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Article

A Method for Calculating the Velocity of Corner-to-Corner Rear-End Collisions of Vehicles Based on Collision Deformation Analysis

School of Transportation Engineering, Dalian Jiaotong University, Dalian 116028, China
*
Author to whom correspondence should be addressed.
Appl. Sci. 2021, 11(22), 10964; https://doi.org/10.3390/app112210964
Submission received: 30 September 2021 / Revised: 9 November 2021 / Accepted: 16 November 2021 / Published: 19 November 2021
(This article belongs to the Section Transportation and Future Mobility)

Abstract

:
To improve the efficiency of solving vehicle collision velocity and provide sufficient evidence for the identification of accident responsibility, we proposed a method combining the momentum equation and finite element simulation. We built a finite element simulation model of a vehicle where multiple collision simulation experiments were carried out, and studied the calculation method of collision deformation. After fitting and analyzing the simulated deformation data of an accident vehicle under different velocities through collision simulation experiments, a relationship model between collision velocity and deformation was established, and a method to solve the collision velocity was proposed by combing the existing two-dimensional collision momentum equation of the vehicle. For actual collision cases, the proposed velocity solution method and the simulation software were used for reconstruction analyses, respectively, and the results of the instantaneous contact velocity of vehicle collision were compared. It was found that the velocity calculation results obtained using the two methods above were in good agreement; the shape and depth of the simulated deformation were consistent with the actual deformation of the vehicle.

Graphical Abstract

1. Introduction

With the rapid development of the global economy and the rapid growth of vehicle ownership, vehicles have become an important means of transportation for people, but at the same time, road traffic accidents have also become a global public hazard. Once a vehicle crash has happened, it is impossible to reappear. This irreversible characteristic makes it difficult to accurately determine a vehicle’s velocity before collision, causing a great deal of inconvenience in identifying accident liability, especially if the parties involved have different opinions on the circumstances of the accident. In numerous vehicle collision accidents, corner-to-corner rear-end collisions of vehicles are more common, especially in urban road systems. Therefore, it is necessary to use relevant technical means to find a solving method to study the collision velocity of corner-to-corner rear-end vehicle collision accidents.
At present, scholarly research is mainly focused on dynamic calculations and finite element analyses. In terms of dynamic calculations, the National Highway Traffic Safety Administration (NHTSA) has successfully developed the world’s first vehicle crash simulation software, SMAC [1], which is mainly used for simulation analyses of collisions between two vehicles, and in which the theoretical model is mainly based on numerical solution of classical Newton’s laws. According to the relationship between the average impact force of a vehicle and residual deformation, a model was built, and CRASH analysis software was developed [2]. Dr. Hermann Steffan from Austria constructed the model based on the momentum theory and PC-Crash simulation software based on the Kudlich-Slibar model [3]. Zhang and Huang et al. studied a dynamic model of vehicle-to-vehicle collision and concluded that vehicle collision parameters can be optimized using the wheel imprint and the stationary position of the vehicle. They also put forward the error factors of a stationary vehicle, in the middle position, and on a direction angle, and established the objective function of collision parameter optimization. Based on actual accident cases, PC-Crash software was used to simulate the accident and verify the effectiveness of the vehicle-to-vehicle collision dynamics model [4,5].
On this basis, Inhwan et al. proposed an analysis method based on qualitative vehicle collision mechanics using the law of conservation of momentum [6]. Zou et al. analyzed the uncertainty of accident reconstruction using mathematical theory, transformed it into a problem of extreme value, and proposed a simplified algorithm for accident reconstruction. The algorithm was applied to cases of actual accidents, and error analysis showed that the algorithm could be used in road accident reconstruction within an acceptable range [7].
Based on momentum conservation, information regarding body deformation was used. According to the theory of the relationship between deformation and energy, Guo obtained a reconstruction method for traffic accidents and found that the collision deformation was consistent with that of the accident vehicle through calculations of actual accident cases [8]. Zhiqiang et al., using PC-Crash simulation software and the principle of energy and momentum conservation, analyzed the relationship between total deformation energy and velocity before collision, and proposed an energy-based model for calculating the side impact velocity of a vehicle, of which the validity was verified using numerical simulations [9]. Voevodin et al. proposed a calculation model of vehicle driving dynamics during collision by studying the destruction of vehicle elements after collision [10].
Vangi has performed a great deal of research in reducing errors and improving efficiency. In order to reduce errors in the process of vehicle collision, a computational model of linear vehicle velocity and angular velocity was proposed to analyze the phase of a vehicle after collision [11]. In order to quickly calculate the energy loss during collision, a “triangle method” for defining body damage was proposed [12]. In addition, in order to reduce the calculation time, a reduced order model for accident reconstruction was proposed, which accurately calculated kinematic data and deformation of the vehicle [13]. Ji et al. used energy loss-based vehicular injury severity (ELVIS) to describe the impact of energy absorption during vehicle collisions, and a regression model was used to study the relationship between injury and collision mechanisms [14].
From the aspect of finite element simulations, Day and York improved the finite element collision method for automobiles and increased the efficiency of finite element simulation analysis [15]. For vehicle-pier collision accidents, El-Tawil et al. used the inelastic transient finite element method to reconstruct an accident and obtained deformation data under different conditions by changing the velocity. Through analysis of the experimental results, some suggestions for collision design specification were put forward [16]. Fahlstedt et al. built a finite element collision model of vehicles and carried out simulation analyses to study the effects of the initial impact velocity and angle on the results of accident reconstruction [17]. Macurová et al. discussed the possibility of studying the value of energy-equivalent velocity using PC-Crash software and provided a theoretical basis [18]. Based on finite element simulation, Evtiukova proposed a method to calculate vehicle velocity through vehicle collision deformation, but it is only applicable for calculating the velocity of frontal vehicle collisions with non-deformable obstacles [19].
In order to improve the simulation efficiency of finite element simulation, Zhang et al. used the method of combining neural networks and finite element analysis to simulate vehicle collision accidents and found that the application of neural networks can improve the simulation efficiency; thus obtaining the relationship between initial vehicle collision parameters and deformation. Used to verify cases of typical accidents in which the pre-collision velocities were obtained, the method is noted as being applicable for vehicle accidents without tire tracks [20]. Chen et al. developed an artificial neural network method using virtual collision data generated by finite element simulation software, and proved that plastic deformation characteristics can effectively invert the data before vehicle collision [21].
To sum up, research in the field of vehicle collision is based on a single theory and lacks mutual combination. A calculation method based on the dynamics principle fails to take advantage of the important information of vehicle collision deformation, and the reliability of velocity results is insufficient. The finite element reconstruction-based method requires repeated simulation experiments to determine the velocity at the moment of vehicle collision contact, which is inefficient; moreover, the vehicle finite element model has a strong directivity and it is difficult to apply it to other accidents.
In view of the above, with our focus on corner-to-corner rear-end vehicle collision accident patterns, we constructed a vehicle collision model, obtained collision deformation results at different velocities with the help of a large number of finite element collision simulation experiments, and established a relationship model between impact velocity and deformation through data fitting. A method for calculating the impact velocity based on classical mechanics and the finite element method is proposed using the existing vehicle collision momentum equations. The empirical results have important theoretical significance in revealing the formation mechanism of vehicle collision deformations and developing a theory of accident-reconstruction analysis, and also have important value for practical applications in improving the level of accident reconstruction analysis and accident handling as well as the determination of responsibility.

2. Collision Simulation Experiment

2.1. Design of the Experiment

Two vehicles drove in the same direction from front to back (the rear vehicle is defined as vehicle 1 and the front vehicle is defined as vehicle 2). Vehicle 2 slowed down and changed lanes, and vehicle 1 cannot avoid it, resulting in a diagonal rear-end collision. During the collision, the included angle between vehicle 1 and vehicle 2 was 15°.
The vehicle collision model was built using Ls-Prepost and the model and mesh were optimized using HyperMesh software. The areas that had a great impact on the results were finely divided, and the mesh size of the other areas was increased appropriately. The initial velocity of vehicle 1 and vehicle 2 was 25 km/h and 20 km/h, respectively, with an additional gradient of 5 km/h. The ending velocity of the experiment was 65 km/h and 60 km/h, respectively. The simulation experiment of 30 km/h−20 km/h was introduced as an example. LS-DYNA was used to simulate the angular and diagonal rear end collision under different combinations of velocities. After verifying the reliability of the vehicle model, the vehicle deformation data were obtained using post-processing software, and then follow-up data analysis was carried out. The simulation experiment process is shown in Figure 1.

2.2. Finite Element Model of Vehicle

(1) Material Property
According to materials of actual vehicle bodies, the material properties of the vehicle model were set [22]. The material parameters of the main body parts are shown in Table 1.
(2) Contact Way
The possible contact of the vehicle was set using Ls-Prepost software. Contact among the parts of the vehicle was set using the keyword *CONTACT *AUTOMATIC_SINGLE_SURFACE. The contact settings among the vehicle bodies were set using *AUTOMATIC_SINGLE_SURFACE_TO_ SURFACE in the *CONTACT keyword. Because the instantaneous automobile collision process is generally 70–120 ms, the friction between the vehicle’s tires and the ground was ignored.
(3) Basic Parameter Setting
The velocity of vehicle 1 was set to an X-axis component of 8333.33 mm/s, and a Y-axis component of 0 mm/s; the velocity of vehicle 2 was set to an X-axis component of 5366.28 mm/s and a Y-axis component of 1437.89 mm/s, with a pre-collision horizontal distance of 7.3 mm and an angle of 15°. To ensure that the model collision was fully effective in the simulation experiment, the termination time of the experiment was 130 ms and the hourglass coefficient was a default value of 0.1.

2.3. Model Checking

(1) System Energy Analysis
The energy conversion curves of the collision process were obtained through a hypergraph, from which can be seen that at t = 0.02–0.04 s, the kinetic energy and internal energy curves change significantly at the moment of vehicle collision and the curve of total energy basically remains stable; after t = 0.08 s, the kinetic energy and internal energy curves remain horizontal, indicating that the energy conversion at the moment of vehicle collision is over. Overall, the kinetic energy of the system is converted into internal energy in the collision process, and the total energy remains the same.
The post-processing software calculated that the percentage of the hourglass energy to the total energy of the system was 0.8%, and the mass increase was 0.99%, both of which were far less than 5%, making the impact negligible [23]. Therefore, the finite element model is reasonable.
(2) Vehicle Velocity Analysis
By observing the change curve in the vehicle velocity, it could be found that the velocity of vehicle 1 decreased significantly, while that of vehicle 2 increased. After t = 0.12 s, the velocity of vehicle 1 dropped to about 6.67 × 103 mm/s, and the velocity of vehicle 2 increased to 7.1 × 103 mm/s, as shown in Figure 2. By comparing the velocity differences between the two vehicles, it can be inferred that the two vehicles were in a collision separation state. The change of velocity conforms to the law of real vehicle collision velocity.
The finite element model of the whole vehicle was reasonably established through comprehensive analyses, and the collision simulation experiments also met the objective laws and relevant requirements.

3. Methodology

3.1. Calculation Method of Deformation

Calculation steps of the deformation are: ① determine the deformation range; ② determine key points; and ③ calculate the deformation with the help of a formula. Taking vehicle 1 as an example, in the upper, middle, and lower horizontal positions of the front deformation area, an average of 4 key points was selected for each row. The key points of each row and column were required to be on the same straight line with the deformation range divided into six regions by key points, and the overall deformation of the deformation area was calculated by the deformation of these key points. The selection of the key points is shown in Figure 3.
The overall deformation (C) calculation formula is:
C = C x 2 + C y 2 + C z 2
In the formula, Cx, Cy, and Cz are the deformation amount of the deformation area in the X, Y, and Z directions, respectively, which is obtained by calculating the average value of the key points in these directions.
Deformation data of the key points of vehicle 1 are shown in Table 2.

3.2. Data Collection

In the same way, the deformations of the two vehicles after experiments under different velocities were calculated, and the statistics are shown in Table 3.

3.3. Data Fitting

The experimental data were fitted many times to obtain a three-dimensional surface diagram of the relationship between the deformation and driving velocity (as shown in Figure 4), and the corresponding relations (2) and (3) were established.
X 1 = A 1 i v 1 3 + A 1 i v 2 3 + A 1 i v 1 2 + A 1 i v 2 2 + A 1 i v 1 2 v 2 + A 1 i v 1 v 2 2 + A 1 i v 1 + A 1 i v 2 + A 1 i v 1 v 2 + b 1
X 2 = A 2 i v 1 3 + A 2 i v 2 3 + A 2 i v 1 2 + A 2 i v 2 2 + A 2 i v 1 2 v 2 + A 2 i v 1 v 2 2 + A 2 i v 1 + A 2 i v 2 + A 2 i v 1 v 2 + b 2
In Formulas (2) and (3), b 1 = 62.94 , b 2 = 28.49 . The values of A 1 i and A 2 i are shown in Table 4.
For research on the solution of the vehicle collision velocity, the basic equation for two-dimensional eccentric dynamics was determined according to the momentum equation and the momentum conservation law [24]. For the establishment of the equations, some scholars used the elastic coefficient of restitution and some introduced a relative friction coefficient and other methods, but the selection of coefficients inevitably involves personal subjective thinking, which will reduce the credibility of the results. Therefore, the relationship between the amount of deformation and the driving velocity ((2) and (3)) are used as equations, which are combined with the dynamics equations to build the calculation model of vehicle collision dynamics parameters.

4. Case Study

4.1. Brief Case

In December 2009, near the intersection of Xinyang Road and Anguang Street in Daoli District, Harbin, China, a black Audi and a white Jetta were driving in the same direction from east to west when a rear-end collision occurred, causing damage to both vehicles. It is known that the accident occurred in winter, on an icy, snowy road and at a gradient of 2.8%. The total mass of the Audi was 1200 kg, and the total mass of the Jetta was 2025 kg. When the two vehicles were stationary, the base of the left rear wheel of the Jetta and Audi front right wheel were 1.6 m apart; tire brake tracks were 8 m and 8.5 m, respectively; and the collision angle of the two vehicles was 15°.

4.2. Case Solving

(1) Model Solving
Calculated according to the vehicle’s trace inspection report: the overall deformation of the Audi was 30 mm and the overall deformation of the Jetta was 122 mm.
X1 = 30 mm, X2 = 122 mm are brought into Formulas (2) and (3), the v1 of Audi and v2 of Jetta before collision are obtained:
v1 = 35.42 (km/h)
v2 = 32.20 (km/h)
By using the two-dimensional dynamic equation and the slip trajectory equation, the instantaneous velocities after collision are obtained: v1′ = 32.86 (km/h), v2′ = 33.77 (km/h); angular velocity: w1 = −0.45 rad/s, w2 = 0.86 rad/s.
According to the parameters of the accident vehicles, finite element models of the Audi and Jetta were established. The obtained values for the velocities were taken as the driving value of velocity, and the instantaneous motion state of the vehicles was reproduced by LS-DYNA.
The collision between two vehicles led to the conversion of system energy. It can be seen in Figure 5 that, during the collision, the vehicle running velocities decreased suddenly, and the corresponding kinetic energy also changed, with the overall kinetic energy of the system decreasing from 64,244,600 MJ to 60,928,400 MJ. Due to the collision friction, the internal energy increased from 0 MJ to 2,795,150 MJ, and the vehicle collision experienced a conversion from kinetic energy to internal energy. Owing to the limitations of the experimental setup, the hourglass energy of 521,050 MJ generated during the simulation was much less than 5% of the total energy. The experiment accords with the objective facts and the law of energy conservation; therefore, the obtained data have a certain credibility.
(2) Simulation reconstruction.
PC-Crash software is a mature simulation software with a long history of use and high authority in the field of automobile collisions. The above-mentioned traffic accident was reconstructed with the help of PC-Crash.
After constant adjustment of the experimental parameters, it was finally determined that when the velocity of the Audi was 33.91 km/h and the velocity of the Jetta was 33.53 km/h, the trajectory of the vehicle after the collision, the stopping location, and the collision position were closest to those of the actual scene. The stopping location of the accident vehicle, the collision point, and the slip trajectory of the simulated vehicles are shown in Figure 6.

4.3. Result Analysis

Table 5 shows the results obtained from the two calculation methods and compares the relative errors.
The results show that the relative error of the two methods is less than 5%, which indicates that the calculation results of the mathematical model are close to those of the PC-Crash simulation.
Through the finite element simulation experiment, it is found that the simulation experiment is consistent with the actual deformation parts and deformation range of the vehicle. The overall deformation of the Audi and the Jetta are 34 mm and 136 mm respectively, with errors of less than 15% compared with the actual vehicle deformation. The LS-DYNA simulation results are compared with the actual vehicle deformation, as shown in Figure 7.

5. Conclusions

(1)
Based on the principles of classical mechanics and the finite element method, a method for solving the velocity of rear-end vehicle collisions is proposed. The case study shows that the results obtained using this method are in good agreement with those calculated with PC-Crash software, and the error is within 5%; reconstruction results of collision deformation are basically consistent with actual deformations, and the error is within 15%.
(2)
This method utilizes information from vehicle collision deformations and improves the reliability of analysis results of corner to corner rear-end collision of vehicles. A relationship model between collision velocity and deformation is established that overcomes the limitations of the traditional finite element method, such as low reconstruction efficiency and the model has strong pertinence.
(3)
By combining the finite element simulation with the dynamic model method, the vehicle velocity can be quickly calculated according to the vehicle deformation, which breaks through the traditional algorithm of calculating the vehicle velocity using tire traces and scattered objects, and improves the efficiency and accuracy of the calculation results.
The method proposed in this study is only applicable to the special accident form of corner rear-end collisions of vehicles. In the simulation experiments, the collision angle was 15°, which has some limitations. Therefore, follow-up research should expand the range of angles to explore the relationship between different velocities, different angles, and collision deformation. The basic principles and general rules of this study can still be used as reference for similar studies.

Author Contributions

Conceptualization, Y.C., X.Y. and G.H.; methodology, Y.C. and X.Y.; software, G.H.; validation, Y.C., X.Y. and G.H.; formal analysis, Y.C.; investigation, Y.C.; resources, Y.C.; data curation, Y.C.; writing—original draft preparation, G.H.; writing—review and editing, X.Y.; visualization, G.H.; supervision, Y.C.; project administration, Y.C.; funding acquisition, Y.C. All authors have read and agreed to the published version of the manuscript.

Funding

This research was supported by the National Natural Science Foundation of China (grant No. 11702049), the Scientific Research Funding Project of Liaoning Provincial Education Department in 2020 (grant No. JDL2020017), the Educational Science Planning Project of Liaoning Province (grant No. JG20DB69), the Research Project on Economic and Social Development of Liaoning Province in 2022 by the Liaoning Provincial Federation Social Science Circles (grant No. 2022lslybkt-022) and the 2021 Project of Dalian Academy of Social Sciences (grant No. 2021dlsky050).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Simulation experiment construction process.
Figure 1. Simulation experiment construction process.
Applsci 11 10964 g001
Figure 2. Change curve of vehicle velocity.
Figure 2. Change curve of vehicle velocity.
Applsci 11 10964 g002aApplsci 11 10964 g002b
Figure 3. Diagram of selection of vehicle 1 deformation range and key points.
Figure 3. Diagram of selection of vehicle 1 deformation range and key points.
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Figure 4. A 3D curved surface diagram of the relationship between deformations X1 and X2 and the collision velocity (v1 and v2).
Figure 4. A 3D curved surface diagram of the relationship between deformations X1 and X2 and the collision velocity (v1 and v2).
Applsci 11 10964 g004
Figure 5. Energy variation curves.
Figure 5. Energy variation curves.
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Figure 6. Vehicle collision track.
Figure 6. Vehicle collision track.
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Figure 7. Deformation comparisons between the simulation model and the actual vehicles.
Figure 7. Deformation comparisons between the simulation model and the actual vehicles.
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Table 1. Materials and properties of major automotive components.
Table 1. Materials and properties of major automotive components.
NumberPartsMaterial
Number
Density
(t/mm³)
Young’s Modulus
(Mpa)
Poisson’s RatioYield Stress (Mpa)
1Front fender024 1.415 × 10−91.00 × 1030.320
2Bumper024 7.890 × 10−92.00 × 1050.3800
3Door and Hood024 7.890 × 10−92.00 × 1050.3271
4Engine001 1.582 × 10−92.00 × 1040.3\
5Engine Cover001 7.890 × 10−92.00 × 1050.3\
6Tailgate024 1.005 × 10−91.00 × 1030.320
7Roof024 7.890 × 10−92.00 × 1050.3220
8Window Glass123 2.500 × 10−97.00 × 1040.2230
9Tire001 1.750 × 10−93.00 × 1020.3\
Table 2. Deformation data of vehicle 1 (30 km/h).
Table 2. Deformation data of vehicle 1 (30 km/h).
Key PointDeformation (mm)Key PointDeformation (mm)
XYZX Y Z
A14−1849B361−3439
A215−2549B424−2443
A323−2754C119−1939
A411−2356C219−2041
B123−2141C315−1943
B271−3740C410−1850
According to Formula (1), Cx, Cy, and Cz are 25 mm, −24 mm, and 45 mm, respectively, and the overall deformation (C) of vehicle 1 is 57 mm.
Table 3. Deformation of vehicle 1 under collision at different velocities (mm).
Table 3. Deformation of vehicle 1 under collision at different velocities (mm).
Overall Deformation of the Vehicle 1: C1
V20 km/h25 km/h30 km/h35 km/h40 km/h45 km/h50 km/h55 km/h60 km/h65 km/h
Overall deformation of the vehicle 2: C220 km/h-295770119132155178277354
25 km/h108-36588898101123229276
30 km/h156134-436996110116143189
35 km/h174196150-5367102103114139
40 km/h179275217164-6385108120148
45 km/h191278255273186-50101111135
50 km/h221311294292257182-7196119
55 km/h222317320325362285224-126125
60 km/h228324346379387388342343-92
65 km/h286305365403410452415354306-
Table 4. Values of coefficients A 1 i and A 2 i .
Table 4. Values of coefficients A 1 i and A 2 i .
i123456789
A1i0.00967−0.01029−0.6034−0.2137−0.025750.0261419.21−17.930.8444
A2i0.00585−0.00231−0.2844−1.818−0.027410.02769−5.81414.451.79
Table 5. Summary of results calculated by the two methods.
Table 5. Summary of results calculated by the two methods.
Calculation ResultsMethod of CalculationComparative
PC-Crash Mathematical Model CalculationRelative Error
Driving Velocity: v1 (km/h)33.9135.424.45%
Driving Velocity: v2 (km/h)33.5332.203.97%
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Cao, Y.; Ye, X.; Han, G. A Method for Calculating the Velocity of Corner-to-Corner Rear-End Collisions of Vehicles Based on Collision Deformation Analysis. Appl. Sci. 2021, 11, 10964. https://doi.org/10.3390/app112210964

AMA Style

Cao Y, Ye X, Han G. A Method for Calculating the Velocity of Corner-to-Corner Rear-End Collisions of Vehicles Based on Collision Deformation Analysis. Applied Sciences. 2021; 11(22):10964. https://doi.org/10.3390/app112210964

Chicago/Turabian Style

Cao, Yi, Xingwang Ye, and Geng Han. 2021. "A Method for Calculating the Velocity of Corner-to-Corner Rear-End Collisions of Vehicles Based on Collision Deformation Analysis" Applied Sciences 11, no. 22: 10964. https://doi.org/10.3390/app112210964

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