3.1 Failure modes
It is apparent that in Figure 6 that these three LFB specimens are all with the typical shear failure modes. In detail, only limited fresh failure surface observed from the coal rejects. A large amount of the obvious separation was found from the interface between the coal rejects and the cementitious grout material, indicating that the interface is the weakest zone for LFB material.
Different from LFB specimens without any confinement, all FPTSS specimens failed by the rupture of exterior FRP composite under hoop tension (see Figures 7a-c). There were some white cracks before the final rupture of FRP jacket associated with the loud noise. After the failure of the exterior FRP jacket, the structural form can still sustain somewhat axial load until the large axial shortening. Without the confinement provided by the FRP jackets, the axial load experiences the sharply decline from the peak load to the low level, which can be found from the axial load-axial shortening curves shown in Figure 7 as well. During this period, the inner PVC tube experience the outward buckling until the large axial shortening. When the exterior FRP-PVC tube was removed, it can be found that there were some cracks observed from the coal rejects.
For FTSS specimen presented in Figure 8, the exterior FRP tube in FTSS specimen experienced a rupture under tension associated with a sudden load shedding event. Whereas, the serve buckling of exterior PVC tube were observed in Figure 9.
3.2 Axial load-axial shortening behaviour
The key results of all tested specimens are listed in Table 1, in which the axial loads of LFB specimens and exterior container averaged from two or three identical specimens were termed as Pinfill and Pexterior, respectively. The peak axial load of FPTSS specimen, PTSS specimen and FTSS specimens was denoted as Ptotal. The axial shortening corresponding to the peak axial load was denoted as Stotal. Pinfill + Pexterior represents the ultimate load of constitute material regardless of the possible difference attributed to the combined effect of different materials. Then, (Ptotal - Pexterior)/ (Pinfill) was adopted to represent the enhancement of load carrying capacity of LFB material with confinement. The axial shortening of LFB specimens corresponding to the peak load Pinfill is denoted as Sinfill, and Stotal/ Sinfill presented in Table 1 indicates the enhancement of ductility of confined LFB material in different specimens.
The axial load-axial shortening curves of unconfined LFB specimens are plotted in Figure 6, in which the axial shortening was averaged from these two LVDT installed on the loading platens of the compression machine. The constant axial load-axial shortening curves of LFB specimens obtained from three identical specimens indicate that the preparation of LFB specimens with non-uniform distributed coal rejects is reliable and reasonable. As mentioned earlier, the axial load will experience the sharply decline due to the development of failure occurred around the interface between the coal reject and cementitious grout material. Once the peak load was reached, the integrity of the material will be significantly affected. It is thus believed that the LFB cannot be directly used as a secondary standing support.
Figures 7 present the compressive behaviour of FPTSS specimens with different thickness of FRP jacket. Compared with these unconfined LFB specimens, all FPTSS specimens achieved a large axial shortening, not only in terms of the axial shortening at the peak axial load, but also the ultimate axial shortening (> 60 mm, equivalent to 30% of the overall height of the specimen).
As shown in Figure 7, the axial load-axial shortening curves of FPTSS specimens can be divided into three portions: (1) ascending part with a bilinear shape; (2) sudden load shedding part with a linear shape; and (3) slight ascending part with minor fluctuations. The transition point between the first portion and the second portion corresponds to the rupture of FRP composite which were observed from the testing procedure. It is not difficulty to explain the specific behaviour of FPTSS specimens under compression. As mentioned above, the FRP-PVC container will not act as the container for ease of construction but also provide confining pressure to infill material. In this case, the infill material is under the tri-axial state and the behaviour of which will be closely related to the confining action of the exterior device. At the beginning of the test, the axial load of FPTSS was initially resisted by the infill material and the exterior FRP-PVC tube. With the increasing lateral expansion of infill material, the confining pressure provided by the FRP-PVC container leads to the ascending prat of the axial load-axial shortening curves. This process will last for a long time until the rupture of the exterior FRP jacket associated with the sudden load shedding. Then, the confining pressure acting on the infill material is mainly from the PVC tube and the residual FRP jacket apart from the ruptured zone. More detailed discussion on the confining action of FRP-PVC container on infill material can be found from the following section.
3.3 Comparison between FPTSS and FTSS specimens
As can be seen from the preparation procedure of the FPTSS specimen, the only difference between FPTSS specimen and FTSS specimen is the former of which contains the additional PVC tube. Therefore, it is believed that the difference between the compressive behaviour of these specimens is mainly attributed to the existence of the PVC tube. To verify the above conclusion, the axial load-axial shortening curves of these specimens are depicted in Figure 8, in which all these specimens had a 3-ply FRP jacket. In addition, the plain LFB specimens without confinement was also plotted in Figure 8 for comparison.
It is apparent that the axial peak loads of FPTSS specimens are higher than that of FTSS specimens, mainly attributed to the additional use of PVC tube in resisting somewhat axial load. As listed in Table 1, the sum of the axial load resisted by the hollow PVC tube and the FTSS is approximately equal to the axial load of FPTSS, which can be regarded as the other evidence to support above assumption.
The other attractive observation obtained from the above comparison is the axial deformation ability of the FPTSS specimen is much superior than its counterparts. As shown in Figure 8, the average axial load of FPTSS specimens is about 125 kN (equal to 50% of the peak load) corresponding to the large axial deformation (i.e. 80 mm). However, the axial deformation of FTSS is only 40 mm when the axial load reduced to 50% of the peak load. This comparative advantage indicates that the effect of the PVC tube is not only increase the axial load carrying capacity but also enhance the axial deformation ability.
3.4 Comparison between FPTSS and PTSS specimens
The axial load-axial curves of FPTSS specimens and PTSS specimens are plotted together in Figure 9 to investigate the effect of FRP jacket on the compressive behaviour of FPTSS specimens. As mentioned above, the only difference between the FPTSS specimens and PTSS specimens herein is the additional FRP jackets. It is thus feasible to obtain the understanding of the contribution provided by the FRP jacket.
It is evident that the peak axial loads of FPTSS specimens are larger than that of corresponding PTSS specimens. As can be seen from Table 1, the peak axial loads of FPTSS specimens are still higher than that of PTSS specimens when the axial load resisted by FRP composite was excluded. This observation suggests that the enhancement of load carrying capacity of FPTSS specimens is attributed to the confining action of exterior FRP jacket. Different from PVC tube, the linear tensile behaviour of FRP jacket will result int the increasing confining action applied on the infill material and the infill material will be under the tri-axial state. If the confining pressure acted on the infill material is large enough, the axial load-axial shortening curves of confined material will be thus in the manner of strain hardening. Even though, the tensile rupture strain of FRP composite is generally smaller than that of these PVC tube. As a result, the axial load of FPTSS will not sustain a high value for a long time. Due to the large rupture strain of PVC tube, the axial load carrying capacity of FPTSS specimen will not decline to an extremely low level after the occurrence of the FRP rupture. In addition, the residual FRP jacket apart from the rupture zone will also provide somewhat confining pressure, resulting in the slightly increasing of the axial load at the large axial shortening.
Different from the obvious enhancement of the load carrying capacity, the effect of the utilization of FRP jacket in enhancing the deformation ability is limited. As seen from Figure 9, there is no significant enlargement of the axial shortening when these two types of structural forms are compared. Because that the rupture strain of FRP jacket is much smaller than that of PVC tube in tension, the large deformation ability of FPTSS specimens is mainly attributed to PVC tube rather than the exterior FRP jacket.