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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 592
NONLINEAR STATIC SIMULATION OF AUTOMOTIVE BUMPER OF
A PASSENGER CAR IN LOW SPEED IMPACT CRASH SIMULATION
Rajshekhar A Kharde1
, S. F. Patil2
1
M.Tech Student, KLE Dr. M.S Sheshgiri College of Engg & Tech, Belgaum, Karnataka, India
2
Mechanical Engineering, KLE. Dr. M.S Sheshgiri College of Engg & Tech, Belgaum, Karnataka, India
Abstract
Bumpers are important structural components of vehicles in terms of safety, static strength, and styling. This work describes
various aspects of the nonlinear static FEA of vehicle front bumpers using the commercial software Ls-Dyna, and the
correlation with physical tests. The basic concepts, procedures and techniques of nonlinear FEA are presented. The effects of
various aspects of nonlinear simulations like numerical integration, contact parameters, non-conformance of the mesh and
material law are studied. A nodally integrated element formulation for plates is proposed for analysis, and the formulation is
implemented in Ls-Dyna using the UEL user subroutine. Numerical tests are carried out on the new element. Suggestions are
proposed in simulation to improve the correlation of CAE results with physical test.
Keywords: CATIA V5, HYPERMESH v11, EPS, Ls-Dyna, ASTM D880.
--------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
Bumpers are automotive parts situated at the front and rear
of vehicle to ensure the protection of a vehicle body in case
of a low speed crash. This is enabled via the formability of
bumpers and energy absorption during an impact. The crash
capability of the bumper should also meet worldwide
regulations regarding the safety of passenger this
dissertation describes the nonlinear static simulation of
stiffness performed on an automotive front bumper. A brief
introduction to automotive front bumpers, and to nonlinear
static simulation is presented [1].
1.1 Bumpers
Bumpers are fixed on the front and on the back side of a car
to provide protection. They reduce the effects of collision
with other cars and objects due to their large deformation
zones. The bumpers are designed and shaped in order to
deform itself and absorb the force (kinetic energy) during a
collision [2].
Various national regulations have been enacted with regard
to the performance of bumpers under low speed impact such
as 49 CFR (Code of Federal Regulations) Part 581 of the
National Highway Traffic Safety Administration (NHTSA)
in the United States, the United Nations Economic
Commission for Europe (ECE) regulation No. 42, and the
CMVSS (Canada Motor Vehicle Safety Standard) 215.
There are no AIS (Automotive Industry Standards)
regulations for bumpers in India as of 2011.
With the increasing emphasis on energy efficiency in
automobiles due to the rising cost of fuel, there is a push
towards reducing the weight of all components, including
bumpers. Thus, the challenge in bumper design is to
maintain a delicate balance between vehicle weight
reduction, having sufficient stiffness, and meet safety
standards at the same time [1].
The whole frontal bumper system consists fascia, absorber
and grille.
Fig -1: Frontal bumper system components
In this work simulation results are validated by
experimental results and displacements at critical points
such as 5, 7, 8 and 9 are computed. In this paper, the focus is
on improving the accuracy of the nonlinear static
simulations performed on vehicle front bumpers to evaluate
their stiffness and strength.
2. TYPES OF NONLINEARITY
There are two common sources of nonlinearity: (1)
geometric and (2) material. The geometric nonlinearity
arises purely from geometric consideration (e.g. nonlinear
strain-displacement relations), and the material nonlinearity
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 593
is due to nonlinear constitutive behavior of the material of
the system. A third type of nonlinearity may arise due to
changing initial or boundary conditions [3].
3. EXPERIMENTAL TESTING OF BUMPER
The physical tests on the bumper were carried out at the
laboratory of Faurecia Automotive Exteriors. The test
conditions for subjective stiffness are known. They define
the acceptable maximum displacement under a defined
effort, the type of impactor and the test locations on the
bumper fascia. This data will also vary as per the bumper
model for the same client (sedan, utility, etc.).
Fig -2: Test setup for full bumper system
The front or rear of a vehicle is cut and mounted on a plaque
that can adapt to the arrangement of the Faurecia laboratory.
It is also supported by two jacks on the bottom to avoid
excessive vertical movement during the performance of
stiffness tests. This setup is provided by the manufacturer.
The bumper is attached to this unit via the standard
attachment points defined for this purpose.
Fig -3: Test positions
4. MODEL PREPARATION
The first step in the model preparation is to mesh all the
individual parts based on the CAD file which is created in
Catia V5. The CAD file is meshed using a pre-processing
software like ANSA and Hyper mesh. While meshing, it is
necessary to maintain minimum quality criteria for every
element. A complete meshed model is shown in Fig. 4
Fig -4: Complete meshed model of bumper
5. SIMULATION OF BUMPER
The vehicle manufacturer’s specification gives the
maximum displacement of the areas to be tested under a
given static load. The compression force is applied normal
to the skin (fascia). A mark is applied to the fascia to
indicate the position to be tested.
5.1 Simulation Results
5.1.1 Point 5
Fig.5 shows the displacement contour for subjective rigidity
test on test position 5.Where the maximum displacement is
about 14.41mm for applied load of 250N.
Fig -5: Displacement contour plots for various positions of
bumper
5.1.2 Point 7
Fig.6 shows the displacement contour for subjective rigidity
test on test position 7.Where the maximum displacement is
about 5.01mm for applied load of 250N.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 594
Fig -6: Displacement contour plots for various positions of
bumper
5.1.3 Point 8
Fig.7 shows the displacement contour for subjective rigidity
test on test position 8.Where the maximum displacement is
about 31.50mm for applied load of 250N.
Fig -7: Displacement contour plots for various positions of
bumper
5.1.4 Point 9
Fig.8 shows the displacement contour for subjective rigidity
test on test position 9.Where the maximum displacement is
about 10.10mm for applied load of 250N.
Fig -8: Displacement contour plots for various positions of
bumper
6. RESULTS AND DISCUSSION
6.1 Point 5
Fig. 9 shows correlation between physical test result and
CAE test result at Point 5. In physical test the displacement
is about 10.1mm for applied load of 250N and in CAE test
the displacement is 11.5mm for applied load of 250N. The
percentage of error based on test is 28.36%.
Fig -9: Correlation Load-Deflection curves at Point 5.
6.2 Point 7
Fig.10 shows Correlation between physical test result and
CAE test result at Point 7. In physical test the displacement
is about 5.86mm for applied load of 250N and in CAE test
the displacement is 5.1mm for applied load of 250N. The
percentage of error based on test is 3.4%.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 595
Fig -10: Correlation Load-Deflection curves at Point 7.
6.3 Point 8
Fig.11 shows Correlation between physical test result and
CAE test result at Point 8. In physical test the displacement
is about 30mm for applied load of 250N and in CAE test the
displacement is 31.50mm for applied load of 250N. The
percentage of error based on test is 12.02%.
Fig -11: Correlation Load-Deflection curves at Point 8.
6.4 Point 9
Fig.12 shows Correlation between physical test result and
CAE test result at Point 7. In physical test the displacement
is about 7.8mm for applied load of 250N and in CAE test
the displacement is 7.8mm for applied load of 250N. The
percentage of error based on test is 27.77%.
Fig -12: Correlation Load-Deflection curves at Point 9.
The improved percentage of error based on test is shown
below in table-1,
Table -1: Improved percentage of error based on test.
Poi
nts
Test Mesh
conform
ed
Mesh
conform
ed,
Contact
and
penetrat
ion
correcte
d
Mesh
conforme
d,
Contact
and
penetrati
on
corrected
,
Material
Law
modified
Error
%
5 10.1m
m
14.1mm 13.5mm 11.5mm 28.36
7 5.86m
m
5.6mm 5.3mm 5.2mm 3.4
8 30mm 34.1mm 34.0mm 31.50mm 12.02
9 7.8mm 10.8mm 10.5mm 7.8mm 27.77
7. CONCLUSION
The contact and penetration errors, mesh conformance and
material law do have important effects on the results. The
main causes for non-correlation were inaccuracy of contact
and penetration modeling, mesh and conformance errors,
and material law difference. However, the contribution of
each of these factors varies as per the load case. As can be
seen from Figs. 9, 10, 11 and 12, after these aspects are
taken care, the results are improved and there a good
correlation of 88% between the CAE and physical test
results.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 596
REFERENCES
[1]. Bhavesh A. Bohra,Pawar. D.B, Comparative analysis of
frontal car bumper during impact, ISSN 2319 – 4847, 2014.
[2]. Kee Joo Kim, Jun-Hyub Park, Crash simulation and
development of automotive bumper impact beam design for
weight reduction, Tongmyong University, 2012.
[3]. Reddy, J. N., An Introduction to Nonlinear Finite
Element Analysis, Oxford University Press, 2004.
[4]. Ls-Dyna Analysis User’s Manual, ver 6.10.
[5]. Radioss Theory Manual, ver 10.0, Part 2, Section 9.3,
Elasto-plasticity of isotropic materials, 2009.

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Nonlinear static simulation of automotive bumper of a passenger car in low speed impact crash simulation

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 592 NONLINEAR STATIC SIMULATION OF AUTOMOTIVE BUMPER OF A PASSENGER CAR IN LOW SPEED IMPACT CRASH SIMULATION Rajshekhar A Kharde1 , S. F. Patil2 1 M.Tech Student, KLE Dr. M.S Sheshgiri College of Engg & Tech, Belgaum, Karnataka, India 2 Mechanical Engineering, KLE. Dr. M.S Sheshgiri College of Engg & Tech, Belgaum, Karnataka, India Abstract Bumpers are important structural components of vehicles in terms of safety, static strength, and styling. This work describes various aspects of the nonlinear static FEA of vehicle front bumpers using the commercial software Ls-Dyna, and the correlation with physical tests. The basic concepts, procedures and techniques of nonlinear FEA are presented. The effects of various aspects of nonlinear simulations like numerical integration, contact parameters, non-conformance of the mesh and material law are studied. A nodally integrated element formulation for plates is proposed for analysis, and the formulation is implemented in Ls-Dyna using the UEL user subroutine. Numerical tests are carried out on the new element. Suggestions are proposed in simulation to improve the correlation of CAE results with physical test. Keywords: CATIA V5, HYPERMESH v11, EPS, Ls-Dyna, ASTM D880. --------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION Bumpers are automotive parts situated at the front and rear of vehicle to ensure the protection of a vehicle body in case of a low speed crash. This is enabled via the formability of bumpers and energy absorption during an impact. The crash capability of the bumper should also meet worldwide regulations regarding the safety of passenger this dissertation describes the nonlinear static simulation of stiffness performed on an automotive front bumper. A brief introduction to automotive front bumpers, and to nonlinear static simulation is presented [1]. 1.1 Bumpers Bumpers are fixed on the front and on the back side of a car to provide protection. They reduce the effects of collision with other cars and objects due to their large deformation zones. The bumpers are designed and shaped in order to deform itself and absorb the force (kinetic energy) during a collision [2]. Various national regulations have been enacted with regard to the performance of bumpers under low speed impact such as 49 CFR (Code of Federal Regulations) Part 581 of the National Highway Traffic Safety Administration (NHTSA) in the United States, the United Nations Economic Commission for Europe (ECE) regulation No. 42, and the CMVSS (Canada Motor Vehicle Safety Standard) 215. There are no AIS (Automotive Industry Standards) regulations for bumpers in India as of 2011. With the increasing emphasis on energy efficiency in automobiles due to the rising cost of fuel, there is a push towards reducing the weight of all components, including bumpers. Thus, the challenge in bumper design is to maintain a delicate balance between vehicle weight reduction, having sufficient stiffness, and meet safety standards at the same time [1]. The whole frontal bumper system consists fascia, absorber and grille. Fig -1: Frontal bumper system components In this work simulation results are validated by experimental results and displacements at critical points such as 5, 7, 8 and 9 are computed. In this paper, the focus is on improving the accuracy of the nonlinear static simulations performed on vehicle front bumpers to evaluate their stiffness and strength. 2. TYPES OF NONLINEARITY There are two common sources of nonlinearity: (1) geometric and (2) material. The geometric nonlinearity arises purely from geometric consideration (e.g. nonlinear strain-displacement relations), and the material nonlinearity
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 593 is due to nonlinear constitutive behavior of the material of the system. A third type of nonlinearity may arise due to changing initial or boundary conditions [3]. 3. EXPERIMENTAL TESTING OF BUMPER The physical tests on the bumper were carried out at the laboratory of Faurecia Automotive Exteriors. The test conditions for subjective stiffness are known. They define the acceptable maximum displacement under a defined effort, the type of impactor and the test locations on the bumper fascia. This data will also vary as per the bumper model for the same client (sedan, utility, etc.). Fig -2: Test setup for full bumper system The front or rear of a vehicle is cut and mounted on a plaque that can adapt to the arrangement of the Faurecia laboratory. It is also supported by two jacks on the bottom to avoid excessive vertical movement during the performance of stiffness tests. This setup is provided by the manufacturer. The bumper is attached to this unit via the standard attachment points defined for this purpose. Fig -3: Test positions 4. MODEL PREPARATION The first step in the model preparation is to mesh all the individual parts based on the CAD file which is created in Catia V5. The CAD file is meshed using a pre-processing software like ANSA and Hyper mesh. While meshing, it is necessary to maintain minimum quality criteria for every element. A complete meshed model is shown in Fig. 4 Fig -4: Complete meshed model of bumper 5. SIMULATION OF BUMPER The vehicle manufacturer’s specification gives the maximum displacement of the areas to be tested under a given static load. The compression force is applied normal to the skin (fascia). A mark is applied to the fascia to indicate the position to be tested. 5.1 Simulation Results 5.1.1 Point 5 Fig.5 shows the displacement contour for subjective rigidity test on test position 5.Where the maximum displacement is about 14.41mm for applied load of 250N. Fig -5: Displacement contour plots for various positions of bumper 5.1.2 Point 7 Fig.6 shows the displacement contour for subjective rigidity test on test position 7.Where the maximum displacement is about 5.01mm for applied load of 250N.
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 594 Fig -6: Displacement contour plots for various positions of bumper 5.1.3 Point 8 Fig.7 shows the displacement contour for subjective rigidity test on test position 8.Where the maximum displacement is about 31.50mm for applied load of 250N. Fig -7: Displacement contour plots for various positions of bumper 5.1.4 Point 9 Fig.8 shows the displacement contour for subjective rigidity test on test position 9.Where the maximum displacement is about 10.10mm for applied load of 250N. Fig -8: Displacement contour plots for various positions of bumper 6. RESULTS AND DISCUSSION 6.1 Point 5 Fig. 9 shows correlation between physical test result and CAE test result at Point 5. In physical test the displacement is about 10.1mm for applied load of 250N and in CAE test the displacement is 11.5mm for applied load of 250N. The percentage of error based on test is 28.36%. Fig -9: Correlation Load-Deflection curves at Point 5. 6.2 Point 7 Fig.10 shows Correlation between physical test result and CAE test result at Point 7. In physical test the displacement is about 5.86mm for applied load of 250N and in CAE test the displacement is 5.1mm for applied load of 250N. The percentage of error based on test is 3.4%.
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 595 Fig -10: Correlation Load-Deflection curves at Point 7. 6.3 Point 8 Fig.11 shows Correlation between physical test result and CAE test result at Point 8. In physical test the displacement is about 30mm for applied load of 250N and in CAE test the displacement is 31.50mm for applied load of 250N. The percentage of error based on test is 12.02%. Fig -11: Correlation Load-Deflection curves at Point 8. 6.4 Point 9 Fig.12 shows Correlation between physical test result and CAE test result at Point 7. In physical test the displacement is about 7.8mm for applied load of 250N and in CAE test the displacement is 7.8mm for applied load of 250N. The percentage of error based on test is 27.77%. Fig -12: Correlation Load-Deflection curves at Point 9. The improved percentage of error based on test is shown below in table-1, Table -1: Improved percentage of error based on test. Poi nts Test Mesh conform ed Mesh conform ed, Contact and penetrat ion correcte d Mesh conforme d, Contact and penetrati on corrected , Material Law modified Error % 5 10.1m m 14.1mm 13.5mm 11.5mm 28.36 7 5.86m m 5.6mm 5.3mm 5.2mm 3.4 8 30mm 34.1mm 34.0mm 31.50mm 12.02 9 7.8mm 10.8mm 10.5mm 7.8mm 27.77 7. CONCLUSION The contact and penetration errors, mesh conformance and material law do have important effects on the results. The main causes for non-correlation were inaccuracy of contact and penetration modeling, mesh and conformance errors, and material law difference. However, the contribution of each of these factors varies as per the load case. As can be seen from Figs. 9, 10, 11 and 12, after these aspects are taken care, the results are improved and there a good correlation of 88% between the CAE and physical test results.
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 596 REFERENCES [1]. Bhavesh A. Bohra,Pawar. D.B, Comparative analysis of frontal car bumper during impact, ISSN 2319 – 4847, 2014. [2]. Kee Joo Kim, Jun-Hyub Park, Crash simulation and development of automotive bumper impact beam design for weight reduction, Tongmyong University, 2012. [3]. Reddy, J. N., An Introduction to Nonlinear Finite Element Analysis, Oxford University Press, 2004. [4]. Ls-Dyna Analysis User’s Manual, ver 6.10. [5]. Radioss Theory Manual, ver 10.0, Part 2, Section 9.3, Elasto-plasticity of isotropic materials, 2009.