Numerical and Experimental Research on Similarity Law of the Dynamic Responses of the Offshore Stiffened Plate Subjected to Low Velocity Impact Loading

Abstract

Similarity laws of scaled models of offshore platform deck structures under low velocity impact loading are proposed in the present research. The similarity laws of scaled models with different scaling factors are established in forms of dimensionless factors with consideration of flow stress differences of the materials. A dimensionless displacement is defined by dividing displacement by plate thickness and a dimensionless force is defined by dividing force by flow stress and plate thickness; then, a dimensionless force-displacement relationship is established. Dynamic responses of three geometrically similar stiffened structures with scaling factors of 1:4, 1:2, and 1:1 subjected to the dropping impact of a rigid triangular pyramidic impactor are investigated by an experimental test and a finite element analysis. Results show that dimensionless force-displacement curves of geometrically similar plates coincide with each other; meanwhile, the difference of maximum impact force for the three structures with various scaling factors is less than 5%, and the difference of maximum impact depth is less than 1%, which definitely show the effectiveness of the scaling laws based on dimensionless factors. The present research provides useful insight into the similarity laws of dynamic responses of deck structures subjected to falling object impact and would be used in the crashworthiness research and design process of the offshore structures.

1. Introduction

Low velocity impacts of ships and offshore structures, including collision and grounding, floating object collision and falling object impact, are prone to catastrophic disasters. Thus, researchers worldwide pay particular attention to investigations of ship structure collisions, as plenty of useful conclusions have been obtained by analytical investigations, numerical research and experimental tests [1,2]. Among these investigations, important factors such as impact load, stress distribution, damage initiation and propagation would be obtained by experimental research; furthermore, experimental test results provide benchmark studies for numerical simulations and analytical research. Thus, experimental methods play an irreplaceable role in collision research.

A small-scaled model test has been mainly adopted in ship collision research for the purpose of reducing difficulty and economic consumption [3,4]. One of the most important factors is to establish the similarity laws between the scaled model and the prototype. Jones [5] proposed the similarity law to transfer the scaling model impact test results into the prototype impact results. Calle [6] proposed a scaling law with consideration of material yield, material strain hardening, damage initiation and strain rate effect.

The above-mentioned research provides support for the extension of scale model test results to full-scaled prototypes for ship collisions. However, the research mentioned above mainly focuses on collisions of ship side structures, and few investigations have been proposed on research of deck structures under the impact of dropping objects; thus, similarity laws of structure models with different scaling factors should be considered. The present research conducts tests on similarity laws of scaled models of an offshore platform deck structure under low velocity impact of dropping objects. The first step is to propose the similarity laws between a small-scaled model and a full-scaled prototype, and to introduce a couple of dimensionless factors; the following step is to establish three geometrically similar stiffened plate structures with different scaling factors; then, experimental and numerical simulation research on low velocity impact has been completed and the last step is to analyze the experimental and numerical results with the dimensionless factors. Finally, the similarity laws are verified.

2. Similarity Laws

Generally, a dynamic impact test is conducted on a geometrically similar small-scaled model to obtain dynamic responses with consideration of economical consumption. In this series of research, a prototype means a model which is the same as the stiffened plate of a real offshore structure; they have the same length, width, the same shell thickness, the same stiffeners and the same stiffener spaces. Meanwhile, the scaled model is geometrically similar to the prototype, whereas they are of the same shape but a different size. Furthermore, the scaled models and the prototype are usually manufactured with the same material and the same fabrication method.

Thus, the first priority is to establish scaling principles between scaled model and prototype. For a full-scaled prototype model and the corresponding geometrically similar small-scaled model, the relationships between the characteristics of the scaled model and the prototype are established by using the scaling factor [5]. The scaling factor $\beta$ between the geometrically similar small-scaled model and the full-scaled prototype is defined as:

$$\beta =L_s/L_p$$

(1)

where L_S means length of the scaled structure and L_p means length of the full-scaled prototype. As well, in a low velocity impact scenario the impact displacement, shell thickness, impact force and energy absorption follow the following scaling principle:

$${\Delta }_s:{\Delta }_p=\beta :1$$

(2)

$$t_s:t_p=\beta :1$$

(3)

$$F_s:F_p={\beta }^2:1$$

(4)

$$E_s:E_p={\beta }^3:1$$

(5)

These similarity laws were established under the assumption that the small-scaled model and the full-scaled prototype were fabricated by the same material with the same values of mass density (ρ), elastic module (E), Poisson’s ratio (μ), yield strength (σ_s) and ultimate strength (σ_b). However, experimental test results show that yield strength and ultimate strength of the plates with different thicknesses are slightly different in many cases. Thus, the influence of the differences of yield strength should be considered in the scaling laws. Previous experimental and theoretical studies show that the impact force is proportional to the flow stress of the materials [4,7]:

$$F\propto {\sigma }_0$$

(6)

where (σ₀) = (σ_s + σ_b)/2 means the flow stress of the materials, and which equals to the average value of yield stress and ultimate strength. Thus, the influence of the differences of flow stress should also be considered in the scaling law; an effective way is to establish a couple of dimensionless factors. A dimensionless displacement is defined by dividing displacement by shell thickness and a dimensionless impact force is defined by dividing force by flow stress and shell thickness:

$$\left\{\begin{array}{c}{\overline{\Delta }}_s=\frac{{\Delta }_s}{t_s},\hspace{1em}\hspace{1em}\hspace{1em}{\overline{\Delta }}_p=\frac{{\Delta }_p}{t_p}\\ {\overline{F}}_s=\frac{F_s}{{\left({\sigma }_0\right)}_s · t_s^2},\hspace{0.17em}\hspace{0.17em}{\overline{F}}_p=\frac{F_p}{{\left({\sigma }_0\right)}_p · t_p^2}\end{array}\right.$$

(7)

In the same way, the dimensionless energy absorption is also defined as:

$$\left\{\begin{array}{c}{\overline{E}}_s=\frac{E_s}{{\left({\sigma }_0\right)}_s · t_s^2 · t_s}=\frac{E_s}{{\left({\sigma }_0\right)}_s · t_s^3}\\ {\overline{E}}_p=\frac{E_p}{{\left({\sigma }_0\right)}_p · t_p^2 · t_p}=\frac{E_p}{{\left({\sigma }_0\right)}_p · t_p^3}\end{array}\right.$$

(8)

In Equations (1)–(8), the symbols with subscript “s” represent the physical quantity of the small-scaled model, whereas the symbols with subscript “p” represent the physical quantity of the full-scaled prototype; the same as below, as shown in

Table 1. Meaning of the symbols of small-scaled model and full-scaled prototype.

	Small-Scaled Model	Full-Scaled Prototype
Length	Ls	Lp
Shell thickness	ts	tp
Displacement	Δs	Δp
Impact force	Fs	Fp
Energy absorption	Es	Ep
Flow stress of material	(σ0)s	(σ0)p
Dimensionless displacement	${\overline{\Delta }}_s$	${\overline{\Delta }}_p$
Dimensionless impact force	${\overline{F}}_s$	${\overline{F}}_p$
Dimensionless energy absorption	${\overline{E}}_s$	${\overline{E}}_p$

. Theoretically, the dimensionless impact force and energy absorption of the scaled model should be equal to those of the full-scaled prototype under the same dimensionless displacement. In another way, the dimensionless force-displacement curves and dimensionless energy absorption curves of models with different scaling factors should be the same shape.

3. Materials and Methods

Three types of geometrically similar stiffened plate models with different scaling factors were designed, an impact tower for drop weight impact was established, and an FEA (finite element analysis) of the dynamic impact scenarios was conducted for further investigations.

3.1. Specimens

Rectangular stiffened steel plates, which were derived from the deck structure of an offshore platform, were conducted in the present research. Three similar specimens, including two small-scaled models with a 1:4 and a 1:2 scaling factor, and one full-scaled prototype, were proposed. As shown in Figure 1 and Figure 2, three geometrically similar specimens were stiffened by three uniformly distributed L-shaped stiffeners. The thicknesses of the plates were 3.9 mm, 7.8 mm and 15.6 mm, respectively.

Since the sharp edge of the dropping container would cause deck damage in case of falling, a rigid triangular pyramidic impactor derived from a container was conducted with the length of the edge “L” equal to 200 mm, as shown in Figure 3. The impactor was fabricated with abrasive steel, and a heat treatment process ensured its surface hardness.

3.2. Experimental Set-Up

The low velocity impact was carried out by the weight drop impact test tower. As shown in Figure 4, the test specimen was located at the bottom of the tower. In order to prevent the specimen from bounding or sliding away, the specimen was clamped by a dozen of bolts located around the stiffened plate during the impact process. The impactor was guided by two vertical rails and consisted of three parts: an impactor, a force transducer and the mass. During the impact process, the initial impact energy was achieved by adjusting the drop height and the mass property of the impactor; contact force versus time history could be achieved by the piezo-electric force transducer connected to the impactor under a sampling frequency of 40 kHz. The vertical displacement of the impactor was tested by the laser displacement transducer, and furthermore, the initial impact velocity was calculated by the differential of displacement. Then, energy absorption during the impact procedure could be calculated by trapezoidal numerical integration of the force–displacement curve. The piezo-electric force transducer, with a code number of L1100–909543, was fabricated by Xiyuan Electronic Technology Co., Ltd, Yangzhou, China. The laser displacement transducer, with a code number of HG–C 1400, was fabricated by Panasonic Co., Ltd, Kasugai, Japan.

3.3. Finite Element Method

For the numerical simulation of low velocity impact, the commercial package ABAQUS/Explicit with a non-linear explicit algorithm was implemented. As shown in Figure 5, the numerical model consisted of two parts, the impactor and the specimen. The triangular pyramidic impactor was modeled as a rigid body, and a concentrated mass point was defined to simulate the mass of the impactor. The specimens with different scaling factors were modeled by shell model. Marinatos [8] suggested that the aspect ratio of the elements was kept as close as possible to 1:1, and l_e/t ≤ 1 (where l_e means the element size, and t means the shell thickness) led to better reproduction of the experimental results; thus, S4R elements (4-node doubly curved shell reduced integration elements) with sizes of 4 mm, 8 mm and 16 mm were used to discretize the specimens in the 1:4 scaled model, the 1:2 scaled model and the full-scaled prototype, respectively. In the numerical models, an automatic surface to surface contact strategy provided by ABAQUS/Explicit (Version 6.11, created by Dassault System, permission from Huazhong University of Science and Techonolgy, Wuhan, China) was selected to simulate the contact problem. The friction coefficient was set to 0.3 for the tangential contact surfaces, which was proven to be efficient to match with the experimental results in previous studies [9,10]. Boundaries of the stiffened plate were modeled as fully clamped, whereas the freedom of the pyramidic impactor was restricted except in the vertical impact direction. Furthermore, a predefined field built into the software was adopted to define the initial impact velocity of the impactor.

The built-in ductile damage model built into the ABAQUS software was employed to characterize the mild steel material. Tensile tests were conducted under the guidance of GB/T 228-2002, a metallic materials–tensile test at ambient temperature. The uniaxial tensile tests were implemented by a universal tension test machine with a code number of WAW–600 E, fabricated by Chuance Test Machine Co., Ltd, Jinan, China. A dog-bone specimen shown in Figure 6 was cut down from the plate by wire electrical discharge, and uniaxial tensile curves of the specimens were carried out by the universal tension test machine under a tension velocity of 3 mm/min.

Based on the tensile test results, a combined material relationship was adopted to express the true stress-strain curves. The true stress-strain relationship before necking was proposed as follows:

$${\epsilon }_t=ln\left(1+{\epsilon }_n\right), {\sigma }_t={\sigma }_n\left(1+{\epsilon }_n\right)$$

(9)

where ε_n and σ_n represent the nominal strain and nominal stress, respectively, and ε_t and σ_t represent the true strain and true stress, respectively. Since fracture strain defined in the finite element software was larger than that obtained by the tensile test, the true stress-strain relationship σ_t − ε_t beyond necking was expressed by using upper power law and lower power law [11]:

$${\sigma }_t={\sigma }_t^0\left[0.5\times \left(1+{\epsilon }_t-{\epsilon }_t^0\right)+0.5\times {\left({\epsilon }_t/{\epsilon }_t^0\right)}^{{\epsilon }_t^0}\right]$$

(10)

where ${\sigma }_t^0$ and ${\epsilon }_t^0$ represent the true stress and true strain at the necking point [10]. Nominal stress-strain curves and true stress strain curves of the plates with different thicknesses are shown in Figure 7. Then, the material properties of the steel were defined in the ABAQUS software. The elastic module of the steel is defined as 210 GPa, a density of 7800 kg/m³ and a Poisson’s ratio of 0.3, and plastic behaviors of the steel were defined by the curves in Figure 7.

A ductile failure criterion built into the ABAQUS software, which simulated the damage initiation and propagation of the ductile mild steel with acceptable accuracy [12,13], was adopted to simulate failure behavior. In this criterion, damage initiation and evolution were determined by an indicator, which was a function of the equivalent plastic strain and stress triaxiality. Once damage initiation occurred at a certain point, the material stiffness degradation occurred at that point correspondingly. When the stiffness degradation reached a critical value, the material point was assumed to fail, and the corresponding element was deleted. In the low velocity impact scenarios, such as ship collision and falling object impact, the impact velocity was far lower than the wave speed in the mild steel, and the strain rate effect slightly affected the dynamic responses. Thus, the strain rate effect was neglected in the numerical simulation of the impact process [10,14].

4. Results and Discussion

In terms of the impact force response and the deformation mode, the numerical simulation results match well with the experimental results. In both the experimental test and the numerical simulation, the initial impact energy was adjusted by adjusting the mass property and the impact velocity; details were listed in

Table 2. Impact velocity and energy in impact test.

Scaling Factor	Mass (kg)	Impact Velocity (m/s)	Initial Impact Energy (J)
1:4	362.2	5.00	4528
1:2	502.2	8.75	19,224
1:1	795.0	11.30	50,757

. As shown in Figure 8 and Figure 9, the plates were torn by the sharp rigid impactor and the deformed shape was similar to the shape of the impactor. Due to the sharp corner of the rigid impactor, firstly, the plates underwent a premature fracture, then were torn with three cracks. Due to the strengthening effect of the stiffener, the damage area was located between two stiffeners next to the impact point, and the stiffeners did not suffer obvious plastic deformation. Figure 10 presents the impact force-displacement curves, and the numerical simulation results match well with the experimental test results. As the impactor fell, the impact force raised rapidly until the premature fracturing of the plate; then, the force raised with the tearing of the plate; at the last step, the impact rebounded due to the elastic energy of the stiffened plate.

The similarity rules were verified by comparing dimensionless force-displacement relationships of models with different scaling factors. Yield stress, ultimate stress and flow stress of the plates with different thicknesses were listed in

Table 3. Necessary stress of the materials gained by a tensile test (unit: MPa).

Shell Thickness	Yield Strength	Ultimate Strength	Flow Stress
3.9 mm	473	758	615
7.8 mm	433	667	550
15.6 mm	376	635	506

; thus, the curves shown in Figure 10 were converted to non-dimensional forms by the Equation (7), and the non-dimensional curves were shown in Figure 11. Since agreement between the FEA results and the impact test results were achieved in Figure 10, only the simulation results were listed in Figure 11 for the purpose of clear and concise expression. It was shown that the three curves coincide with each other perfectly; the maximum impact displacement and the residual plastic deformation significantly decreased with an increase in the scaling factor. The main reason for the differences was that the 1:2 scaled model and full-scaled prototype underwent a relatively “low energy impact” compared with the 1:4 scaled model. For the 1:4 scaled model, 1:2 scaled model and full-scaled prototype, the initial dimensionless impact energy, which were calculated by Equation (8), were 124.1, 73.7 and 26.4, respectively. The main reason for adopting a relatively “low energy impact” for the 1:2 scaled model and the prototype was that the impact tower cannot withstand such a high energy impact test. For instance, the initial energy should be set to 2.38 MJ for the full-scaled prototype under a dimensionless initial energy of 124.1.

For further investigation, high energy impact scenarios with the same dimensionless initial energy were carried out by the FEA, and agreement was achieved. In the numerical models, the dimensionless initial impact energy was set to 124.1 under the same impact velocity of 5 m/s, which means that the mass property of the impactor was adjusted to fulfill the demands of the initial impact energy. More details in the finite element model were listed in

Table 4. Mass property, impact velocity and energy in finite element analysis.

Scaling Factor	Mass (kg)	Impact Velocity (m/s)	Initial Impact Energy (J)	Initial Dimensionless Energy
1:4	362.2	5.00	4528	124.1
1:2	2591.4	5.00	32,393	124.1
1:1	19,072.3	5.00	2,384,038	124.1

. The calculated results of dimensionless force-displacement curves were shown in Figure 12; there were slight fluctuations in the curves mainly due to elastic waves in the structure and the element deletion strategy adopted in the finite element model. To avoid unexpected distortion of the elements, the failed elements were deleted during the simulation process. Thus, a slight drop–down of the impact force occurred as soon as an element was deleted. Except for the slight fluctuations, the three curves almost coincided with each other perfectly, which verified the correctness and effectiveness of the similarity laws.

5. Conclusions

Similarity laws of scaled models of offshore platform deck structures under low velocity impact of dropping objects were conducted in the present research. The similarity laws of scaled models with different scaling factors were proposed. The dynamic responses of three geometrically similar stiffened structures with scaling factors of 1:4, 1:2, and 1:1 under the dropping impact of a triangular pyramidic impactor were investigated by experimental and numerical methods, and the useful conclusions are listed below:

(1)

Similarity laws between scaled models and prototypes of stiffened structures under low velocity impact were established, in forms of dimensionless factors including dimensionless force and displacement, with consideration of flow stress of the different plates.

(2)

Finite element results and experimental tests show that the dimensionless force–displacement curves of different models match well, which show the effectiveness of the similarity law.

(3)

Stiffened plates of an offshore platform deck would suffer a premature fracture under the impact of a sharp triangular pyramidic impactor; the structure could still withstand impact energy absorption after fracture initiation due to tearing of the plate.

The present research provides useful insight into the similarity laws of dynamic responses of deck structures subjected to falling object impact, and were used in the crashworthiness research of offshore structures.