Shock and Vibration
Volume 2018 (2018), Article ID 9632523, 22 pages
https://doi.org/10.1155/2018/9632523

Research Article

Seismic Performance of Base-Isolated Precast Concrete Shear Wall Structure with AHW Connections

Wei Wang,¹ Aiqun Li,2,3 and Xingxing Wang¹

¹School of Architecture and Civil Engineering, Jiangsu University of Science and Technology, 2 Mengxi Road, Zhenjiang 212003, China
²Beijing Advanced Innovation Center for Future Urban Design, Beijing University of Civil Engineering and Architecture, 1 Zhanlanguan Road, Beijing 100044, China
³School of Civil Engineering, Southeast University, 2 Sipailou, Nanjing 210096, China

Correspondence should be addressed to Wei Wang; wangweidimias@sina.com

Received 7 December 2017; Revised 25 February 2018; Accepted 7 March 2018; Published 22 April 2018

Academic Editor: Aly M. Aly

Copyright © 2018 Wei Wang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

To improve the seismic performance and seismic reliability of precast concrete shear wall (PCSW) structure with improved assembly horizontal wall connections (AHW connections), base isolation technology was proposed to be applied in the PCSW structure. Two 1/4-scaled structure models using the improved AHW connections were constructed: a lead-rubber bearing (LRB) base-isolated PCSW structure model and a base-fixed PCSW structure model. Shaking table tests were conducted on these two models with three strong ground motions to assess the seismic performance of the structures. It was found that the improved AHW connections in the base-isolated PCSW structure are useful and effective and that they fulfil the requirements to be met by the connections to withstand an earthquake. In addition, the maximum absolute acceleration and base shear force of the base-isolated PCSW structure model were less than those of the base-fixed PCSW structure model, and the isolation effect on the absolute acceleration responses and base shear responses increased with increase in the intensity of ground motions. In a word, the seismic performance and seismic reliability of PCSW structures can be effectively improved using base isolation technology. After this investigation, the seismic responses of the base-isolated PCSW structure model were numerically simulated using OpenSees software. There was a reasonable agreement between the numerically simulated results and test results; thus, the numerical simulation method and analysis model used for the base-isolated PCSW structure model were verified.

1. Introduction

Cast-in-place concrete shear wall structures (CCSW structures) are widely used throughout the world for their high strength and stiffness. Unlike in the case of CCSW structures, part of the field work can be transferred to the plant in the case of precast concrete shear wall (PCSW) structures; this can save a large amount of labour, reduce material consumption, and shorten the time for construction projects. Thus, PCSW structures can support the development of industrialised construction [1–6].

1.1. Horizontal Connection

Assembly wall connections are the key elements of PCSW structures, which consist of assembly vertical wall connections and assembly horizontal wall connections (AHW connections). Assembly vertical wall connections are normally employed as energy dissipation connections or emulation connections. However, reliable AHW connections can normally guarantee the normal function of the PCSW structures.

There are three methods of assembling the AHW connections in the PCSW structures: (a) splicing longitudinal rebars using sleeves or stirrups combined with high-strength mortar [7–9]; (b) tying together the horizontal connections using unbounded posttensioned (UPT) precast concrete wall plates [2, 10, 11]; (c) connecting the longitudinal rebars using bolted connections [12, 13]. Several studies [1, 8, 11] indicate that the required mechanical properties of the AHW connections can be achieved with the assembly connection methods mentioned above by adopting effective construction measures.

There are some studies on the seismic performance of PCSW structures with UPT connections and sleeve connections combined with high-strength mortar. One such study [5, 6] presents shaking table tests and numerical analysis of the UPT wall structures. The results show that the UPT wall structures exhibit no residual deformation and show minimal damage during an earthquake. Some studies [1, 14] indicate that the seismic performance of the PCSW structure with AHW connection (i.e., longitudinal rebars spliced using sleeves combined with high-strength mortar) and the CCSW structure are similar. However, there has been little investigation on the seismic behaviour of PCSW structures with AHW connection using bolted connections.

1.2. Base Isolation Technology

Seismic isolation is a useful technology to reduce the seismic forces acting on structures. Base-isolated systems are effective because of their excellent energy dissipation characteristics and flexibility. Over the years, many studies have dealt with reliability analysis and reliability-based optimization of base-isolated systems including uncertainties such as isolation device properties and ground motion characteristics [15–17]. The results indicate that base isolation technology can improve the seismic reliability of structures subjected to earthquakes [18–20]. Lead-rubber bearing (LRB) is one of the most useful isolation devices in practice. During an earthquake, the LRBs dissipate most of the input earthquake energy. After the earthquake, because of the recentering capacity of the LRBs, the original position (corresponding to zero deformation) can be restored [21–23]. In recent years, LRBs have been extensively employed in structures to reduce the seismic effects because of their energy dissipation and recentering capacity [24, 25]. In addition, one such study [26] presents sensitivity analysis on mechanical characteristics of LRBs. The results show that the lead core radius is the dominant parameter in affecting LRBs’ performance.

1.3. Scope of Present Study

As base isolation can reduce the seismic forces acting on the structures, the forces acting on the base-isolated structures are less than those on the base-fixed structures; accordingly, the forces acting on the AHW connections in the base-isolated PCSW structures are lower. In other words, the performance of the AHW connections can be improved in the base-isolated PCSW structures. However, there has been little study on the seismic properties of base-isolated PCSW structures with AHW connections.

An improved AHW connection for PCSW structures has been presented in literature [1], and shaking table tests, and numerical simulation have been performed to evaluate the seismic performance of a base-fixed PCSW structure with the improved AHW connections [1]. The tested results indicate that there will be some cracks in the AHW connection area of the PCSW structure with improved AHW connections during server earthquakes. In order to reduce the cracks in the AHW connection area of the PCSW structure, base isolation technology is proposed to be applied in the PCSW structure.

This paper presents the seismic properties of a base-isolated PCSW structure model with the improved AHW connections. To study the seismic performance and energy dissipation capacity of the base-isolated PCSW structures, two 1/4-scaled models of the PCSW structure were built: a base-isolated PCSW structure model and a base-fixed PCSW structure model. Shaking table tests of the two models were conducted, and the absolute acceleration responses and the displacement responses of the base-isolated PCSW structure model were measured to reveal the dynamic properties of the structure. In addition, the seismic behaviour of the improved AHW connections was studied. Finally, the acceleration responses in the fourth storey and shear force-displacement responses in the isolation storey of the base-isolated PCSW structure were numerically simulated using OpenSees software.

2. Improved AHW Connection

The improved AHW connection technology used to realize the horizontal connection of the precast shear wall is shown in Figure 1 [1]. Connection steel plates and bolts are used to make the AHW connection between the lower and upper wall plates. The assembly sequence of the improved AHW connection is as follows.

(a) Elevation

(b) Profile at section A-A

(c) Completed assembly

Figure 1: Improved AHW connection [1].

Weld the longitudinal rebars to their corresponding connection steel plates (see Figure 1(a)).

Before hoisting the precast wall plates, cast a layer of high-strength mortar on the top of the lower wall plate; during the hoisting of the precast wall plates, insert the connection steel plates of the lower wall plate into the reserved channels of the upper wall plate at bottom (see Figure 1(b)).

Adjust the positions of the upper and lower wall plates to align the reserved bolt holes in the connection steel plates and wall plates, insert the bolts in the aligned holes, and tighten the nuts to complete the improved AHW connection (see Figure 1(c)).

3. Description of the Experiment

3.1. Test Specimens

A four-storey base-isolated PCSW structure prototype was designed according to the “code for design of concrete structures” (GB50010-2010) of China [27]. Then, two four-storey 1/4-scaled superstructure models of the base-isolated PCSW structure were constructed. The similitude coefficients of the model are presented in Table 1. One is mounted on four LRBs to form the base isolation model (denoted as Specimen A); the other is bolted to the shaking table to form the base-fixed structure model (denoted as Specimen B). The drawings and images of Specimens A and B are shown in Figure 2 [1]. The scaled model of the superstructure has a dimension of 1400 × 1400 mm in the plan view; the thickness of the shear walls is 35 mm; the height of the storey is 750 mm; and the cross section of the coupling beams is 100 × 100 mm.

Table 1: Similitude coefficients.

Physical quantity
Ratio of similitude

Mass

Length

Elastic modulus

Acceleration

Velocity

Displacement

Volume

Time

Frequency

Force

(a) Plan layout of a standard storey (unit: mm)

(b) Distribution of rebars in Specimen A (unit: mm)

(c) Distribution of rebars in Specimen B (unit: mm)

(d) Images of the installations of Specimens A and B

Figure 2: Test models and drawings.

Ready-mixed concrete was used for casting the structure. The design compressive strength of the concrete was 22 MPa. Table 2 presents the measured mechanical properties of the concrete.

Table 2: Measured mechanical properties of concrete.

Specimen
Cubic compressive strength fcu (MPa)

1st storey
21.63

2nd storey
22.26

3rd storey
22.33

4th storey
21.10

Isolation storey
25.76

Galvanized iron wires of ϕ2.2 were used for the longitudinal rebars and the transverse rebars in the shear walls and for the stirrups of the coupling beams and columns. Galvanized iron wires of ϕ3 were used for the longitudinal rebars of the beams in the -direction. The measured mechanical properties of the galvanized iron wires are presented in Table 3.

Table 3: Measured mechanical properties of galvanized iron wires.

Mechanical properties
Diameter
(mm)
Yield strength
(MPa)
Tensile strength
(MPa)
Elongation
(%)
Elastic modulus
(MPa)

φ2.2
2.2
241.6
330.6
19.7

φ3
3
235.7
319.6
20.2

Three types of connection steel plates were used; their dimensions are shown in Figure 3. The thickness of the steel plates is 3 mm; the diameter of the bolt holes is 8.5 mm; the 3 mm diameter holes are used for connecting the rebars. Figure 4 shows the improved AHW connections, transverse rebars, and longitudinal rebars used in the model.

(a) Connection steel plate 1

(b) Connection steel plate 2

(c) Connection steel plate 3

Figure 3: Connection steel plates.

Figure 4: Construction of precast shear wall plates.

The weights of the base beam, and the wall and floor of each storey are 2.48 t, 0.35 t, and 0.25 t, respectively. Based on the scaling relation, the added mass of each storey is 0.6 t, and accordingly the total weight of the model is 7.06 t. High-strength mortar was used to fix the gravity load trough to the structure.

3.2. LRB

The LRBs were formed by bonding 14 rubber layers and 13 shim layers alternatively (Figure 5). Table 4 summarizes the related parameters of the LRB. The mechanical properties of the LRBs were tested in the previous cyclic loading experiments. Figure 6 depicts the load-deformation curves of the LRB with 100% shear strain and 250% shear strain. It is observed that the lateral stiffness of the LRB shows approximately a bilinear mode.

Table 4: Parameters of LRB.

Scale parameter
Value
Force property parameter
Value

Diameter (mm)
100
Rubber shear modulus (N/mm2)
0.4

Rubber height (mm)
1.5
Equivalent lateral stiffness (kN/mm)
0.24

Total rubber height (mm)
21
Equivalent damping ratio
0.11

Shim height (mm)
4
Post-yielding stiffness (kN/mm)
0.13

Total shim height (mm)
52
Yield displacement (mm)
0.81

Total height (mm)
89
Initial lateral stiffness (kN/mm)
1.21

Diameter of lead (mm)
10

Note. Mechanical parameters of the LRB with 100% shear strain.

Figure 5: Image of LRB.

(a) 100% shear strain

(b) 250% shear strain

Figure 6: Hysteresis curve of LRB.

3.3. Test Procedure and Measurements

The dimension of the shaking table is 4 × 6 m; the maximum acceleration is 1.5 g. During testing, the shaking table was driven in the -direction of the structure model.

Three ground motions were selected: the 1968 Castaic (CA) ground motion, the 1952 Taft (TA) ground motion, and a 2015 artificial (AR) ground motion; these motions are compatible with the response spectrum for soil type II in the “code for seismic design of buildings,” GB 50011-2010 [27]. Figure 7 shows the acceleration time histories corresponding to the three ground motions with 100% PGA scale, and Figure 8 shows the response spectrum curves of the acceleration time histories with a damping ratio of 5% ((peak ground acceleration (PGA) = 400 gal)).

(a) CA1968

(b) AR2015

(c) TA 1952

Figure 7: Acceleration time histories of input ground motions.

Figure 8: Response spectrum curves (damping ratio: 5%) for input ground motions with PGA = 400 gal.

To excite the specimens, ground motions with PGAs of 70 gal, 200 gal, and 400 gal were inputted in the shaking table, corresponding to the intensities of minor earthquakes, moderate earthquakes, and rare earthquakes, respectively, with a seismic fortification intensity of 8 degrees, as mentioned in the “code for seismic design of buildings” (GB50011-2010) [28]. Further, a white-noise ground motion (PGA = 25 gal) in the -direction was inputted in the shaking table to identify the dynamic properties of the specimens. The test sequence is presented in Table 5.

Table 5: Test cases.

Test case
Input excitation
PGA (gal)

Rnd 1
White noise
25

Test 1
CA (1968), TA (1952), AR (2015)
70

Rnd 2
White noise
25

Test 2
CA (1968), TA (1952), AR (2015)
200

Rnd 3
White noise
25

Test 3
CA (1968), TA (1952), AR (2015)
400

Rnd 4
White noise
25

The absolute acceleration and absolute displacements of the storeys of the test models were measured using piezoelectric accelerometers and displacement transducers, respectively.

4. Experimental Results

4.1. Test Phenomenon and Failure Modes

Typical cracks in the specimens are shown in Figure 9. It should be noted that the cracks in the structure model are relatively smaller than the whole structure, and it is difficult to see the crack marks in the whole structure photograph. Hence, the crack distribution in specimens is provided using pictures drawn by software CAD, as depicted in Figures 10 and 11. They reflect the failure modes and seismic properties of the specimens. It can be seen that compared with Specimen B, Specimen A had less cracks in the coupling beams and shear walls, indicating that the isolation system had reduced the crack formation effectively. In addition, there was no crack in the AHW connection area in Specimen A, indicating that the reliability of the improved AHW connection and the safety of the PCSW structure can be ensured during earthquakes.

(a) Cracks in coupling beams

(b) Cracks in shear walls

Figure 9: Typical crack distribution in specimens.

Figure 10: Crack distribution in Specimen A.

Figure 11: Crack distribution in Specimen B.

4.2. Modes

Figure 12 illustrates the first modes of Specimens A and B obtained from the experiment. It is observed that, in the first mode of Specimen A, the isolation storey undergoes deformation but the superstructure behaves as essentially rigid, while the first mode of Specimen B corresponds to a typical flexure type deformation. It can be seen that the modes of Specimens A and B before and after the tests are almost the same.

(a) First modes of Specimen A

(b) First modes of Specimen B

Figure 12: Modes obtained from the experiment. Note. Storey number “0” corresponds to the isolation storey.

4.3. Dynamic Characteristics

The frequencies and damping ratios of the structure models were obtained from the transfer functions, which were derived from the recorded acceleration responses. Figures 13 and 14 show the frequencies and damping ratios of the first modes, respectively, of Specimens A and B. Based on the results, conclusions are made as follows.

Figure 13: Frequency versus PGA.

Figure 14: Damping ratio versus PGA.

With increase in the input PGA, the frequency in the case of Specimen A remains almost constant at approximately 2.2 Hz, whereas in the case of Specimen B, the frequency decreases. When the input PGA is less than 70 gal, the frequency in the case of Specimen B is approximately 16.5 Hz, and when the input PGA is 400 gal, the frequency reduced to 3.12 Hz. It can be inferred that the stiffness of Specimen A is less than that of Specimen B.

With increase in the input PGA, the damping ratio of Specimen A remains almost constant at approximately 16%. When the input PGA is less than 70 gal, the damping ratio of Specimen B is approximately 3.6%, and when the input PGA is 400 gal, the damping ratio increases to 7.54%. Thus, the damping ratio of Specimen A is larger than that of Specimen B.

The frequency and the damping ratio of Specimen A are mainly decided by the LRBs. Because there are no significant changes in the mechanical properties of the LRBs during the tests, there are no remarkable changes in the frequency and damping ratio of Specimen A. However, in the case of Specimen B, the frequency decreases and the damping ratio increases during the tests because of the cumulative damage in this specimen.

4.4. Acceleration Responses

The maximum storey acceleration of Specimens A and B is shown in Figure 15, and the maximum fourth-storey acceleration in all the test stages is displayed in Figure 16. It is clear that the maximum storey acceleration of both Specimens A and B increases when the input PGA increases. In addition, with increase in the input PGA, there is insignificant increase in the maximum storey acceleration of the superstructure of Specimen A; however, there is a significant increase in the maximum storey acceleration of Specimen B.

Figure 15: Acceleration.

Figure 16: Maximum fourth-storey acceleration. Note. Storey number −1 represents the shaking table facility, and 0 represents the base beam.

The equation for the acceleration reduction ratio of the base-isolated structure is as follows:

where is the maximum acceleration of the base-fixed structure and is the maximum acceleration of the base-isolated structure.

Figure 17 depicts the acceleration reduction ratios in the fourth storey of Specimen A. It can be seen that, with the increase in the input PGA from 70 gal to 400 gal, there is an improvement in the reduction effect of acceleration responses. When the input PGA is 70 gal, the acceleration reduction ratio in the fourth storey is approximately 45%, and when input PGA is 400 gal, the ratio increases to approximately 55%. Compared to Specimen B, Specimen A with LRB base isolation system experienced significantly smaller acceleration. This auspicious response of Specimen A in terms of storey acceleration responses as compared to Specimen B is the result of the combined effect of a smaller equivalent lateral stiffness and a higher equivalent damping ratio of the LRBs.

Figure 17: Fourth-storey acceleration reduction ratios. Note. Storey number −1 represents the shaking table facility, and 0 represents the base beam.

4.5. Interstorey Drift (ISD) Responses

The ISD is closely related to structural damage. Figure 18 describes the maximum ISDs of Specimens A and B; Figures 19 and 20 depict the maximum ISDs in the fourth storey and the isolation storey in all the test stages, respectively. It is clear that the maximum ISDs of both specimens increase with the increase in the intensity of ground motion. Further, the maximum ISDs of Specimen A are less than those of Specimen B. For Specimen A, the ISDs in the base-isolated storey are much larger than those in the superstructure.

Figure 18: Maximum ISDs.

Figure 19: Maximum ISDs in the fourth storey.

Figure 20: Maximum ISDs in the isolation storey.

The equation for the ISD reduction ratio of the base-isolated structure is as follows:

where is the maximum ISD of the base-fixed structure and is the maximum ISD of the base-isolated structure.

Figure 21 depicts the ISD reduction ratios in the fourth storey. It can be seen that the ISD reduction ratios increase with increase in the input PGA. When the input PGA is 70 gal, the ISD isolation ratio in the fourth storey is approximately 35%, and when the input PGA is 400 gal, the ISD isolation ratio increases to approximately 60%. The present LRB base isolation system reduces the ISDs to a great extent when subjected to ground motions with various PGA levels. This demonstrates the capability of the LRB base isolation system in protecting the PCSW structure against earthquakes.

Figure 21: ISD reduction ratios in the fourth storey.

4.6. Interstorey Shear Force (ISSF) Responses

Figure 22 shows the maximum ISSFs in Specimens A and B when subjected to ground motions with PGAs of 70 gal, 220 gal, and 400 gal. Figure 23 displays the maximum ISSFs of the first storey in the specimens in all the test stages. It can be seen that the maximum ISSFs in both specimens increase with the increase in the intensity of ground motions. The maximum ISSFs of Specimen A are less than those of Specimen B.

Figure 22: Maximum ISSFs.

Figure 23: ISSFs of first storey.

The equation for the ISSF reduction ratio of the base-isolated structure is as follows:

where is the ISSF of the base-fixed structure and is the ISSF of the base-isolated structure.

The ISSF reduction ratios of the first storey in Specimen A are shown in Figure 24. It can be observed that, with increase in the input PGA, the ISSF reduction ratios in the first storey increase. When the input PGA is 70 gal, the ISSF reduction ratio in the first storey is approximately 25%, and when the input PGAs are low, the ISSF reduction effect of the LRB is not significant. With increase in the input PGA, Specimen A exhibited better ISSF reduction capacity. When the input PGA is 400 gal, the ISSF reduction ratio of the first storey increases to approximately 50%. In the case of a minor earthquake, the lateral stiffness of the LRB is relatively high, and the ISSF reduction effect is not significant. In the case of severe earthquakes, the equivalent lateral stiffness of the LRB decreases, and the ISSF reduction effect improves.

Figure 24: ISSF reduction ratios of first storey.

4.7. Energy Dissipation Property of Isolation Storey

Figure 25 shows the shear force-displacement hysteresis curves of the isolation storey in Specimen A, when subjected to input excitations with PGAs of 70 gal, 220 gal, and 400 gal. The dissipation energies of the isolation storey in all the test stages are shown in Figure 26. It can be seen that the shear force-displacement hysteresis curves of the isolation storey are spindle-shaped; this demonstrates the satisfactory energy dissipation property of the LRBs.

(a) CA1968

(b) AR2015

(c) TA1952

Figure 25: Shear force-displacement hysteresis curves of the isolation system.

Figure 26: Dissipation energy of the isolation storey.

5. Numerical Simulation

The responses of the LRB base-isolated PCSW structure with improved AHW connections obtained during the tests were simulated using OpenSees software. As the improved AHW connection was in elastic state during the shaking table tests and there was no crack in the AHW connection area, it is assumed that mechanical performance of the improved AHW connection is akin to the equivalent cast-in-place connection and that the longitudinal rebars in the AHW connection region are continuous.

In the OpenSees modelling, the LRB was defined using the LeadRubberX element. The multilayer shell element was used to simulate the shear wall (refer http://www.luxinzheng.net). The concrete was divided into six layers, and the rebars were smeared into four layers. Point-mass model was used to simulate the added mass on each floor of the structures. The Rayleigh damping coefficient was taken as 0.05 to simulate the energy dissipation in the models.

The numerically simulated structural responses were compared with the test results, and the acceleration time history responses for the fourth storey of Specimen A, obtained from simulation and tests, are shown in Figure 27. It can be observed that the numerically simulated storey acceleration is close to the values obtained during the tests. The shear force-displacement hysteresis curves for the isolation storey of Specimen A, obtained from simulation and tests, are shown in Figure 28; the figure shows that the two curves match well. The results shown in Figures 27 and 28 indicate that the multilayer shell element and LeadRubberX element can be used to simulate the precast reinforced concrete shear wall and the LRB, respectively, and that the assumption of the longitudinal rebars in the AHW connection region being continuous is reasonable.

(a) CA1968

(b) TA1952

(c) AR2015

Figure 27: Comparison of acceleration history responses of the fourth storey for PGA = 400 gal.

(a) CA1968

(b) TA 1952

(c) AR2015

Figure 28: Comparison of shear force-displacement hysteresis loops of the isolation system for PGA = 400 gal.

6. Conclusions

Shaking table tests and numerical simulation were performed to evaluate the seismic behaviour of a base-isolated PCSW structure model using improved AHW connections. During the tests, performance of the improved AHW connections was especially studied. The absolute acceleration responses and deformation responses of the base-isolated PCSW structure model were measured to reveal the dynamic properties and failure modes of the structure. Furthermore, OpenSees software was used to simulate the seismic response of the base-isolated PCSW structure model. Based on the results, conclusions are draw as follows.

There was no crack in the AHW connection area in the base-isolated PCSW structure model, indicating that the reliability of the improved AHW connection and the safety of the PCSW structure can be ensured during earthquakes.

Compared with the base-fixed PCSW structure model, the base-isolated PCSW structure model had less cracks in the AHW connection area, coupling beams and shear walls, indicating that the LRB isolation system can reduce cracks effectively.

The structural damping ratio can be increased to 16% by installation of LRBs, and the frequency of the structure can be reduced to 2.2 Hz.

The absolute acceleration response, ISD response, and maximum ISSF response of the PCSW structure model can be reduced significantly by the installation of LRBs. When the input PGA is 400 gal, the acceleration reduction ratio was approximately 55%; the ISD isolation ratio was approximately 60%; and the ISSF reduction ratio of the first storey was approximately 50%.

The seismic responses of the base-isolated PCSW structures with the improved AHW connections can be numerically simulated using OpenSees software, based on the assumptions that mechanical performance of the improved AHW connection is akin to the equivalent cast-in-place connection and that the longitudinal rebars in the AHW connection region are continuous.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

The authors are grateful for the funding provided by National Key Research and Development Program of China (Grant No. 2017YFC0703602), the National Natural Science Foundation of China (Grants nos. 51708257 and 51708258), Natural Science Foundation for Colleges and Universities in Jiangsu Province (17KJB560002), and the Science Foundation of Jiangsu University of Science and Technology (Grant no. 1122931605).

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