Cyclic Behavior of Steel Frames Equipped with Partial-Connected Crossing-Stiffened Corrugated Steel Plate Shear Walls

Abstract

In order to protect the boundary columns once tension region form on shear walls subjected to seismic loads, a new shear wall system constructed by partial-connected crossing-stiffened corrugated steel plate shear walls (PCCSWs) is proposed and investigated. Numerical modeling of the PCCSWs was conducted and validated by a similar test on single-span two-story corrugated steel plate shear wall test specimen. Some key parameters, such as material properties, height-to-thickness ratio, wave length, and width of the crossing stiffeners, were then investigated through parametric analyses, and the results of PCCSWs were compared to the results of other types of steel shear walls. And a theoretical mechanical model was developed for predicting the ultimate capacity of the PCCSWs taking basis of the parametric results. Several findings can be concluded: (1) The finite element method (FEM) simulates buckling modes and the buckling positions of corrugated steel plates and boundary columns precisely, with the errors of initial stiffness and ultimate shear resistance being less than 10%, which proves the feasibility of the FEM. (2) The optimal values on such key parameters were the height-to-thickness ratio of 510~680 at the center, wave lengths of 360~480 mm, and varying widths of crossing stiffeners which are 64.41~136.89. (3) The relative errors between the theoretical and the numerical results were within 14.17%, and most of the variations were less than 10%, indicating the effectiveness of the developed mechanical model.

1. Introduction

In light of high beginning stiffness, great flexibility, solid seismic resistance, as well as diminishing primary distortions, the steel plate shear wall (SPSW) has been broadly utilized as a horizontal power-opposing framework (LFRS) for medium or elevated structures [1,2,3,4]. Yet, the SPSW easily buckles and has a low capacity to dissipate energy. Additionally, it can create a tension field, resulting in reductions in shearing resistance and lateral stiffness [5,6,7,8].

Under cyclic loading, many scholars often adopt approaches of material enhancement or structural strengthening to address some existing damage problems of structures. Zhang et al. significantly improved the mechanical properties of a new type of enhanced structure by performing CFRP strengthening and UHPC enhancement on the structure [9]. Compared with the non-stiffened SPSW, the diagonal stiffener played a significant role in improving the capacity to dissipate energy, ultimate load-carrying capacity, early stiffness, and ductility [10]. Cheng et al. [11] proposed to reinforce the wall with CFRP to improve the buckling capacity of the shear wall structure and conducted experimental and numerical modeling studies. The results show that the use of CFRP can improve the performance of shear walls. Haddad et al. [12] conducted a study on both stiffened and non-stiffened SPSWs by means of cyclic loading and found that the stiffened SPSWs with cross-shaped stiffeners exhibited a notable enhancement in terms of ductility, energy dissipation capacity, and shear stiffness. Additionally, the quasi-static tests carried out by Mu et al. [13] on two single-span double-story specimens illustrated that the flexural and torsional stiffness of groove stiffeners were fully exploited, thereby significantly enhancing the structure’s load-carrying capacity, stiffness, and resistance to elastic buckling.

The corrugated steel plate shear walls (CSPWs) have attracted more attention compared to the traditional SPSW because the CSPW exhibits excellent ductility, energy dissipation capacity, and shear strength [14,15]. Vaziri et al. [16] carried out numerical analysis on 20 specimens of CSPWs with different geometric parameters, and the findings indicated that CSPWs possessed greater initial stiffness than SPSWs. Ghodratian et al. [17] carried out experimental and numerical investigations on the specimen of double CSPWs (DCSPWs), and results indicated that the DCSPW exhibits excellent load-carrying and energy-dissipating capacity. And Wen et al. [18] carried out numerical simulation and theoretical analysis on DCSPWs and obtained stability analysis curves as well as proposed a bearing capacity design formula under combined shear and compression loads. In addition, adjusting the size of corrugated plates can prevent elastic buckling [19,20,21]. As the height-to-width ratio, number of fastening bolts, and ripple amplitude increase, the ultimate shear resistance of the CSPW also increases. However, to prevent a significant drop in strength after buckling, it is necessary to choose reasonable geometric parameters [22,23,24,25,26]. Further, the tension field is generated by the corrugated steel plate’s linkage to the boundary column; hence, the boundary columns need to possess adequate strength to hold back the extra forces derived from such tension fields [27]. And the beam-only-connected SPSW was proposed to prevent high flexural movement in the boundary columns [28]. Afterwards, Hu et al. [29] investigated a fully precast double-layer CFST/moment resistant frame structure by means of cyclic tests and theoretical analysis. It clearly demonstrated that the beam-connected SPSWs increase the ductility and initial stiffness of these frames. And Nima Paslar et al. [30] conducted an accurate study on the connection between steel plate and boundary frame by establishing 57 calculation models, and the results revealed that the lateral load-carrying capacity of the structure was reduced significantly by the shear wall connected with the beam than that with the boundary column. The test of beam-only-connected SPSWs with composite columns was carried out by Guo et al. [31]. According to their findings, under cyclic loads, SPSWs with buckling-restrained infill plates demonstrated acceptable ductility and steady hysteretic responses.

Although the SPSW structure has been focused on in many experimental and theoretical investigations, the out-of-plane buckling still occurs at the early stage. Therefore, it is necessary to study the stiffened corrugated shear wall steel plate. The asymmetric diagonal stiffened beam-only-connected corrugated steel plate shear wall (ASW) has been proposed by our research group, and the seismic performance of ASW has also been investigated through the test-validated FEM [32]. In order to further investigate the lateral resistance of the stiffened CSPW, this research proposed a different stiffened CSPW called the beam-only-connected CSPW with crossing stiffeners, as shown in Figure 1. Within this design, the corrugated steel plate is connected to the beam by bolts, with the connection realized via intermittent angle steels or fishplates [33], and crossing stiffeners are provided in the corrugated steel plate. This configuration postpones the formation of tension fields and the general buckling of overall wall panels as early as during the early stages in the construction process. In addition, the direct effects demonstrated serve to mitigate out-of-plane buckling in the central area of the plate. As a result, the bearing capability of the beam-only-connected corrugated steel plate shear wall (BCSPW) is improved and the wall becomes more ductile and capable of energy dissipation during an earthquake. In this research, the finite element (FE) model was established and verified by using the 2022 version of ABAQUS software. We investigate the cyclic performance of the PCCSW and estimate whether certain parameters affect the behavior of the structure. Finally, there are commercial vehicle shear resistance formula stakeholders that can be obtained from the computational model. Theoretically derived results are subsequently compared against those obtained from FE analysis, so as to verify the validity of the formula.

2. Numerical Modeling

2.1. Model Description

A single-span double-story PCCSW is selected from a CSPW structure; Figure 1 displays the dimensions of the PCCSW specimen. The column section is H 400 × 400 × 20 × 22 (section height × flange width × web thickness × flange thickness). The bottom-beam and top-beam portions are the same size, H 400 × 300 × 16 × 18. For the middle beam, its dimensions are H 350 × 300 × 14 × 16. The PCCSW is simulated using ABAQUS software, as illustrated in Figure 2a. The CSPW is only coupled to the beam at angles. The boundary stiffeners are welded with CSPWs, while the crossing stiffeners are welded to their outside surface.

To compare the seismic performance of the PCCSW to the BCSPW with boundary stiffeners (BSW) and the unstiffened BCSPW (USW), a BSW and an USW with the same sizes of boundary frames and CSPW are also modeled; these models are illustrated in Figure 2b,c.

These specimens all use vertical trapezoidal corrugated steel plates with a length and width of 3060 mm. The thickness is 4 mm and the slit spacing is 70 mm, as shown in Figure 1. The thickness of boundary stiffeners is 10 mm, and the width is 200 mm; the thickness of crossing stiffeners is 6 mm, and the width is 50 mm. The beam–column joints as well as column base joints use rigid connections.

Table 1. Material properties of structural steel.

Steel Type	σy/MPa	εy	σu/MPa	εu	σst/MPa	εst
E235B	235	0.001	420	0.15	330	0.22
E355B	355	0.002	550	0.116	450	0.17

Note: The σ_y and ε_y are yield strength and yield strain, respectively; the σ_u and ε_u are tensile strength and strain at tensile strength, respectively; the σ_st and ε_st are stress and strain at failure state, respectively.

displays the specific material properties of E235B steel (used for corrugated steel plates and crossing stiffeners) and E355B steel (used for beams, columns, column stiffeners, and boundary stiffeners).

The stiffeners, corrugated steel plates, and boundary frame are all modeled numerically using S4R four-node shell components. Assuming that the steel is an ideal elastic–plastic material, and since a thin steel plate is used, the residual stress induced by welding is not considered. The component size of the frame is 40 mm × 40 mm. Based on mesh sensitivity analysis [34] and convergence analysis [35], and considering both computational accuracy and efficiency, 30 mm × 30 mm is selected as the size of the corrugated steel plate. To accurately and reliably simulate the failure mode and cyclic behavior of the specimen, L/750 of the maximum out-of-plane deformation of the corrugated steel plate is chosen as the initial imperfection and applied to the finite element model [35]. The weld connections in the beams, columns, column stiffeners, and corrugated steel plates are simulated using the “Merge” combination command. Corrugated steel plates are attached to the crossing stiffeners and boundary frames using the “TIE” instruction.

The vertical axial force is applied on the columns to simulate the gravity loads of structures; it is designed as 2000 kN according to the Chinese standard JGJ/99-2015 [36]. Cyclic stress is exerted on the center position of the top beam, while the loading scheme is formulated in line with the Chinese standard JGJ/99-2015 [36].

2.2. Validation of FEM

The finite element model of the PCCSW has not yet been validated by any cyclic experiments. Therefore, this study establishes a refined finite element model of the single-span double-layer CSPW specimen VCoSPSW-I [37] using the same modeling method. The corrugated steel plates and boundary frames are numerically modeled with S4R four-node shell elements. The welded connections among beams, columns, column stiffeners, and corrugated steel plates are simulated using the “merge” assembly command, while the corrugated steel plates are fixedly connected to the boundary frames via the “TIE” command. The same loading scheme is also adopted for the finite element analysis. Finally, it is subjected to comparative verification against the test results of VCoSPSW-1. The test specimen was designed with reduced size; the section size of the top beam and the bottom beam were the same, and they were H 250 × 200 × 12 × 14. The section of the middle beam was H 175 × 175 × 8 × 10, and middle-column section was H 200 × 200 × 8 × 12. The bolt-welded connection was utilized in beam–column joints, and the particulars of the specimen are introduced in Figure 3.

The steel used in the boundary frame and CSPW was Q345 and Q235, respectively. The detailed material properties of specimen VCoSPSW-I are shown in

Table 2. Material properties of VCoSPSW-I [37].

Items	fy/MPa	fst/MPa	δ (%)	fst/fy	E/GPa
Corrugated steel plate	290.59	431.13	21.7	1.48	170.30
Middle-beam web	386.60	551.90	29.4	1.43	196.30
Middle-beam flange	345.27	478.27	27.9	1.39	192.30
Top/bottom-beam flange	418.57	542.73	31.6	1.30	206.70
Top/bottom-beam web	345.60	519.13	32.3	1.50	182.00
Column web	348.38	511.15	32.0	1.47	181.00
Column flange	320.33	494.40	34.2	1.54	203.00

Note: The δ is the elongation after fracture.

.

Figure 4 compares the hysteretic and skeleton curves of FEM analysis and tests.

Table 3. Detailed comparison results between the test and FEM.

Results	Py/kN	△y/mm	Initial Stiffness/(kN/mm)	Pmax/kN	△u/mm
Test	577.30	18.66	30.94	672.80	128.30
FEM	609.34	17.31	35.20	672.94	131.00
Error	5.55%	7.23%	13.77%	0.02%	2.10%

Note: P_y and P_max are the yield load and maximum load, respectively; △_y and △_u are the yield and maximum displacement, respectively.

displays the specific findings. Throughout the loading process, the hysteretic curves of both the test and the finite element model exhibited a full spindle shape. In the later loading stage, the hysteretic curve of the test developed a pinching effect due to the occurrence of obvious out-of-plane deformation of the corrugated steel plate and local tearing of the steel plate. In contrast, the FE model adopted the assumptions of “no slippage or deformation at connections” and “steel as an ideal elastic–plastic material” (modeling settings in Section 2.1 of the manuscript), which prevented such damage and deformation from occurring. As a result, the FE model’s hysteretic curve remained fuller. And errors in initial stiffness and ultimate shear resistance are less than 10%.

At the final loading case, the column flanges and joints were seriously damaged. At the same time, the out-of-plane deformation in the corrugated steel plates was obvious, and some parts of the plates were torn. Figure 5 shows the comparison of failure modes between the test observations and finite element analysis. The finite element method simulates buckling modes and the buckling positions of corrugated steel plates and boundary columns precisely, verifying the reasonableness of the finite element model. It is obvious that the modeling method for the PCCSW in Section 2.1 is sensible, and the method can be utilized for parametric study.

2.3. Comparative Analysis on Seismic Performance

Under cyclic loads, USW, BSW, and PCCSW FE studies are carried out. Figure 6 depicts the skeleton curves and hysteretic curves, while

Table 4. Characteristic results of specimens.

Specimen	Py/kN	△y/mm	Pmax/kN	△u/mm	μ
USW	2052.71	45.21	2354.70	240.33	5.32
BSW	2188.01	47.38	2411.90	225.48	5.15
PCCSW	2281.75	47.81	2670.11	305.08	6.38

Note: μ is ductility factor, and μ = △_u/△_y.

displays the specific data.

At the initial loading stage, there was little difference in the hysteresis loops among the three specimens. After yielding occurred, the energy-dissipating ability of specimen PCCSW was enhanced, with its hysteresis loop growing fuller. During late-stage loading, the steel plate in specimen USW experienced a bearing capacity decrease because of the overall buckling of specimens. In comparison, the bearing capacity of BSW declined earlier due to the out-of-plane buckling of its stiffeners. Notably, specimen PCCSW not only had a more gradual bearing capacity decrease but also exhibited superior ductility.

The maximum load of the PCCSW increased by 13% and 11% compared to the values of USW and BSW, respectively, and the ductility factor increased by 21% and 24%, respectively. Owing to the restraint of out-of-plane buckling deformation by the crossing stiffeners, both the area of the shear-flexural zone and the shear resistance of the PCCSW are increased.

The equivalent viscous damping coefficient h_e can be obtained by Equation (1):

$$h_e={\displaystyle \frac{1}{2\pi }}\times {\displaystyle \frac{S_{(\mathrm{ABC}+\mathrm{ACD})}}{S_{(\mathrm{OBE}+\mathrm{ODF})}}}$$

(1)

where S_(OBE+ODF) is the amount of the areas of ODF and OBE, and S_(ABC+ACD) is the region of the hysteresis circle. The calculation diagram is shown in Figure 7.

Figure 8a,b shows the energy dissipation capacity of the USW, BSW, and PCCSW. The total energy dissipation of the PCCSW increases by 23% and 20% compared to BSW and USW, respectively. The difference in total energy dissipation between USW and BSW is small. The results show that the boundary stiffeners had little effect on total energy dissipation of CSPW, but it is obviously increased by crossing stiffeners.

3. Parametric Analyses of PCCSW

3.1. Design of Parameters

Table 5. Details parameters of parametric analysis.

Series Name	Material Type of Corrugated Steel Plate	t/mm	l/mm	b/mm
PCCSW-M	Variable	4	360	50
PCCSW-T	Q235	Variable	360	50
PCCSW-L	Q235	4	Variable	50
PCCSW-B	Q235	4	360	Variable

Note: t is thickness of corrugated steel plate; l is wave length; b is width of crossing stiffeners.

lists some common parameters that were designed to illustrate how material strength, height–thickness ratio, wave length, and the width of crossing stiffeners influence the seismic performance of the PCCSW. There are four series and a sum of 19 examples in this review. The height of these corrugated steel plates is the same, and the height of the FEM specimen is 45 mm.

The same modeling technique described in Section 2.2 is used to create FEM models of these PCCSWs. The displacement-controlling loading scheme of this parametric study is shown in Figure 9. Before the yield displacement σ_y, the step loading with a 0.2σ_y interval was used, and each level of loading can require two cycles. When reaching the yield displacement σ_y, the step loading with a σ_y interval was used until the specimen was damaged, and each level of loading can require three cycles. The specimens in Table 5 share the same dimensions, material characteristics, boundary, and loading circumstances as the corrugated steel plate and boundary frame. In each series, just one parameter is altered; the others remain constant.

3.2. Effects of Material Strength of PCCSW

There are four varieties of corrugated steel plates with varying material strengths, including LY100, LY160, LY225, and Q235. The stiffeners use Q235 steel for all the specimens in the PCCSW-M series.

Table 6. Parameters of PCCSW-M series [35].

Name	Steel Type	t/mm	E/MPa	fy/MPa	fu/MPa	δ (%)	fy/fu
PCCSW-M1	LY100	4	199,000	128	252	47.3	0.51
PCCSW-M2	LY160	4	194,000	186	294	44.5	0.63
PCCSW-M3	LY225	4	202,500	225	295	44.0	0.65
PCCSW-M4	Q235	4	205,000	235	420	34.0	0.56

Note: t is thickness of corrugated steel plates; E is the elastic modulus; δ is elongation; f_y and f_u are yield strength and tensile strength, respectively.

shows the specific parameters of the PCCSW-M series.

3.2.1. Analysis of Load–Displacement Curves

Figure 10 shows load–displacement curves of the PCCSW-M. With the buckling of the diagonal stiffener, the load-carrying capacity of the specimens diminished differently because of the different material strength of corrugated steel plates. Compared to M1, the ultimate resistance of M2, M3, and M4 increases by 19.8%, 31.3%, and 37.8%, respectively; and the initial stiffness increases by 7%, 7%, and 8%, respectively. The specimen’s ultimate displacement decreased successively with the increase in the strength of the corrugated steel plates, and the ductility coefficient of these specimens changed little. Due to efficient limitation of crossing stiffeners, the corrugated steel plates in these specimens reach their yield strength; thus, the lateral stiffness and ultimate resistance of the PCCSWs are increased by increasing the yield strength of corrugated steel plates.

3.2.2. Analysis of Energy Dissipation

Figure 11 presents a comparison of energy dissipation capacity and the h_e for the PCCSW-M series. Compared to M1, the h_e of M2, M3, and M4 increases by 4.2%, 5.8%, and 7.4%, respectively; the energy dissipation of M2, M3, and M4 increases by 15%, 20%, and 25%, respectively. The low-yield-strength steel works in the earlier plastic stage, so the contribution of crossing stiffeners is not obvious for them. Therefore, under the condition with enough shear resistance, appropriately reducing the strength of the corrugated steel plate could enhance the specimen’s ability to bend plastically and dissipate energy, and the material could be fully used.

3.3. Effects of Height-to-Thickness Ratio of PCCSW

These SPSWs’ width and thickness can be altered to meet the steel boundary frame’s lateral stiffness and resistance requirements [38]. According to different height-to-thickness ratios, five types of corrugated steel plates are designed. Specific parameters of the PCCSW-T series are displayed in

Table 7. Parameters of specimens PCCSW-T.

Serial Number	Steel Type	t/mm	Height-to-Thickness Ratio
PCCSW-T1	Q235	4	765
PCCSW-T2	Q235	4.5	680
PCCSW-T3	Q235	5	610
PCCSW-T4	Q235	6	510
PCCSW-T5	Q235	6.5	470

.

3.3.1. Analysis of Load–Displacement Curves

Figure 12 shows the hysteresis loops for the PCCSW-Ts. The sample moves into the plastic stage earlier as the steel plate thickness increases and the stiffeners’ solidity proportion decreases. Compared to T1, the ultimate resistance of T2, T3, T4, and T5 increases by 9.41%, 13.41%, 29.38%, and 33.65%, respectively; the ductility decreases by 0.25%, 2.55%, 3.62%, and 4.82%, respectively; and the height-to-thickness proportion of the relating steel plate diminishes by 11.11%, 20.1%, 33.3%, and 38.5%, respectively. As the folded steel plate height-to-thickness proportion diminishes, the sidelong stiffness of the example improves steadily. However, there is less flexibility.

3.3.2. Analysis of Energy Dissipation

The correlations between comparable viscous damping coefficient h_e and PCCSW-Ts’ energy scattering are displayed in Figure 13. Compared with T1, the h_e of T2, T3, T4, and T5 increases by 2.07%, 3.25%, 0.30%, and 2.37%, respectively; the energy dissipation of T2, T3, T4, and T5 increases by 12.11%, 4.23%, 5.14%, and 4.23%, respectively. Therefore, the energy dissipation capacity of the structure can be accordingly enhanced by properly reducing the height-to-thickness ratio of corrugated steel plates. And below 510 for the steel plate’s height-to-thickness ratio, the specimen’s ductility, load-bearing capacity, and stiffness decrease rapidly. Therefore, it is recommended that the wave height is 4.5~6 mm, where the equivalent height-to-thickness ratio is 510~680.

3.4. Effects of Wave Length of PCCSW

Several CSPWs with varying wave lengths (360, 400, 480, 520, and 560 mm) are planned in order to focus on how the wave length of the CSPW can affect hysteretic execution. The definite boundaries of PCCSW-Ls are displayed in

Table 8. The dimensions of specimen PCCSW-L.

Serial Number	PCCSW-L1	PCCSW-L2	PCCSW-L3	PCCSW-L4	PCCSW-L5
l/mm	360	400	480	520	560

Note: l is wave length of the steel plate.

.

3.4.1. Analysis of Load–Displacement Curves

The hysteresis loops of the PCCSW-L series are displayed in Figure 14. Compared with L1, the yield loads of L2, L3, L4, and L5 increase by 2.9%, 8.9%, 10%, and 11.3%, individually; the ductility decreases by 7%, 24.8%, 31.44%, and 33.24%, respectively. Increasing the wave length can somewhat increase the ability to support loads, but when the wave length is too long, the stiffener buckles more easily. Having analyzed the results, the ductility is better when the wave length of the specimen is 360~480 mm.

3.4.2. Analysis of Energy Dissipation

The comparisons between the energy dissipation capacity of the PCCSW-L series are displayed in Figure 15. Contrasted with L1, the h_e of L2, L3, L4, and L5 diminishes by 0.84%, 2.06%, 2.82%, and 3.91%, separately, and the energy dissipation diminishes by 0.52%, 8.01%, 8.36%, and 9.41%, individually. Hence, it is recognizable that raising the wave length of the creased steel plate will diminish the energy scattering limit of the example. At the point when the wave length is longer than 480 mm, the pliability diminishes maximally by 32% and the limit of stiffness misfortune is 92.9%. Subsequently, the suggested wave length in this paper is 360~480 mm.

3.5. Effects of Width of Crossing Stiffeners on PCCSW

The most prominent factor affecting the out-of-plane stiffness of inclined stiffeners lies in the variations in their width. β represents the ratio of the flexural rigidity of the stiffener to that of the layered plate, and the computation process are as follows:

$$\beta ={\displaystyle \frac{E{I}_{\mathrm{b}}B}{D_x(h\sin \alpha +B\cos \alpha )}}$$

(2)

$$D_x={\displaystyle \frac{E{t}^3\left[4{(d/t)}^2+1\right]}{6\eta }}$$

(3)

$$I_{\mathrm{b}}={\displaystyle \frac{2b^3{t}_1}{3}};\eta ={\displaystyle \frac{a_1+a_2\cos \theta }{a_1+a_2}}$$

(4)

where the width of layered steel plates and the width of crossing stiffeners are denoted by h, B, and b, respectively; t₁ and t are the thickness of crossing stiffeners and the thickness of corrugated steel plates, respectively; the angle between columns and crossing stiffeners is represented as α; d is the amplitude length of trapezoidal corrugated steel plates; η is the reduction factor of corrugated steel plates; and θ, a₁, a₂ are wave angle, length of horizontal section, and length of wave ridges of corrugated steel plates, as shown in Figure 16.

For the purpose of concentrating on the influence of a range of widths of corner-to-corner stiffeners on the hysteretic performance of structure, five kinds of crossing stiffeners with distinct widths were devised. The specific parameters of specimen PCCSW-B are displayed in

Table 9. Parameters of specimens PCCSW-B.

Serial Number	PCCSW-B1	PCCSW-B2	PCCSW-B3	PCCSW-B4	PCCSW-B5
b/mm	30	50	70	90	110
Stiffness ratio β	5.07	23.47	64.41	136.89	249.94

Note: b is width of crossing stiffeners.

.

3.5.1. Analysis of Load–Displacement Curves

The hysteresis loops of the PCCSW-B series are displayed in Figure 17. Because of the prohibitive impact of crossing stiffeners, expanding the width of stiffeners can further develop the bearing capacity. Compared with B1, the ultimate loads of specimens B2, B3, B4, and B5 increase by 1%, 4%, 5%, and 5%, respectively, and the ductility increases by 9.9%, 9.6%, 10.3%, and 5.6%, respectively. However, compared with B5, the width of stiffener of specimen B4 increases by 20 mm, but the maximum load-carrying capacity increases only by 3.13 kN; the ductility decreases. Properly increasing the width of stiffeners in this manner not only alleviates the out-of-plane buckling of steel plates but also further boosts the bearing capacity and malleability of the specimen.

3.5.2. Analysis of Energy Dissipation

Figure 18 provides comparisons of energy dissipation for the PCCSW-M series with the same thickness. Compared with B1, the h_e of B2, B3, B4, and B5 increases by 0.59%, 0.93%, 0.97%, and 1.89%, respectively; the energy dissipation of B2, B3, B4, and B5 increases by 1.77%, 8.16%, 7.98%, and 8.51%, respectively. Consequently, the ability to consume energy can be marginally improved by increasing the width of crossing stiffeners. The ductility of the specimen will be reduced, as the width of the stiffener is greater than 90 mm or less than 50 mm. Therefore, it is suggested that the width of the stiffener is 50~90 mm and the stiffness ratio of the corresponding stiffener is 64.41~136.89.

4. Calculation Method for Ultimate Shear Resistance

4.1. Theoretical Model of Specimen

When the boundary frame of the PCCSW reaches its maximum lateral resistance, plastic hinges form at the ends of the beams and columns [37,38]. It is estimated that a partial tension field is formed on the BCSPW when it reaches the maximum shear resistance. A mechanical diagram of the PCCSW model is proposed based on the suggestions by Berman and Bruneau [39], and it is presented in Figure 19. The shear resistance of each story of the PCCSW under the proposed mechanical model is calculated by the following [39]:

$${\displaystyle \sum _{i=1}^n{F}_i{H}_i=M_P^f+{\displaystyle \sum _{i=1}^n(V_w^i-V_w^{i+1})H_i}}$$

(5)

where $V_w^i$ is the shear load of the ith-story of the PCCSW, H_i is the height from the ith- story to the ground, and F_i is the shear load of the ith-story.

$M_P^f$ is the plastic second limit of the limit outline. When the bearing capacity of the specimen attains its maximum value, the plastic hinges at the column tops and bottoms fail to form completely. This leads to a certain degree of reduction in the plastic moment capacity. When calculating the second plastic limit of the column, the attenuation coefficient is taken as 0.8 [32]; the calculation is shown in Equation (6).

$$M_P^f=0.8\times 4W_P{f}_y=3.2W_P{f}_y$$

(6)

where W_p and f_y are plastic resistance moment and yield strength of columns, respectively.

The calculation method for the shear resistance of the PCCSW (V_w) is given by Equation (7):

$$V_w=V_C+V_S$$

(7)

where V_C and vs. are shear resistance of CSPW and stiffeners, respectively.

Berman & Bruneau [39] and Clayton [40] established that the SPSWs can be considered as tension fields when determining the ultimate shear capacity; this has been followed by AISC [41]. However, for the beam-only-connected SPSWs, Guo et al. [42], Jiang et al. [33], and Hu et al. [29] laid out a partial tension field model. A mechanical model describing stress distribution was proposed for the PCCSW, with the establishment basis being the partial tension field model; it is shown in Figure 19. The shear-ruled zone and the shear-flexural zone are the two zones that are propounded by the mechanical outline.

The shear resistance V_C is obtained by integrating τ(x), as shown in Equation (8):

$$V_C=t{\displaystyle {\int }_0^B\tau \left(x\right)dx=t(B-B_1){\tau }_y}$$

(8)

where t is the width of the steel plate. In this formula, all parameters, except B_1, are known.

In Figure 20, the normal stress on the shear-flexural zone edge of the corrugated steel plates is denoted by δ_y. The first one deals with normal stress while the second one accounts for shear stress, whereby stress combination in accordance with the von Mises yield equation is given in Equation (11). For stress state, in the shear-dominated zone, τ(x) = τ_y, so that by putting this into Equation (9), δ_y(x) = 0.

$${\delta }_y\left(x\right)=\sqrt{f_y^2-3{\tau }^2(x)}$$

(9)

According to Tan et al. [43], the boundary stiffeners could change the area of the shear-dominated zone by changing the stiffness of them, and the length of B₁ can be decreased accordingly. Once the stiffness of the boundary stiffeners reaches the threshold value in Equation (10) [31], all of the areas of the BCSPW can be estimated as shear-dominated zone, and B₁ = 0 in this situation.

$$A_s\ge {\displaystyle \frac{{\tau }_{y}tH}{2f_{y,s}}}=A_{s,\min }$$

(10)

where H is the corrugated steel plate clear height; A_s is the section area of boundary stiffeners; A_s,min is the threshold section area; and f_y,s is the material yield strength of the boundary stiffeners. The ratio of the section area of the boundary stiffeners to the threshold section area of the boundary stiffeners is defined as ζ, and it can be calculated by the following:

$$\zeta ={\displaystyle \frac{A_s}{A_{s,\min }}}$$

(11)

Based on Figure 20, the equilibrium equation for the edge of the shear-flexural zone can be expressed as Equation (12):

$$(1-\zeta ){\tau }_{y}tH=2{\displaystyle {\int }_0^{B_1}{\delta }_y(x)t_{e}dx}$$

(12)

Shear stresses operating on the inclined plate of the corrugation plate can be canceled out in a direction perpendicular to the inclined plate since the inclined plate is symmetrical. Consequently, B₁ and t continue to represent the shear stress pattern thickness and distribution length, respectively. The equivalent thickness t_e can be found using the following formula, which depends on the equivalent area:

$$t_e={\beta }_{1}t={\displaystyle \frac{a_1+a_2}{a_1+a_2\cos \theta }}t$$

(13)

where a₁, a₂, θ represent the straight plate length, inclined plate length, and wave angle of corrugated plate, respectively, and β₁ represents the conversion coefficient of thickness.

By substituting Equation (9), Equation (11), and f_y = $\sqrt{3}$τ_y into Equation (12), the expression of B₁ can be obtained by the following:

$$B_1={\displaystyle \frac{2\sqrt{3}H(1-\zeta )}{3\pi {\beta }_1}}$$

(14)

V_C can be obtained by the following:

$$V_C=\left\{\begin{array}{cc}t(B-{\displaystyle \frac{2\sqrt{3}H(1-\zeta )}{3\pi {\beta }_1}}){\tau }_y& 0\le \zeta <1\\ tB{\tau }_y& \zeta \ge 1\end{array}\right.$$

(15)

Because the crossing stiffeners are relatively thin elements and can be buckled easily under compressive force, the results of them are not considered in the consequent vs. calculations. Similarly to the calculation of shear resistance of boundary frames, a coefficient of 0.8 is also considered to determine the tensile resistance of the crossing stiffeners, and it can be calculated by the following [44]:

$$V_S=2A_S\times 0.8f_y\cos {\theta }_S=1.6A_S{f}_y\cos {\theta }_S$$

(16)

where the angle between the horizontal direction and the diagonal stiffener is represented as θ_s. A_s is the cross-sectional area of the diagonal stiffener.

Finally, the ultimate shear resistance V_W of the PCCSW can be obtained [44]:

$$V_w=\left\{\begin{array}{cc}t(B-{\displaystyle \frac{2\sqrt{3}H(1-\zeta )}{3\pi {\beta }_1}}){\tau }_y+1.6A_S{f}_y\cos {\theta }_S& 0\le \zeta <1\\ tB{\tau }_y+1.6A_S{f}_y\cos {\theta }_S& \zeta \ge 1\end{array}\right.$$

(17)

4.2. Validation of the Theoretical Method

The first part of the validation is based on the FEM results. Due to the FEM models of this paper being double stories, the parameter n = 2 is thus in Equation (5). In addition, only the top of the second story is subjected to lateral load, where F₁ = 0. Thus, the ultimate shear resistance of the PCCSW in the FE models can be calculated by the following [44]:

$$V=F_2=\left\{\begin{array}{cc}3.2W_P{\displaystyle \frac{f_y}{H_2}}+t(B-{\displaystyle \frac{2\sqrt{3}H(1-\zeta )}{3\pi \beta }}){\tau }_y+1.6A_s{f}_y\cos {\theta }_S& 0\le \zeta <1\\ 3.2W_P{\displaystyle \frac{f_y}{H_2}}+tB{\tau }_y+1.6A_s{f}_y\cos {\theta }_S& \zeta \ge 1\end{array}\right.$$

(18)

The other diameters as well as component performance in terms of material in the FEM models are considered in Equation (18) to obtain the theoretical ultimate shear resistance.

Table 10. Comparisons between ultimate shear resistance of theoretical and FEM results.

Parameters	Type	t/mm	l/mm	b/mm	Theoretical Results/kN	FEM Results/kN	Error
Material	LY100	4	360	50	1991	2141	−7.52%
	LY160				2538	2410	5.01%
	LY225				2585	2580	0.17%
	Q235				2933	2670	8.96%
Thickness of steel plates	Q235	4	360	50	2933	2670	8.96%
		4.5			3152	2892	8.25%
		5			3372	3090	8.36%
		6			3811	3410	10.52%
		6.5			4031	3566	11.53%
Wave length	Q235	4	360	50	2933	2670	8.96%
			400		2843	2776	2.36%
			480		2716	3027	−11.45%
			520		2670	2870	−7.47%
			560		2633	3006	−14.17%
Width of stiffeners	Q235	4	360	30	2885	2652	8.06%
				50	2933	2670	8.96%
				70	2981	2761	7.39%
				90	3029	2770	8.55%
				110	3077	2773	9.88%
						Mean	3.96%
						SD	7.71%

displays the contrast between the theoretical and FEM results for ultimate shear resistance.

The second stage of validation is the test validation. In this paper, seven existing test specimens on the CSPW [43,44,45,46] are used to verify the theoretical model proposed in this paper. And the comparisons between the test results and theoretical results of ultimate shear resistance are summarized in

Table 11. Comparisons between ultimate shear resistance of theoretical and test results.

Specimens		Type	t/mm	l/mm	Column Section/mm	Size of Corrugated Plate/mm	Stiffener Section	Theoretical Result/kN	Test Result/kN	Error
Hao [44]	S-1	Q235	3	160	H200 × 200 × 14 × 16	1800 × 1000	—	1109	1214	−9.44%
	S-2	Q235	3	160	H200 × 200 × 14 × 16	1750 × 1000	—	1083	1059	2.20%
	S-3	Q235	3	160	H200 × 200 × 14 × 16	1200 × 1000	−100 × 10	907	1007	−11.08%
Tan et al [43]	VC-1	Q235	3	120	—	920 × 900	−100 × 10	423	416	1.63%
Li [45]	S-4	Q235	2	150	H200 × 200 × 8 × 12	1100 × 1100	Connected to the column	576	592	−2.67%
Zhao et al [46]	—	Q235	3	160	H200 × 200 × 14 × 16	1750 × 1000	Connected to the column	1083	1100	−1.58%
Zhao et al [46]	VCoSPSW-I	Q235	2	150	H200 × 200 × 8 × 12	1100 × 1100	Connected to the column	588	577	1.90%

.

From the comparative results outlined in Table 10 and Table 11, we can conclude that the ultimate shear resistance forecasted by the theoretical model bears good agreement with both the FEM results and the experimental results. In most theoretical and FEM solutions, error is less than 10%, and the maximum error is 14.17%. The maximum error of data obtained in the experiment relative to the theoretical outcomes is 11.08%, and the majority of them are below 5%. The comparison shows that the proposed theoretical models have acceptable ability for the prediction of the ultimate shear strength of BCSPW and CSPW structures.

5. Conclusions

The partial-connected crossing-stiffened corrugated steel plate shear walls are proposed in this paper. The elastic buckling analysis and hysteretic analysis of the design are performed by using ABAQUS. The conclusion of the paper is as follows:

(1)

A FEM model of a single-span double-story PCCSW was established and was validated by comparing it to test results from a single-span double-story CSPW specimen. The findings demonstrate that the maximum error is less than 10% and that the initial stiffness and ultimate shear resistance as determined by FEM are essentially in agreement with the test results.

(2)

The results analyzed by FEM show that the shear resistance, lateral stiffness, energy dissipation capacity, and ductility of the PCCSW are better than those of the USW and BSW. Compared with the values of the USW and BSW, the maximum load of the PCCSW increases by 13% and 11%, respectively; the ductility factor increases by 21% and 24%, respectively; and the total energy dissipation increases by 23% and 20%, respectively.

(3)

The FEM models show that the material strength, the height-to-thickness ratio, the wave length, and the width of crossing stiffeners can impact the load-carrying capacity of the specimen. The analysis of wave height demonstrates that it ought to be 4.5~6 mm, and the height-to-thickness proportion ought to be 510~680 mm, wave length should be 360~480 mm, and width of crossing stiffeners should be 50~90 mm.

(4)

A theoretical model of the PCCSW is put forward; then, the shear-dominated zone and shear-flexural zone are determined to describe the real state of stress of the PCCSW and thus derive the shear resistance formula of the PCCSW. At the same time, the maximum deviation between theoretical outcomes and FEM outcomes is 14.17%, the maximum deviation between theoretical outcomes and experimental outcomes is 11.08%, and the greater part of them are under 10%. Given the current comparison results and considering the limitation that physical test data remains insufficient, these findings suggest that the proposed theoretical model has the potential to reasonably estimate the ultimate shear resistance of BCSPW and CSPW.