Research Article  Open Access
LeWen Zhang, Jing Wu, DaLiang Zhang, "Shape Optimization and Stability Analysis for Kiewitt Spherical Reticulated Shell of Triangular Pyramid System", Mathematical Problems in Engineering, vol. 2019, Article ID 2723082, 11 pages, 2019. https://doi.org/10.1155/2019/2723082
Shape Optimization and Stability Analysis for Kiewitt Spherical Reticulated Shell of Triangular Pyramid System
Abstract
The Kiewitt spherical reticulated shell of triangular pyramid system is taken as the object of this study; a macroprogram of parametric modeling is developed by using the ANSYS Parametric Design Language. The minimum structural total weight is taken as the objective function, and a shape optimization program is proposed and compiled by adopting the sequence twostage algorithm in FORTRAN environment. Then, the eigenvalue buckling analysis for Kiewitt spherical reticulated shell of triangular pyramid system is carried out with the span of 90 m and risespan ratio of 1/7~1/3. On this basis, the whole nonlinear buckling process of the structure is researched by considering initial geometrical imperfection. The loaddisplacement curves are drawn, and the nonlinear behaviors of special nodes are analyzed. The structural nonlinear behaviors affected by risespan ratio are discussed. Finally, the stability of reticulated shell before and after optimization is compared. The research results show that users can easily get the required models only by inputting five parameters, i.e., the shell span (S), rise (F), latitudinal portions (Kn), radial loops (Nx), and thickness (T). Under the conditions of different span and risespan ratio, the optimal grid number and bar section for the Kiewitt spherical reticulated shell of triangular pyramid system existed after optimization; i.e., the structural total weight is the lightest. The whole rigidity and stability of the Kiewitt spherical reticulated shell of triangular pyramid system are very nice, and the reticulated shell after optimization can still meet the stability requirement. When conducting the reticulated shell design, the structural stability and carrying capacity can be improved by increasing the risespan ratio or the rise. From the perspective of stability, the risespan ratio of the Kiewitt spherical reticulated shell of triangular pyramid system should not choose 1/7.
1. Introduction
The reticulated shell is a major structural style of spatial structures, and it has advantages of reasonable force, rich structure type, convenient installation, etc., which has broad applications [1].
The spherical reticulated shell is a spatial structure of bar system, and its bar system is generated by connecting the nodes according to certain rules. It has the general characteristics of reticulated shell. More recently it has been widely used in largespan spatial structures, such as largesized sports/arts venues, waiting rooms, and other landmark buildings. According to different grid types, there are six typical spherical reticulated shells, i.e., Ribbed spherical reticulated shell, Schwedler spherical reticulated shell, Lamella spherical reticulated shell, Threeway grid spherical reticulated shell, Kiewitt spherical reticulated shell, and Geodesic spherical reticulated shell. Among them, the Kiewitt spherical reticulated shell has the advantages of attractive appearance, reasonable force, low material consumption, large stiffness and span, etc., which has broad application prospects in modern buildings [2].
The Kiewitt spherical reticulated shell of triangular pyramid system combines the virtues of singlelayer and doublelayer spherical reticulated shells. It has higher integral bearing capacity and deformation resistant capability than those of singlelayer spherical reticulated shell, and its total structural weight is less than that of doublelayer spherical reticulated shell. Therefore, the Kiewitt spherical reticulated shell of triangular pyramid system is a newtype spatial structure, which can be widely applied in largespan architectures. However, the number of nodes and bar elements of reticulated shell is too many and the type of bar connection is complicated. Moreover, the variation of span, rise, grid size, type, and other parameters can cause structural internal force reallocation. Thus, the workload of remodeling is very large when conducting shape optimization design and stability analysis. Conventional modeling of reticulated shell often focuses on handmodeling in domestic and foreign studies. The studies of parametric modeling method based on the ANSYS Parametric Design Language (APDL) are not many, and relevant research rarely involves the specific work of shape optimization and stability analysis for the Kiewitt spherical reticulated shell of triangular pyramid system.
In the aspect of shape optimization, many optimized methods have been proposed, and the relevant studies are as follows. Zhang and Dong [3] presented a structural optimization algorithm and developed a computer program, and the effectiveness of the proposed method was verified. Wang and Tang [4] proposed an optimum method based on the optimality criteria, which could be used in optimization design of singlelayer reticulated shells. Rahami et al. [5] introduced a combination of energy and force method and adopted the genetic algorithm for minimizing the weight of truss structures. Wu et al. [6] investigated a new design concept of MAS and proposed a shape optimization method with finite element analysis, which could be used in twodimensional stent models. Luo et al. [7] also studied a meshless Galerkin level set method for shape and topology optimization of continuum structures. Yildiz [8] investigated a comparison of evolutionarybased optimization techniques and proposed a hybrid optimization technique based on differential evolution algorithm for structural design optimization problems. Wang et al. [9] proposed a new MultiMaterial Level Set topology description model for topology and shape optimization of structures involving multiple materials. Lian et al. [10] developed a Tspline isogeometric boundary element method to conduct shape sensitivity analysis and gradientbased shape optimization in the threedimensional linear elastomer. Lian et al. [11] showed that a combined shape and topology optimization method could produce optimal 2D designs with minimal stress subject to a volume constraint. Burman et al. [12] presented a cut finite element method for shape optimization in the case of linear elasticity. In addition, the publications [13–20] also involve the structural optimization design.
In the early days, people adopted the imitative shell method based on continuous medium theory to analyze the stability of reticulated shell [21]. Although this method plays an important role in analyzing the stability of reticulated shell of particular form, it also has some limitations. With the speedy development of computer technology, the nonlinear finite element analysis has become a universal approach for structural stability analysis [22]. During the stability analysis of reticulated shell, the strength and stability are considered independently, which is usually adopted by the traditional linear analysis method. However, the above two factors are considered simultaneously in the nonlinear fullrange analysis, so the loaddisplacement curve can be drawn accurately, and the impacts of various factors on structural stability can be analyzed reasonably.
In terms of structural stability analysis, the research on eigenvalue buckling analysis and nonlinear buckling analysis has got some achievements. Ferreira and Barbosa [23] presented a finiteelement model for geometric nonlinear analysis of composite shell structures. Han et al. [24] investigated the validity of the finite element method on the buckling and postbuckling behavior of laminated composite cylindrical shells that have been subjected to an external hydrostatic pressure. Basaglia et al. [25] adopted the generalized beam theory (GBT) to analyze the global buckling behavior of plane and space thinwalled frames. Papadopoulos et al. [26] presented a computationally efficient method for the buckling analysis of shells with random imperfections, based on a linearized buckling approximation of the limit load of the shell. Ghannadpour and Ovesy [27] presented theoretical developments of an exact finite strip for the buckling analysis of symmetrically laminated composite plates and plate structures. Camotim et al. [28] presented a stateoftheart report on the use of GBT to assess the buckling behavior of plane and space thinwalled steel frames. Alibrandi et al. [29] proposed an efficient procedure for the reliability analysis of frame structures with respect to the buckling limit state. Fekrar et al. [30] conducted the buckling analysis of functionally graded hybrid composite plates by using a new fourvariable refined plate theory. Wang and Peng [31] proposed a Hermite reproducing kernel Galerkin meshfree approach for buckling analysis of thin plates. Ovesy et al. [32] presented an exact finite strip for the buckling analysis of laminated composite plates and plate structures by using Firstorder Shear Deformation Theory. Basaglia and Camotim [33] dealt with the application of beam finite element models based on GBT to analyze the buckling behavior of four thinwalled steel structural systems. Zhou et al. [34] revisited the buckling analysis of a benchmark cylindrical panel undergoing snapthrough when subjected to transverse loads. Ghannadpour et al. [35] presented an exact finite strip for the buckling and postbuckling analysis of moderately thick plates by using the First order Shear Deformation Theory. Kandasamy et al. [36] studied the free vibration and thermal buckling behavior of moderately thick functionally graded material structures including plates, cylindrical panels, and shells under thermal environments. Çelebi et al. [37] conducted the evaluation of the buckling and failure characteristics of shells include linear buckling analysis and nonlinear failure analysis using Riks method.
In the present study, a parametric modeling macroprogram for the Kiewitt spherical reticulated shell of triangular pyramid system is developed by using the APDL. On this basis, a shape optimization program is compiled by adopting the sequence twostage algorithm in FORTRAN environment. Shape optimization is achieved based on the objective function of minimizing total structural weight and the restriction condition of global constraints, locality constraints. Then, stability analysis for the Kiewitt spherical reticulated shell of triangular pyramid system is carried out with the span of 90 m and risespan ratio of 1/7~1/3. The stability analysis includes linear buckling analysis and nonlinear buckling analysis. Finally, the stability of reticulated shell before and after optimization is compared by examples. The conclusions of having reference significance for practical engineering are obtained.
2. Parametric Modeling for Kiewitt Spherical Reticulated Shell of Triangular Pyramid System
2.1. Geometric Descriptions
The span (S), rise (F), latitudinal portions (Kn), radial loops (Nx), and thickness (T) are the main geometric parameters of describing spherical reticulated shell [14, 15]. The schematic diagram of geometric parameters of spherical reticulated shell is shown in Figure 1.
The sphere curvature radius is calculated as follows:
The global angle Dpha of two radial neighboring circle nodes is calculated as follows:
2.2. Parametric Modeling
S, F, Kn, Nx, and are determined in the spherical coordinates; then the and Dpha are calculated. The nodes are generated in each circle from inside to outside in order by using cyclic command statements. Let vertex of upper layer be number 1. Then the numbers and coordinates of nodes are calculated. The bar element is generated by connecting related nodes according to the following conventions: applying loads on nodes whose number is less than starting node number of the outermost circle and imposing displacement constraints on other nodes. A macroprogram of parametric modeling is compiled by using APDL. The specific parametric modeling process can refer to Wu et al. [14, 15].
2.3. The Input Window of Geometrical Parameters and Modeling Examples
A program for input window of geometrical parameters is compiled by using APDL, and the input window is shown in Figure 2. Users can easily get the required models only by inputting the parameters such as S, F, Kn, Nx, and T.
Some parametric modeling examples of Kiewitt spherical reticulated shell are given in Figures 34.
(a) Singlelayer
(b) Triangular pyramid system
(a) S=60; F=15; Kn=6; Nx=16; T=1.0
(b) S=90; F=18; Kn=6; Nx=18; T=1.5
3. Shape Optimization for the Kiewitt Spherical Reticulated Shell of Triangular Pyramid System
3.1. Mathematical Models of Shape TwoStage Optimization
The mathematical models of shape optimization mainly include design variables, objective function, and constraint conditions. The detailed information can be referred in Wu et al.’s previous studies [14, 15].
(1) The FirstStage (CrossSection) Optimization. Mathematical models of crosssection optimization are as follows:
(2) The SecondStage (Shape) Optimization. Mathematical models of shape optimization are as follows:
Given the range of Kn, Nx, and T, the optimal solution is sought with the goal of minimizing the total weight of spherical reticulated shell.
3.2. Process of Shape Optimization
The design concept of twostage optimization can refer to Wu et al. [18].
The specific process of crosssection optimization is described as follows:
(1) Modeling is conducted in the ANSYS software, and S, F, Kn, Nx, and T are input. The loads and boundary constraints are applied on the model. The bar elements are divided into many groups and the material characteristics are input, respectively. Mechanical analysis is carried out and pretreatment files are generated.
(2) Input the number of nodes and bar elements, the grouping number, the types of ball joint, the discrete sets of node and bar element types, and other basic parameters in program.
(3) The first element of the discrete sets is selected as initial design variables, and the corresponding crosssectional area of bar element in the pretreatment files is replaced. Onedimensional searching is conducted.
(4) Internal force analysis of the structure is carried out by calling interface program, in order to check constraints of stress, displacement, and slenderness ratio. If they meet the constraints, then turn to step (7). If not, turn to step (5).
(5) The second level crosssection optimization is carried out.
(6) Internal force analysis of the structure is carried out by calling interface program, in order to check constraints of stress, displacement, and slenderness ratio. If they meet the constraints, then turn to step (7). If not, calculate relative difference quotient and form new design point; then turn to step (5).
(7) Conduct Zeroth correction, and output optimization results (crosssectional area of bar elements).
(8) Ball joints are selected and optimized according to the optimal crosssectional area of bar elements.
(9) Output the whole optimization results, and the program runs to completion.
The crosssection optimization flowchart of Kiewitt spherical reticulated shell of triangular pyramid system is shown in Figure 5.
3.3. Results of Shape Optimization
The bar elements of spherical reticulated shell adopt hotrolling seamless pipe, steel density = 7800 kg/m^{3}, elastic modulus E = 2.06 × 10^{5} Mpa, Poisson ratio =0.3, and yield strength of steel [] =2.15 × 10^{8}N/m^{2}. The steel type is Q235; i.e., outer diameter D=0.152m, wall thickness t=5mm, sectional area S=2.309 × 103m^{2}, second moment of area I=6.2443 × 106m^{4}, and sectional resistance moment W= 8.216 × 10^{−5}m^{3}. The uniform load (q = 2.35 KN/m^{2}) has vertically downward effect on the nodes of spherical reticulated shell. In addition, constraint conditions of the outermost nodes of spherical reticulated shell are simply supported. The optimized results of Kiewitt spherical reticulated shell of triangular pyramid system with the span of 90 m are shown in Table 1.

4. Stability Analysis for the Kiewitt Spherical Reticulated Shell of Triangular Pyramid System
The eigenvalue buckling analysis and geometric nonlinear analysis for Kiewitt spherical reticulated shell of triangular pyramid system are carried out in this section. The structural loaddisplacement curve is got, and the whole changing process of structural displacement is fully understood by response analysis. The structural stability capacity is determined, and the relationship between displacement and stability is discussed.
4.1. Eigenvalue (Linear) Buckling Analysis
Buckling analysis is mainly used for studying structural stability under specific loads and determining the critical load of structural instability. The buckling analysis includes linear buckling analysis and nonlinear buckling analysis. The linear elastic buckling analysis is also known as the eigenvalue buckling analysis. The nonlinear buckling analysis includes geometrical nonlinear buckling analysis, elasticplastic buckling analysis, and nonlinear postbuckling analysis.
The purpose of eigenvalue buckling analysis is to predict theoretical buckling strength of an ideal elastomer, which is similar to buckling analysis of elasticity theory. However, initial imperfection and nonlinear behavior existed in practical reticulated shells. The linear analysis method overestimates the structural loadcarrying capacity, so the solution of eigenvalue buckling analysis is very conservative and not safe. But the primary advantage of this approach is that the analysis process adopts linear computation, and the calculation speed is fast, which can provide a basis for further analysis and determination of the critical load. Therefore, the eigenvalue buckling analysis conducted in advance will contribute to the following nonlinear buckling analysis, and it is the foundation for further geometric nonlinear analysis.
The eigenvalue buckling load is the upper critical point of the linear buckling load, and it can be used as a given load of nonlinear buckling analysis. Feature vector buckling shapes can be used as a basis for applying initial imperfection or disturbance loads.
The eigenvalue can be obtained by the load factor or the scale factor in the flowing equation:
where [K] is the stiffness matrix; [Ks] is the stress stiffness matrix; is the vector of displacement; is the eigenvalue.
The represents the scale factor of a given load. If the given load is a unit load, then the resulting eigenvalue is the buckling load of the reticulated shell.
The eigenvalue (linear) buckling analysis for Kiewitt spherical reticulated shell of triangular pyramid system is carried out with the span of 90 m and risespan ratio of 1/7~1/3. The calculation parameters can refer to Section 3.3. Linear buckling loading coefficients of the first six order modes with the risespan ratio of 1/7~1/3 are listed in Table 2. The first three order modes and buckling loading coefficients with the risespan ratio of 1/5 are shown in Figures 6–8.

(a) The first order mode
(b) The buckling loading coefficient, 8.830
(a) The second order mode
(b) The buckling loading coefficient, 8.833
(a) The third order mode
(b) The buckling loading coefficient, 8.833
It can be obtained from Table 2 and Figures 6–8:
(1) During the eigenvalue buckling analysis, the eigenvalue buckling loading coefficient that corresponded by each order mode increases with the risespan ratio. It can be generally inferred that the stability of Kiewitt spherical reticulated shell of triangular pyramid system increases with the spanrise ratio. Moreover, the influence of risespan ratio on eigenvalue buckling loading coefficient is very large. Take the first order mode for an example: the eigenvalue buckling load coefficient is 5.018 when the risespan ratio is 1/7, while the eigenvalue buckling load coefficient increases to 15.663 when the risespan ratio is 1/3, which has more than tripled.
(2) As for the first three order modes that corresponded by each risespan ratio, the eigenvalue buckling load coefficients of the second order mode and the third order mode are the same, but they are different from that of the first order mode. The integral structural buckling modes of the second order and the third order are positive symmetric, while the first order mode is antisymmetric. The main reason is that the shape of reticulated shell and load distribution are symmetrical.
4.2. Geometrical Nonlinear WholeProcess Analysis
(1) Structural Nonlinear WholeProcess Analysis with Initial Geometrical Imperfection. The geometrical nonlinear buckling analysis is to use the finite element method to analyze the structural stability. The geometrical nonlinear wholeprocess analysis can be conducted through loaddisplacement curves, and then the structural carrying capacity can be determined.
The nonlinear buckling analysis for Kiewitt spherical reticulated shell of triangular pyramid system is carried out by consideration of initial geometrical imperfection, and the geometrical nonlinear whole process is analyzed.
After the stability wholeprocess analysis, the loaddisplacement curve of each node can be obtained. In general, the loaddisplacement curve of the maximum displacement node at the end of iteration is taken as a representative. The wholeprocess analysis curve is very complex. From the perspective of practicability, the equilibration stage and the subsequent buckling path are just taken and researched. During the nonlinear wholeprocess analysis, the relevant geometrical parameters are the same as the parameters of eigenvalue buckling analysis. Take 1/300 of span (90m) as the initial geometrical imperfection, and it is applied on the Kiewitt spherical reticulated shell of triangular pyramid system for nonlinear buckling analysis. The node 77 is located on the main rib of the 4th loop from the vertex to outside, and its displacement is the largest. The nodes 76 and 78 are adjacent to the node 77, and they are located on the same loop. The loaddisplacement curves of the three nodes are shown in Figure 9. The curve is complex and varied, but with good regularity.
It can be reached from Figure 9:
(1) The relationship between the load and displacement is basically linear at the initial stage of loading (i.e., equilibrium path stage). After the upper critical point, the structure enters the postbuckling stage, and the relationship between the load and displacement is obviously nonlinear.
(2) When the structure reaches the upper critical point, the Z direction displacements of the three nodes (76, 77, and 78) are 0.07m, 0.19m, and 0.07m. After the postbuckling stage, the Z direction displacements of the three nodes (76, 77, and 78) are 0.69m, 1.00m, and 0.69m based on the computation convergence. With the node 77, for example, when the postbuckling path reaches the first lower critical point, the displacement is 0.45m. The value has exceeded structural maximum allowable value (span/400=0.225m) according to the architectural structure load code. In the later stages, the displacement that corresponded by each limit point far exceeds the maximum allowable value (0.225). Therefore, the following paths after the first lower critical point have no practical engineering significance for studying reticulated shell.
(3)As far as these three nodes are concerned, the node 77 is the first to buckling. When the structure reaches the ultimate bearing capacity and begins to collapse, the Z direction displacement of node 77 is the largest, and the displacements of nodes 76 and 78 are the same. That is mainly because the two nodes (76 and 78) are symmetrically located on both sides of the node 77.
(4) When the structure reaches the upper critical point, the maximum Z direction displacement is 0.19m, which is 1/450 of the structural span (S=90m). The structural maximum displacement must not exceed 1/400 of the span based on the architectural structure load code, so the displacement meets the relevant requirement of reticulated shell. The stability coefficient of reticulated shell is 6.54. The stability coefficient must not be less than 4.2 according to the technical specification for reticulated shell and design code for the steel structures, so the stability meets the requirement. In conclusion, it can be drawn that the whole rigidity and stability of Kiewitt spherical reticulated shell of triangular pyramid system are relatively good.
(2) Structural Nonlinear Buckling Analysis in Different RiseSpan Ratio. In order to investigate the structural nonlinear buckling affected by the risespan ratio, the risespan ratio of reticulated shell is set as 1/4, 1/5, 1/6, and 1/7, respectively, and the structural nonlinear buckling process is analyzed. The loaddisplacement curves of the node 77 (the maximum displacement node) with the risespan ratio of 1/4~1/7 are shown in Figure 10.
It can be reached from Figure 10:
(1) For the Kiewitt spherical reticulated shell of triangular pyramid system, the loaddisplacement curves vary greatly in different risespan ratio. But their common feature is that the equilibrium path before reaching the upper critical point is nearly linear, and the displacement is small. For the postbuckling stage, the curves come in all shapes and sizes, but they converge eventually. During the postbuckling stage, the displacement increases rapidly.
(2) The stability coefficient of reticulated shell changes with the risespan ratio, and the stability coefficient is the largest when the risespan ratio is 1/5.
(3) Within a certain range, the larger the risespan ratio, the greater the critical bearing capacity. Going even further, the bearing capacity and deformation capacity of the postbuckling stage are also greater. Therefore, when conducting reticulated shell design, the structural stability and bearing capacity can be improved by increasing the risespan ratio or rise appropriately.
(4) When the risespan ratio is 1/7, the corresponding stability coefficient is 4.45. Although the value can meet the relevant requirements of specification, it is close to the allowable value 4.2. Moreover, the displacement is only 0.0345m when reticulated shell converges eventually. At the moment, the structural deformation capacity is much of poor. Therefore, from the perspective of stability, the structural risespan ratio should not choose 1/7 in practical engineering.
In addition, the stability of the optimized Kiewitt spherical reticulated shell of triangular pyramid system is analyzed. The optimal geometrical parameters after optimization are as follows: The risespan ratio is 1/5; the latitudinal portions are 8 (Kn=8); and the radial loops are 15 (Nx=15). The optimal values of bar section are shown in Table 3.

The optimized sectional dimensions are given to the bar elements, and then the structural nonlinear buckling analysis is carried out. The loaddisplacement curves are drawn, as shown in Figure 11.
It can be known from Figure 11: The structural stability coefficient is 6.33 before optimization, while it is 4.28 after optimization. The stability coefficient became smaller. That is to say that the safety stock of reticulated shell is reduced on the premise of satisfying the design requirements of structural global stability. The main reason is that the total weight of optimized reticulated shell is reduced. However, the optimized stability coefficient is still higher than the limiting value in the technical specification of reticulated shell. It shows that the optimized reticulated shell still satisfies the safety requirement specified by the code.
5. Conclusions
An efficient parametric modeling method is proposed for the Kiewitt spherical reticulated shell of triangular pyramid system. A shape optimization program is compiled by using sequence twostage algorithm in FORTRAN environment. The eigenvalue buckling analysis for Kiewitt spherical reticulated shell of triangular pyramid system is carried out with the span of 90 m and risespan ratio of 1/7~1/3. On this basis, the structural nonlinear buckling wholeprocess is researched by considering initial geometrical imperfection. Some useful conclusions are drawn as follows:(i)Users can easily get the required models only by inputting five parameters, i.e., the shell span (S), rise (F), latitudinal portions (Kn), radial loops (Nx), and thickness (T).(ii)Under the conditions of different span and risespan ratio, the optimal grid number and bar section of Kiewitt spherical reticulated shell of triangular pyramid system existed after optimization. Moreover, at this moment, the total weight is the lightest.(iii)The whole rigidity and stability of Kiewitt spherical reticulated shell of triangular pyramid system are very good, and the optimized reticulated shell can still meet stability requirements.(iv)The stability and carrying capacity can be improved by increasing risespan ratio or rise when conducting design of reticulated shell.(v)From the perspective of stability, the risespan ratio of Kiewitt spherical reticulated shell of triangular pyramid system should not choose 1/7.
Data Availability
The data used to support the findings of this study are available from the corresponding author upon request.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
The authors would like to acknowledge the financial support from the China Postdoctoral Science Foundation (Grant No.: 2019M652384) and the Natural Science Foundation of Shandong Province (Grant No.: ZR2017MEE032).
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Copyright © 2019 LeWen Zhang 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.