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Elastic buckling of simply supported stiffened steel plates with circular opening
Journal of Engineering and Applied Science volumeÂ 69, ArticleÂ number:Â 106 (2022)
Abstract
Steel plates are used as the main components of steel elements in many structures. Openings in steel elements may exist for maintenance or inspection purposes in addition to creating paths for different fixtures such as air conditioning, pipes, and facilities. The structural performance of plates with openings is different from that of solid plates when subjected to axial compressive load. Openings affect local buckling, lateral torsional buckling, and shear of plates. Adding stiffeners around openings is a common engineering practice to strengthen plates. However, different design codes and guides provide estimates of the flexural and shear capacity of beams with no clear formulas for the influence of such openings on axial buckling strength. In this study, a parametric study has been performed using generalpurpose finite element software, ANSYS, in order to study the effect of using stiffeners around circular opening in simply supported axially loaded plates on the elastic buckling behavior. Different parameters were considered including the aspect ratio of the plate, opening diameter, opening position in both horizontal and vertical directions, and stiffenerâ€™s dimensions. The results of the extensive parametric study are used to propose an empirical design formula considering the different studied parameters.
Introduction
Introducing openings to plates affects their structural behavior. Instability/buckling can occur under axial compressive loads at loading levels lower than anticipated. Common design practices usually include strengthening of perforated plates with stiffeners around openings. The AISC design guide [1] provides design formulas to estimate the shear and flexural capacity of steel beams with web openings. However, the guide focuses on the case of plates subjected to linear stress gradient without accounting for stiffener dimensions and opening location. Moreover, while the formulae proposed by the guideline are simple and useful to apply to real situation, it needs more research to account for different parameters and factors [2]. Elastic buckling and elastoplastic buckling of perforated plates and Ibeams have been intensively investigated by several researchers through experimental and numerical analyses [3,4,5,6,7,8,9,10,11,12,13,14,15,16,17]. Performed research focused on the influence of different opening shapes, size of opening, and location of opening in addition to plate boundary conditions. Results from numerical and experimental investigations were used to build interaction diagrams and design curves [3, 5, 7, 8, 18,19,20,21] or proposing design formulas that account for different parameters [15, 20, 22]. In addition, recommendations regarding critical zones in perforated plates where it is not recommended to place openings and value of critical buckling strength were evaluated by several researchers [8, 13, 23]. Cheng and Zhao [24] were the first to study the strengthening of simply supported square steel plates with a centrally placed circular hole subjected to uniaxial compressive loads using stiffeners. Four types of stiffeners were considered including ringed stiffener, flat stiffener, longitudinal stiffener, and transverse stiffener as shown in Fig. 1. A series of numerical analyses of both elastic and elastoplastic buckling behaviors for stiffened and unstiffened perforated plates were carried out. However, the study focused on strengthened plates with central circular openings. In addition, stiffener plates were extended through the whole width or depth of perforated plates which might not be practical in some cases. In the current research, an extensive parametric study is performed to study the effect of strengthening on elastic buckling of simply supported plates while considering different locations for openings. Parameters also include plateâ€™s aspect ratio (Î±), widthtothickness ratio (Î»), circular opening diameter, and opening location with respect to X and Y axes. Results are analyzed to pinpoint the key parameters. Accordingly, a formula is developed to estimate the elastic buckling coefficient of unstiffened and stiffened plates with circular openings.
Methods
Description of models
SHELL63 element is used to model plates and stiffeners using ANSYS 11 finite element software [25]. This element has both bending and membrane capabilities. Both inplane and normal loads are permitted. The element has six degrees of freedom at each node: translations in the nodal x, y, and z directions and rotations about the nodal x, y, and z axes.
Models in the current study are divided into two main groups: (1) plates with circular unstiffened opening and (2) plates with circular stiffened opening. Stiffening configurations included stiffeners parallel to load direction, stiffeners perpendicular to load direction, and stiffeners forming box shape around the opening as illustrated in Fig. 2. Modeled plates have length W, height D, and thickness t_{b}. Circular openings have diameter OPH, edge distance from the Yaxis OPX, and edge distance from the Xaxis OPY. In addition, stiffener dimensions are length H_{s}, breadth B_{s}, and thickness t_{s}.
Boundary conditions have a large influence on the buckling resistance of plates as they control behavior during buckling. Web plates are usually considered to be simply supported or partially fixed. For the top end of the model, the top area of the steel plate was constrained in X and Z directions to represent hinged support at the top end of the plate. Several meshing trials were made for solid plate and compared to the theoretical equation proposed by Timoshenko [26] till the most fitting mesh was reached. Figure 3a shows boundary conditions considered for the different models in the current study. Models are analyzed under uniaxial compressive stresses. Pressure is applied at two opposite edges as shown in Fig. 3b.
Eigenvalue buckling analysis
Buckling load and subsequently buckling coefficient (K) are estimated through eigenvalue buckling analysis for the unloaded steel plates. The buckling coefficient is determined considering the following formula:
Where
Ï¬_{cr}: Critical buckling stress calculated as per theoretical or numerical methods
Î½: Poissonâ€™s ratio
E: Youngâ€™s modulus
D and t: Plate dimensions as defined in Fig. 2
The buckling factor (K) was given a suffix to indicate whether it is calculated for the solid plate (K_{no}), plate with circular opening (K_{o}), or strengthened plate with circular opening (K_{s}).
Model verification
Several initial runs are performed to test the sensitivity of the used mesh and determine the best size that will guarantee suitable run time and accuracy. Afterwards, verification of models is performed first for solid plates against elastic buckling values estimated by Timoshenko [26] as listed in Table 1.
Models for plates with circular openings are built and verified against results reported by Cheng and Zhao [24] for elastic buckling of a rectangular plate with circular opening under constant load. Figure 4 shows the effect of opening position and opening diameter on the elastic buckling load resulting in the current study compared to values reported by Cheng and Zhao [24]. Good agreement is observed between the results of the mentioned paper compared to the results extracted from the analyticalÂ model. FigureÂ 4 shows that the maximum error between results reaches 2% which is considered aÂ small valueÂ and can be accepted.
Figure 5 shows the verification of strengthened plates against results reported by Cheng and Zhao [24] for longitudinal and transversal stiffeners. Results show good agreement with a maximum error of 10%. The difference is due to neglecting transverse shear deformations in the current study.
Independent parameters
The parametric study is performed using the calibrated analytical models to investigate the effect of different parameters that may affect the elastic buckling behavior of unstrengthened and strengthened plates with circular opening under uniaxial compressive loading. The studied independent parameters used in the study can be summarized as shown in Table 2. The considered independent parameters include the widthtodepth ratio of the plate (W/D), widthtothickness ratio of the plate (W/t_{p}), location of the opening in X and Ydirections, and dimensions of the added stiffeners (H_{s}, B_{s}, and t_{s}). The parametric study is established by varying the value of each independent parameter separately. Figure 6 summarizes performed analyses and symbols used throughout the performed study.
Several runs are also performed considering stiffeners forming a box shape around the opening. This trial was made to check whether combining the stiffeners parallel to the load direction with those normal to the load direction will enhance elastic buckling behavior or not. The additional runs are executed only considering Î± = 1.0 combined with stiffenersâ€™ dimensions with respect to the circular opening diameter (B_{s}/OPH = 0.6) for opening moving in X and Ydirections.
Results and discussion
An extensive parametric study is conducted to evaluate the effect of the different geometric parameters on the elastic buckling of strengthened and unstrengthened plates with circular openings in order to deduce a suitable formula for the buckling coefficient (K). Effects of the different considered parameters will be exhibited in the next sections for unstrengthened and strengthened plates separately.
Unstrengthened plate with circular opening
Influence of slenderness ratio (W/t _{p})
Several runs were performed to study the influence of plate slenderness ratio on the buckling coefficient factor (K) as illustrated in Fig. 8, where symbols OP1, OP2, and OP3 present opening diametertowidth ratios of 0.1, 0.2, and 0.3, respectively. Numbers between brackets refer to the position of the opening center with respect to the X and Y axes. Figure 7 shows that the plate slenderness ratio has no effect on the buckling factor coefficient (K_{o}). If the buckling coefficient (K_{o}) for perforated plates is compared to the ones extracted from solid plate models, it can be observed that the coefficient (K_{o}) decreases by about 1â€“2.5% for plates with an opening near the corner. However, for models having small diameters, the decrease in buckling coefficient can be neglected. For plates having an aspect ratio equal to 1.5 and a central opening, the buckling coefficient of perforated plates slightly increased when compared to solid plates.
Influence of aspect ratio (W/D)
As indicated by previous researchers, the aspect ratio of plates has a great effect on the buckling coefficient factor (K). Figure 8 shows that the buckling coefficient factor (K_{o}) decreases linearly when the aspect ratio is less than 1 with a high slope. However, for aspect ratios ranging between 1 and 1.5, the buckling coefficient factor (K_{o}) increases slightly then decreases again as the aspect ratio reaches to 2. It is also clear from curves that the general relationship between the buckling coefficient factor (K_{o}) and plate aspect ratio is the same for all considered slenderness ratios.
Influence of opening position in the Xdirection (OPX/W)
For a small aspect ratio equal to 0.5 and a small opening diameter, the position of the hole affects the buckling coefficient factor significantly. As shown in Fig. 9, the local buckling factor (K) decreases as the opening moves towards the center of the plate. While for aspect ratios equal to 1 till 2, the buckling coefficient factor (K_{o}) slightly changes as the position of open changes.
For the different considered aspects, the buckling coefficient factor (K_{o}) decreases as the opening gets near to the center. The decrease ranges from 4 to 10.4% for the aspect ratio equal to 0.5. Meanwhile, the decrease in buckling coefficient factor (K_{o}) ranges from 2.8 to 4.1% for the aspect ratio equal to 1.0. For the aspect ratio equal to 2, the buckling coefficient factor (K_{o}) decreases as the opening gets near to the center except for the case of openings near the plate corner. In this case, a slight increase may occur and reaches 0.5%. While the decrease ranges from 1 to 4%. This shows that for aspect ratios larger than 1.0, the effect of the opening is less pronounced than other aspect ratios.
Influence of opening position in the Ydirection (OPY/W)
The position of the opening in the Ydirection is varied for different plate aspect ratios and the influence on the local buckling factor (K_{o}) is studied. It is generally observed that the buckling factor decreases as the opening approaches the center of the plate. Meanwhile, for an aspect ratio equal to 1 through 2, the buckling coefficient factor (K_{o}) slightly changes as the position of the open changes as shown in Fig. 10.
Figure 11 shows the effect of the opening diameter on the buckling coefficient factor (K_{o}) at the same aspect ratio which was taken to be 1. The results show that the buckling coefficient factors (K) decrease as the opening diameter increases.
Strengthened plate with longitudinal stiffener
Several runs are performed while considering longitudinal stiffeners around the introduced circular opening. Two cases are considered for the location of the circular opening: (1) a circular opening moving in the Xdirection and centered in the Ydirection and (2) a circular opening moving in the Ydirection and centered in the Xdirection. These cases are considered for circular openings having OPH/W ratios ranging between 0.1 and 0.5 while considering plate aspect ratios of 0.5, 1, 1.5, and 2. Accordingly, the buckling coefficient factor for stiffened plate (K_{s}) is compared to the buckling coefficient factor for unstiffened plates with a circular opening (K_{o}) and the buckling coefficient factor of the solid plate (K_{no}).
Results are exhibited for different plate aspect ratios while comparing normalized buckling factor with respect to the unstrengthened plate with opening (K_{s}/K_{o}) and normalized buckling factor with respect to the solid plate (K_{s}/K_{no}). Figure 12 shows the relation between the normalized buckling factor coefficient (K_{s}/K_{o}) with the position of the cutout with respect to the yaxis (OPX/W) and variation of B_{s}/OPH for plate aspect ratio equal to 0.5.
It can be deduced from the curves that:

For OPH/W = 0.1, as the location of the opening in Xdirection with respect to plate width (OPX/W) changes from 0.1 to 0.5, the buckling coefficient factor ratio (K_{s}/K_{o}) increases by a percentage ranging from 101 to 108.3%. Meanwhile, for OPH/W = 0.2, the buckling coefficient factor ratio (K_{s}/K_{o}) increases by a percentage ranging from 112.5 to 137.8%. This ratio increases between 122.5â€“200.7% and 178.9â€“329.6% for the OPH/W ratio equal to 0.3 and 0.4, respectively.

The results also show that the change of stiffener breadth (B_{s}) has no effect on the buckling coefficient factor (K_{s}).
For aspect ratio 0.5, Fig. 13 shows the relation between the normalized buckling factor coefficient (K_{s}/K_{o}) with the variation of B_{s}/OPH and the position of the cutout with respect to the xaxis (OPY/D). Examining the figure, it is clear from the curves that as the OPY/D ratio increases, the buckling coefficient factor ratio (K_{s}/K_{o}) increases. The percentage of increase ranges between 104.7 and 601.7%. The maximum increase is observed when OPH/W = 0.5 and OPY/D = 0.5.
Figure 14 shows the deformed shape for stiffened and unstiffened plates. It can be seen that the horizontal stiffener changes the elastic buckling mode with respect to the number of waves. This is due to the increase in plate stiffness upon strengthening.
Figure 15 shows a comparison between stiffened perforated plate and solid plate for an aspect ratio of 1.5. It is clear from the curves that the influence of adding stiffener for OPH/W = 0.1 is different than other ratios. At this ratio, the local buckling factor increases at OPX/W = 0.1â€“0.3 then it starts to decrease at OPX/W = 0.4 and 0.5. For the other ratios, the buckling coefficient increases as OPX/W increases by a percentage ranging between 108 and 214.3%. In addition, it can be observed that the stiffener breadth (B_{s}) value does not have a large influence on the local buckling coefficient (K_{s}) for the different values of OPH/W. FigureÂ 16 shows the deformed shape of stiffened and unstiffened plates as the opening changes its location in the Xdirection. When the plate aspect ratio exceeds 1.0, the plate deforms in two half waves. Adding a circular opening near the edge or at the middle of these plates has relatively no effect on the plate deformed shape. For other locations of openings, it is observed that deformation of the part including the opening is larger than the one in the other half that does not include an opening. When adding stiffeners parallel to the load direction, a decrease in deformations is generally observed. Increasing the opening diameter gradually changes the deformed shape to a single wave which explains the decrease of the local buckling coefficient for stiffened plates.
Strengthened plate with transversal stiffener
Several runs are performed while considering transversal stiffeners around the introduced circular opening. Two cases are considered for the location of the circular opening: (1) a circular opening moving in the Xdirection and centered in the Ydirection and (2) a circular opening moving in the Ydirection and centered in the Xdirection. These cases are considered for circular openings having OPH/W ratios ranging between 0.1 and 0.5 while considering plate aspect ratios of 0.5, 1, 1.5, and 2. Accordingly, the buckling coefficient factor for stiffened plate (K_{s}) is compared to the buckling coefficient factor for unstiffened plates with a circular opening (K_{o}) and the buckling coefficient factor of the solid plate (K_{no}).
Strengthened plate using box stiffener
Combining longitudinal and transversal stiffeners, a box stiffener is introduced around the opening. Several runs were made on plates with an aspect ratio of 1.0 only to compare the effect of the box stiffener with each case separately. Figures 18 and 19 show results compared to unstiffened opening and opening stiffened with longitudinal and transversal stiffeners, respectively.
Examining Fig. 17, it is clear that the box stiffener strengthens the plate. When compared to longitudinal stiffener, using the box stiffener has a small effect for OPH/W = 0.1â€“0.3. However, its effect increases clearly for OPH/W = 0.4 and 0.5. For OPX/W = 0.3, strength increases by about 40%; meanwhile, it decreases by 20% when OPX/W = 0.5. This can be attributed to the fact that the box stiffener is totally inside the maximum deformed zone and has no effect on the deformed shape. When comparing box stiffener to transversal stiffener, the influence can be neglected when OPH/W = 0.1â€“0.3. However, strength increases by a percentage of 90% when OPH/W = 0.5 and OPX/W = 0.3. Figure 18 shows the comparison between the box stiffener and the transversal stiffener.
It can be seen that using the box stiffener strength doubles the elastic buckling strength when compared to a longitudinal stiffener for OPH/D = 0.5 and OPY/D = 0.3. However, for OPH/D = 0.1â€“0.3, the box stiffener strength provides the same strength of transversal stiffeners. Considering Figs. 19 and 20, it is clear how the deformed shape changes with the change of stiffener type and that explains the trend of curves above.
Proposed formula for elastic buckling of unstrengthened and strengthened plates with circular openings
Timoshenko [26] proposed a formula to calculate the buckling stress for plates with different aspect ratios, slenderness ratios, loading conditions, and boundary conditions as follows:
The main purpose of the current study is to discuss the effect of different parameters on local buckling of plates and to propose an empirical formula to calculate the local buckling coefficient (K_{o}) for a rectangular plate with circular opening having different positions in X and Ydirections. Based on the parametric study results, the plate slenderness ratio proved to have a neglected effect on the buckling coefficient. Hence, parameters considered in the proposed equation include 5 factors (aspect ratio Î±, slenderness ratio Î», normalized opening diameter OPH/W, normalized distance between the center of open to the Yaxis OPX/W, normalized distance between the center of the circle and the Xaxis OPY/D). Several formulas were checked out through many trials using the Eureqa program [27]. The program was used to run a formula search using regression analysis after defining the detrimental factors. Estimated formulas with their different complexity factors and errors were calculated. The most suitable equation was then chosen according to the minimum calculated error. These are shown in Eqs. 3 to 5 for unstiffened and stiffened plates with circular openings. The accuracy of the proposed equations is compared in view of the parametric study results as shown in Fig. 21. The R^{2} value was found to range between 0.86 and 0.98 which can be considered a good match.
Where
K_{o}: Elastic buckling coefficient of the plate with circular opening
\(K:\textrm{Elastic}\ \textrm{buckling}\ \textrm{coefficient}\ \textrm{of}\ \textrm{the}\ \textrm{solid}\ \textrm{plate}={\left(\frac{\alpha }{m}+\frac{m}{\alpha}\right)}^2\) ;
Î±: W/D; X: OPX/W; Y: OPY/D; H: OPH/D; Ï‰: H_{s}/W; Î²: B_{s}/OPH
m: No. of half waves
Conclusions
The aim of the current study is to investigate the influence of different parameters on the local buckling of steel unstrengthened and strengthened plates with circular openings. These parameters include the plateâ€™s aspect ratio, slenderness ratio, circular opening diameter, opening position with respect to the X and Y axes, stiffener dimensions, and configuration. Structural models are established based on the finite element method, where elastic buckling analyses are performed using ANSYS software. Plates with simply supported boundary conditions are subjected to uniaxial compressive uniform pressure. The finite element results are verified against results reported by previous researchers. Comparisons are made considering the different stiffener configurations considered in the current study. The main observations from the study can be summarized as follows:
For unstiffened plates with circular openings:

The slenderness ratio has no significant effect on the local buckling coefficient.

For aspect ratios 0.5 and 1.0, the buckling coefficient factor decreases as the opening size increases and the opening location comes near to the center of the plate, and the percentage of decrease reaches 35% of the solid plate strength.

For aspect ratios 1.5 and 2.0, the buckling coefficient factor decreases when the opening diametertowidth ratio (OPH/W) is 0.1 for all opening positions. While buckling coefficient ratio starts with values less than one when the opening position with respect to the Xdirection to width ratio (OPX/W) is 0.1, then it increases gradually till the opening comes to the center of the plate.
For plates stiffened with stiffeners parallel to load direction:

For aspect ratios 0.5 and 1.0 and for all opening sizes, the buckling coefficient ratio for stiffened to unstiffened plates with opening (K_{s}/K_{o}) increases gradually as the opening moves towards the center of the plate.

The buckling coefficient ratio for stiffened plates with a circular opening to solid plate (K_{s}/K_{no}) is greater than 1 for all opening sizes and positions.

For aspect ratios 1.5 and 2.0, the buckling coefficient ratio for stiffened to unstiffened plates with opening (K_{s}/K_{o}) is greater than 1.0 for all opening positions, but it decreases gradually while opening moves towards the center.

For all aspect ratios except when Î± = 1.5, the change of stiffeners breadth with respect to the opening diameter (B_{s}/OPH) has a minimum effect on the local coefficient ratio for stiffened to unstiffened plates with opening (K_{s}/K_{o}); therefore, it could be neglected.
For plates stiffened with stiffeners perpendicular to load direction:

For aspect ratios 0.5 and 1.0, the buckling coefficient ratio for stiffened to unstiffened plates with opening (K_{s}/K_{o}) is greater than 1.0 for all opening sizes and positions.

The buckling coefficient ratio of stiffened plates with a circular opening to solid plate ((K_{s}/K_{no}) becomes less than 1 for all opening sizes and positions, while it becomes greater than 1.0 for aspect ratio equals to 1.0.

For all aspect ratios, the change of stiffener breadth with respect to the opening diameter (B_{s}/OPH) has a minimum effect on the local coefficient ratio for stiffened to unstiffened plates with opening (K_{s}/K_{o}). Therefore, it could be neglected.
For plates stiffened with box stiffeners:

For opening moves in X and Ydirections, the elastic buckling coefficient ratio (K_{box st}/K_{o}) increases from 1 to 2.5 as the opening moves towards the center and as the opening size increases.

When compared to stiffeners parallel or normal to load direction and opening moves in the Xdirection, their effect is almost the same with a slight decrease when opening reaches the center of the plate when OPH/W = 0.1â€“0.3, while it generally increases the strength when OPH/W = 0.4â€“0.5, but the strength decreases obviously when the opening comes near to center.

When compared to stiffeners parallel to load direction and opening moves in the Ydirection, stiffeners parallel to the load direction give more strength than box stiffeners for all cases.

When compared to stiffeners normal to load direction, the elastic buckling coefficient ratio (K_{box st}/K_{vl st}) is less than 1 when OPH/W = 0.1â€“0.3, while it increases when OPH/W = 0.4â€“0.5 till it becomes 2.14, but it decreases gradually when the opening comes near to center without being less than 1.
According to the extensive performed parametric study, an empirical formula is derived to estimate the buckling factor coefficient for unstiffened and stiffened steel plates with circular openings.
Availability of data and materials
The data that support the findings of this study are available from the authors upon reasonable request.
Change history
24 December 2022
We have updated with a better quality the Fig. 2 and Fig 21.
Abbreviations
 B _{s} :

Stiffener breadth
 D :

Plate height
 H _{s} :

Stiffener length
 K :

Buckling factor
 K _{no} :

Buckling factor of solid plate
 K _{o} :

Buckling factor of an unstrengthened plate with circular opening
 K _{s} :

Buckling factor of a strengthened plate with circular opening
 LS:

Longitudinal stiffener
 m :

No. of half waves
 N _{cr} :

Critical buckling load
 OPH:

Circular opening diameter
 OPX:

Edge distance from the center of the opening along the Yaxis
 OPY:

Edge distance from the center of the opening along the Xaxis
 t _{b} :

Plate thickness
 t _{s} :

Stiffener thickness
 TS:

Transversal stiffener
 W :

Plate length
 Î± :

Plateâ€™s aspect ratio
 Î’ :

Stiffener breadthtodiameter ratio
 Î» :

Widthtothickness ratio
 Ï¬ _{cr} :

Critical buckling stress
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MM performed the conception, designed the work, aided with the analysis and interpretation of data, and created the first draft. SM performed the literature review, applied analysis, and interpretation of data. MH aided in the conception of work, approved the research work plan, and revised results and writing. AF approved the research approach, design of the work plan, and final version of the thesis and manuscript. The manuscript is a byproduct of a M.SC. supervised and approved by MM, MH, and AF. All authors have read and approved the manuscript.
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Maha M. Hassan is on leave from Cairo University.
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Hassan, M.M., Mahmoud, S.I., Serror, M.H. et al. Elastic buckling of simply supported stiffened steel plates with circular opening. J. Eng. Appl. Sci. 69, 106 (2022). https://doi.org/10.1186/s44147022001567
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DOI: https://doi.org/10.1186/s44147022001567