As shown in Figure 10, the specimen is a reinforced embedded part with no pegs on the end slab. The test and simulation values of ultimate capacity differed by 10.6%, which is acceptable. The bearing capacity is always controlled by the strength of shear wall concrete because of the same damage pattern between the two. However, the two exhibited a large difference in the displacement curve. In the early loading stage, the elastic modulus of concrete defined in the simulation calculation can rather truly reflect its actual force state under the test loads because the concrete is still in the elastic stage without crack generation and the structural stiffness does not undergo significant change. The displacement curves of the two were well fitted and the slopes were basically identical. However, as the load continued to increase, cracks appeared, broadened, and increased, and the displacement curves shifted and enlarged gradually. In the later stage of loading, the test displacement value was markedly larger than the simulation value due to the continuously increasing crack width, which is approximately three times that of the simulation value when near the limit, showing a large error. Compared to the simulation curve, the test curve exhibited larger platform damage, stronger load sustainability, and better ductility. Nonetheless, from the perspective of the variation regularity of displacement, the two were basically identical in trends.
As shown in Figure 11, the load–displacement curves of specimen SJ165000N basically coincide in the early loading elastic stage, with only small difference in stiffness. However, with the increase of load, the concrete cracked, stiffness degraded, and test and simulation values of displacement showed a rapid difference, which ever enlarged. The cause of difference in displacement at the upper measuring point between the two was because the cracking discontinuity of concrete cannot be preferably simulated with the concrete constitutive model selected in the simulation calculation. Moreover, on the contact surface between the anchor slab and the concrete, the defined bonded slipping constitutive relation differed somewhat from the experimental one. Moreover, the discreteness of concrete material strength itself and the inhomogeneity of medium were the causes of such discrepancy. The simulation values of displacement at the upper and lower measuring points were basically the same, which was quite different from the test case. The effects of the shear deformation of concrete along the axial direction of shear wall, the cracking of concrete to the limit state, and the width of major crack on the increase in the displacement of
As shown in Figure 12, the specimen SJ165000Y is an anchoring reinforced with pegs. In the ABAQUS finite element simulation, the anchoring reinforcing effect of pegs was realized by adding spring elements and defining the stiffness. The two types of values were rather close regarding the ultimate capacity, with a difference of 11.9%, where the test value was higher than the simulation value. In the early loading stage, the two types of displacement values were relatively close, the curves were well fit, and the displacements of embedded parts at the upper and lower measuring points did not differ much. In the later loading period, the differences between the two values began to increase. The curve for simulation value rose basically along the initial slope to the damage platform of structure, the structure cracked, and the influence of stiffness degradation was small. For the test values, the curve gradually flattened out in the later loading stage, the displacement increased rapidly, and the difference between the embedded part displacements at the upper and lower edges also increased gradually, reflecting that the concrete cracking and the embedded part rotation around the geometric center were greatly influential to the displacement growth. The total displacement was nearly twice the simulation value. Clearly, the simulation value was accurate in calculating the bearing capacity, because the damage patterns of the two were basically identical, both of which are controlled by the strength of concrete. By contrast, the difference in displacement was rather large, mainly because the diffusion crack model incorporated in ABAQUS cannot well simulate the actual cracking pattern of concrete. In the later stage of loading, the cracks widened. Their intensive internal distribution greatly affected the pullout displacement of embedded parts, thus resulting in a large displacement difference. Compared with the SJ165000N without pegs, the simulation value of bearing capacity defined by the spring stiffness increased by 15.4%, which reflected the contribution of pegs to the anchorage reinforcement. In addition, the bearing capacity must be calculated by using the simulation method of defining spring elements.