. The projectile is in an ideal posture before hitting the target plate. The contact with the target plate begins at 5.28 ms. At 12.21 ms, about 2/5 of the length of the blade projectile has passed through the target, and, at 21.12 ms, the titanium-alloy projectile completely passes through the target. During the entire impact of the titanium-alloy blade projectile, the target plate undergoes limited bending deformation, which differs significantly from the case for impact by the gelatin projectile. This also explains the concentrated damage inflicted on the target plate and the low energy absorbed.   Figure 9 shows the process of CFRP projectiles perforating a 2D triaxial braided target in a CFRP-3 test. At 0.42 ms, the CFRP projectile makes initial contact with the target plate, and, at 1.05 ms, it has almost passed through the target plate. The target plate undergoes no obvious bending deformation during the impact, and material is ejected from the back of the target plate due to matrix fragmentation.

Damage Morphology
The triaxial braided composite target plate suffers no visible damage on the i surface when impacted with a gelatin projectile at an impact velocity of 169 m/s. F

Damage Morphology
The triaxial braided composite target plate suffers no visible damage on the impact surface when impacted with a gelatin projectile at an impact velocity of 169 m/s. Figure 10 shows the morphology of the damage suffered by the target after the impact of the gelatin projectile at an impact velocity of 213 m/s. The impact surface reveals no obvious deformation or fiber breakage. However, delamination, matrix cracking, and a small amount of fiber breakage appears in the through-thickness direction of the target. The damage to the exit surface of the target plate is indicative of matrix cracking at a distance from the impact point. The boundary conditions of the composite panel affect the dynamic response and deformation features of the target panel, correspondingly resulting in different damage patterns. Therefore, if clamping in all edges, it is possible to obtain the results of perforation by the gelatin projectile, as illustrated in literature [24]. deformation or fiber breakage. However, delamination, matrix cracking, and a sm amount of fiber breakage appears in the through-thickness direction of the target. T damage to the exit surface of the target plate is indicative of matrix cracking at a distan from the impact point. The boundary conditions of the composite panel affect the dynam response and deformation features of the target panel, correspondingly resulting in d ferent damage patterns. Therefore, if clamping in all edges, it is possible to obtain the sults of perforation by the gelatin projectile, as illustrated in literature [24].
Although the gelatin projectile did not perforate the target, the existing test resu have fully proved that the energy absorption of the composite material panel is mu higher when impacted with soft gelatin projectile than that with the hard metal and co posite material. The main reason for this result is that, due to the fluid behavior of t gelatin projectile during impact, the contact area with the target plate during impact much larger than the impact area of the metal and composite blade-like projectiles. T target plate undergoes an overall large bending deformation, which dissipates more i pact energy. Consequently, the impact energy is more evenly distributed over the ent target plate.  Figure 11a shows the morphology of the damage suffered by the 2D triaxial braid composite target in the Ti-1 test due to the impact of a titanium-alloy projectile at an i pact velocity of 105 m/s. A significant shear fracture rectangular opening appears on t incident surface, with an area and shape that are substantially the same as the cross-s tional area of the titanium-alloy projectile, which was quite small and thin. On the e surface of the target appears an elliptically bulged area of damage. The damaged ar shows obvious damage modes such as fiber breakage, matrix cracking, or delaminatio as shown in Figure 12. Figure 11b shows the damage of a 2D triaxial braided compos Although the gelatin projectile did not perforate the target, the existing test results have fully proved that the energy absorption of the composite material panel is much higher when impacted with soft gelatin projectile than that with the hard metal and composite material. The main reason for this result is that, due to the fluid behavior of the gelatin projectile during impact, the contact area with the target plate during impact is much larger than the impact area of the metal and composite blade-like projectiles. The target plate undergoes an overall large bending deformation, which dissipates more impact energy. Consequently, the impact energy is more evenly distributed over the entire target plate. Figure 11a shows the morphology of the damage suffered by the 2D triaxial braided composite target in the Ti-1 test due to the impact of a titanium-alloy projectile at an impact velocity of 105 m/s. A significant shear fracture rectangular opening appears on the incident surface, with an area and shape that are substantially the same as the crosssectional area of the titanium-alloy projectile, which was quite small and thin. On the exit surface of the target appears an elliptically bulged area of damage. The damaged area shows obvious damage modes such as fiber breakage, matrix cracking, or delamination, as shown in Figure 12. Figure 11b shows the damage of a 2D triaxial braided composite after impact by a titanium-alloy projectile at an impact velocity of 160 m/s (Ti-3 test). Given that the blade projectile has a certain yaw angle when it exits, an open-type tear occurs on the incident surface of the projectile. The damage on the backside of the target plate is more serious: the damage area is about twice that of the incident-projectile surface, and obvious fiber breakage and delamination have occurred.
The test results show that, for the titanium-alloy projectile perforating the 2D triaxial braided composite target plate, the damage form and damage mode of the target plate are basically the same (i.e., fiber shear fracture and local matrix cracks on the impact surface, and bulged deformation with fiber breakage, fiber pull-out, and delamination). The damage area is smaller. obvious fiber breakage and delamination have occurred.
The test results show that, for the titanium-alloy projectile perforating the 2D triaxial braided composite target plate, the damage form and damage mode of the target plate are basically the same (i.e., fiber shear fracture and local matrix cracks on the impact surface, and bulged deformation with fiber breakage, fiber pull-out, and delamination). The damage area is smaller. Figure 11. Damage to 2D triaxial braided composites impacted by titanium-alloy projectile. In rebound cases, the typical damage caused by the CFRP projectile on the front side of the target is relatively similar. As shown in Figure 13a, projectile impact creates a rectangular sunken area of the same size as the cross-section of the projectile. The sunken area is shallow, with no visible cracking or damage. No visible matrix cracking, bending deformation, or serious delamination appears on the exit surface of the triaxial braided obvious fiber breakage and delamination have occurred.
The test results show that, for the titanium-alloy projectile perforating the 2D triaxial braided composite target plate, the damage form and damage mode of the target plate are basically the same (i.e., fiber shear fracture and local matrix cracks on the impact surface, and bulged deformation with fiber breakage, fiber pull-out, and delamination). The damage area is smaller. Figure 11. Damage to 2D triaxial braided composites impacted by titanium-alloy projectile. In rebound cases, the typical damage caused by the CFRP projectile on the front side of the target is relatively similar. As shown in Figure 13a, projectile impact creates a rectangular sunken area of the same size as the cross-section of the projectile. The sunken area is shallow, with no visible cracking or damage. No visible matrix cracking, bending deformation, or serious delamination appears on the exit surface of the triaxial braided In rebound cases, the typical damage caused by the CFRP projectile on the front side of the target is relatively similar. As shown in Figure 13a, projectile impact creates a rectangular sunken area of the same size as the cross-section of the projectile. The sunken area is shallow, with no visible cracking or damage. No visible matrix cracking, bending deformation, or serious delamination appears on the exit surface of the triaxial braided target. The target plate remains basically intact with no visible damage. Figure 13b shows the damage to a triaxial braided composite target after perforation by a CFRP blade-like projectile with an impact velocity of 157 m/s. The damage area is relatively centralized with a rectangular perforative opening at the impact point. The area of the perforative opening is slightly larger than the cross-section of the CFRP projectile. The damage area on the impact surface surrounds the perforative opening and consists of slight damage and a certain degree of cracking and delamination. At the exit surface, the damage to the braided composite is much more serious and consists of massive fiber breakage, yarn pull-out, severe matrix cracking, and delamination in the bulged broom area.
For perforation with various impact velocities, the morphology of the damage to 2D triaxial braided composite target plate is of a similar pattern, although with a diffe extent of damage. A rectangular opening with an area of shear damage and local m cracking appears on the impact surface. In addition, a local bulge deformation area pears with fiber breakage and delamination, and the main failure modes in the dama area are fiber tensile failure, yarn pull-out, matrix cracking, and delamination. From the analysis above, the target plate absorbs the least energy upon impact o titanium-alloy blade projectile. The main reason for this result is that the titanium-a blade projectile is the hardest of the projectiles and has the smallest cross-sectional for the impact surface. Therefore, when a titanium-alloy projectile impacts the compo target, the target plate is damaged in a shear pattern, which hinders the target pla dissipating energy through a bending deformation. In addition, a shorter projectile-ta interaction time means that the target plate has insufficient time to deform. As a re the damage area of the target plate is also small. For perforation with various impact velocities, the morphology of the damage to the 2D triaxial braided composite target plate is of a similar pattern, although with a different extent of damage. A rectangular opening with an area of shear damage and local matrix cracking appears on the impact surface. In addition, a local bulge deformation area appears with fiber breakage and delamination, and the main failure modes in the damaged area are fiber tensile failure, yarn pull-out, matrix cracking, and delamination.
From the analysis above, the target plate absorbs the least energy upon impact of the titanium-alloy blade projectile. The main reason for this result is that the titanium-alloy blade projectile is the hardest of the projectiles and has the smallest cross-sectional area for the impact surface. Therefore, when a titanium-alloy projectile impacts the composite target, the target plate is damaged in a shear pattern, which hinders the target plate in dissipating energy through a bending deformation. In addition, a shorter projectile-target interaction time means that the target plate has insufficient time to deform. As a result, the damage area of the target plate is also small.

Impact Characteristics under Cryogenic and High Temperatures
Based on the research detailed above, the CFRP projectile produces ballistic impacts on triaxial braided composites at cryogenic and high temperatures that most closely resemble the ballistic impacts in real engines. Table 2 presents the results of ballistic-impact tests at cryogenic and high temperatures, where "C" refers to cryogenic conditions, and "H" refers to high-temperature conditions. At cryogenic temperature, the triaxial braided composite target is perforated at 130 m/s, whereas the projectile rebounds at 131.1 m/s at room temperature. At high temperature, the triaxial braided composite target is perforated at 170 m/s, whereas the projectile rebounds at 146 m/s. Based on these results, we deduce that the ballistic-limit velocity is highest at high temperature, followed by the room temperature and then low temperatures. In other words, cryogenic temperatures decrease the impact resistances of the triaxial braided composites, whereas high temperatures increase their impact resistance. Differences between the impact resistance and forms of damage under these three temperature ranges is discussed in detail below based on the test results.

Energy Absorption
To further study the energy absorption by triaxial braided composite materials due to the impact of CFRP blade projectiles at various temperatures, Figures 14 and 15 show the energy absorbed as a function of impact velocity for various temperatures and the average energy absorbed at three temperatures, respectively. Significantly less energy is absorbed by the triaxial braided composite plate at cryogenic temperatures than at room temperature or high temperature. At cryogenic temperatures, the average energy absorbed in cases of target perforation is 189.3 J, which is 22.4% less than at room temperature. The average energy absorbed at high temperature, on the contrary, increases by 13.4% with respect to that at room temperature. These results indicate that low temperature degrades the impact resistance of the two-dimensional triaxial braided composite material, whereas high temperature improves its impact resistance.

Damage Morphology
With the target plate at cryogenic temperature, three impact tests were undertaken using the composite projectile. The projectile perforated the target plate in tests C2 and C3 (see Table 2), and the projectile rebounded in test C1. Figure 16 shows the damage morphology, where the left-hand images show the damage at the impact surface of the target, and the right-hand images show the damage at the exit surface. The picture at the bottom shows a cross-sectional view of the damage. Figure 16a shows damage caused by test C1, in which the projectile failed to perforate the target. In this case, the projectile caused relatively little damage to the target. Only a slight crater appears due to the shearing action of the projectile at the impact surface, whereas no visible damage appears at the back surface of the target. We deduce from these results that the impact velocity is far below the ballistic limit. When the composite target plate is perforated, a strip opening appears on the incident surface that matches the size of the rectangular projectile. At the exit surface of the target, a wide-ranging, elliptically shaped, broom-like damage area appears, and yarn fracture and delamination are evident. In the C3 test (with a larger incident velocity), more severe crack growth appears at the two ends of the perforation strip, and the damage crack is also significantly larger than that of the C2 test.

Damage Morphology
With the target plate at cryogenic temperature, three impact tests were undertaken using the composite projectile. The projectile perforated the target plate in tests C2 and C3 (see Table 2), and the projectile rebounded in test C1. Figure 16 shows the damage morphology, where the left-hand images show the damage at the impact surface of the target, and the right-hand images show the damage at the exit surface. The picture at the bottom shows a cross-sectional view of the damage. A total of four ballistic-impact tests were performed at high temperature. In tests H3 and H4 (see Table 2), the projectiles perforated the target. Figure 17 shows the damage morphology for tests H2 and H4. In tests H2 (impact velocity of 146 m/s) and H1 (impact velocity of 130 m/s) tests, the projectile failed to perforate the target but rebounded. As for  Figure 16a shows damage caused by test C1, in which the projectile failed to perforate the target. In this case, the projectile caused relatively little damage to the target. Only a slight crater appears due to the shearing action of the projectile at the impact surface, whereas no visible damage appears at the back surface of the target. We deduce from these results that the impact velocity is far below the ballistic limit. When the composite target plate is perforated, a strip opening appears on the incident surface that matches the size of the rectangular projectile. At the exit surface of the target, a wide-ranging, elliptically shaped, broom-like damage area appears, and yarn fracture and delamination are evident. In the C3 test (with a larger incident velocity), more severe crack growth appears at the two ends of the perforation strip, and the damage crack is also significantly larger than that of the C2 test.
A total of four ballistic-impact tests were performed at high temperature. In tests H3 and H4 (see Table 2), the projectiles perforated the target. Figure 17 shows the damage morphology for tests H2 and H4. In tests H2 (impact velocity of 146 m/s) and H1 (impact velocity of 130 m/s) tests, the projectile failed to perforate the target but rebounded. As for the tests under cryogenic conditions, rectangular craters of various depths appear on the impact surface of the target. The crater depth of the H2 target (for a larger impact velocity) significantly exceeds that of the H1 test. Therefore, we consider that, under conditions of rebound, the depth of the impact crater increases with increasing impact velocity. When the target was perforated in tests H3 (impact velocity of 170 m/s) and H4 (impact velocity of 185 m/s), a clear, neat strip perforation was produced on the front surface of the target, corresponding to the shape and size of the projectile, and clear cracking and delamination appeared on the exit surface. In addition, when the projectile impacts the target plate, the projectile itself also suffers fiber breakage and delamination failure.  Extensive yarn fracture and pull-out is evident at the exit surface. The tough fracture surface indicates that the yarn failure is the result of tensile forces. Matrix cracking and delamination failure are also significant failure modes at the target exit surface. Moreover, the extent of damage and the damage area of the target in test C3 are greater than in test Figure 17. Damage to 2D triaxial braided composite target plate at high temperature due to impact of rectangular projectile. Figure 18 shows an enlarged view of the local damage to the composite target at cryogenic and high temperatures. The images on the left (right) show the damage to the front (back) surface of the target. For tests at cryogenic conditions, damage at the impact surface consists of a tear opening with longitudinal and transverse cracks. The main failure modes of the target at the front surface are fiber fracture and matrix cracking. For tests at high temperature, the damage at the impact surface clearly differs from that at cryogenic conditions. A neat and complete rectangular perforation is caused by shearing. The main failure modes in this case are fiber shearing failure and matrix crushing failure.

Conclusions
The current study investigates the ballistic impact performance of 2D triaxial braided composite using three types of projectiles (gelatin cylindrical projectiles and CFRP and titanium-alloy blade-like projectiles) with similar masses and equivalent diameters for the casing containment application. Furthermore, impact tests of triaxial braided composites were conducted at cryogenic and high temperatures considering the possible extreme working environment temperature. The current study aims to illustrate how projectile material and temperature affect the impact resistance of the composites. The main conclusions were drawn as follow: (1) Given the fluid behavior of gelatin projectiles under impact load, the triaxial braided composite target impacted with a gelatin projectile undergoes global deformation and therefore absorbs much more energy than when impacted by CFRP or titanium projectiles. Upon impact with a gelatin projectile, delamination, matrix cracking, and slight fiber breakage appear in the through-thickness direction of the target. (2) Triaxial braided composites impacted by CFRP and titanium-alloy blade-like projectiles produce similar damage patterns. A rectangular opening appears at the impact surface and an elliptically shaped damage area appears at the exit surface with massive fiber breakage, yarn pull-out, and severe matrix cracking and delamination. The average energy absorption of the triaxial braided composite when perforated by a CFRP projectile is 77.59% greater than that perforated by a titanium-alloy projectile. Extensive yarn fracture and pull-out is evident at the exit surface. The tough fracture surface indicates that the yarn failure is the result of tensile forces. Matrix cracking and delamination failure are also significant failure modes at the target exit surface. Moreover, the extent of damage and the damage area of the target in test C3 are greater than in test C2. We presume that, at cryogenic temperatures, a greater incident velocity of the projectile correlates with greater damage and a larger damage area of the composite target plate, which differs from the result for metal blade-like projectiles (cf. Section 3.1.3 and previous studies [32]). For tests at high temperature, the exit surface consists of a rough fiber fracture surface with extensive yarn pull-out. The main failure forms are fiber tensile fracture, matrix cracking, and delamination failure, which is consistent with the results obtained at cryogenic temperature and room temperature.

Conclusions
The current study investigates the ballistic impact performance of 2D triaxial braided composite using three types of projectiles (gelatin cylindrical projectiles and CFRP and titanium-alloy blade-like projectiles) with similar masses and equivalent diameters for the casing containment application. Furthermore, impact tests of triaxial braided composites were conducted at cryogenic and high temperatures considering the possible extreme working environment temperature. The current study aims to illustrate how projectile material and temperature affect the impact resistance of the composites. The main conclusions were drawn as follow: (1) Given the fluid behavior of gelatin projectiles under impact load, the triaxial braided composite target impacted with a gelatin projectile undergoes global deformation and therefore absorbs much more energy than when impacted by CFRP or titanium projectiles. Upon impact with a gelatin projectile, delamination, matrix cracking, and slight fiber breakage appear in the through-thickness direction of the target. (2) Triaxial braided composites impacted by CFRP and titanium-alloy blade-like projectiles produce similar damage patterns. A rectangular opening appears at the impact surface and an elliptically shaped damage area appears at the exit surface with massive fiber breakage, yarn pull-out, and severe matrix cracking and delamination. The average energy absorption of the triaxial braided composite when perforated by a CFRP projectile is 77.59% greater than that perforated by a titanium-alloy projectile. When the composite target is impacted by a titanium-alloy projectile, its main damage has a shear pattern, and barely global bending deformation occurs to dissipate energy. Therefore, the usage of composite fan blades is very important, because compared to titanium alloy blades, the application of composite blades could not only reduce the weight of the blade itself, but also further reduce the weight of the composite casing, which will bring enormous economic benefits. (3) Cryogenic temperatures deteriorate the impact resistance of 2D triaxial braided composite material while high temperature improves its impact resistance. This result is attributed mainly to the decreased flexibility of the 2D triaxial braided composite target plate at cryogenic temperature, which permits less global deformation under impact load. The temperature affects the damage pattern of the 2D triaxial braided composites. Therefore, in the design and analysis of the composite containment casing, it is necessary to consider the influence of the working environment temperature.