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Yogendra S. Rajput, Vikas Sharma, Shivam Sharma, Gaurav Saxena / International Journal of
     Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                       Vol. 3, Issue 2, March -April 2013, pp.348-350
                       A Vibration Analysis Of Vehicle Frame
  Yogendra S. Rajput1; Vikas Sharma1; Shivam Sharma1; Gaurav Saxena2
                                       M. Tech. Scholar, RJIT, Tekanpur1
                         Asst. Prof., Dep’t of Automobile Engineering, RJIT, Tekanpur2


Abstract
        Importance in the development of off-
road racing vehicle for the SAEINDIA’s BAJA
competition has raised the value of dynamic
analysis under severe uneven loading. The
dynamic analysis is carried out by the finite
element method simulation thereby predicting
failure modes of the vehicle frame under
vibration analysis. This work investigates the
vibration characteristics of the frame including
the natural frequencies and mode shapes.

Keywords: Finite element method, dynamic
analysis, failure modes, mode shapes.

Introduction to SAE BAJA & Vehicle Frame                  Figure 1, Cross section of frame used
           Baja is a collegiate competition sponsored     Circular section is preferred comparatively for
by the Society of Automotive Engineers, India             torsional rigidity for its higher polar moment of
(SAEINDIA). The object for the team of students to        inertia compared than any other section as per the
develop a dynamically balanced vehicle to                 following formula
                                                                                     𝜋
withstand all kind of terrain during its mobility. The                           𝑇=     𝜏𝑑3
SAE BAJA vehicle development manual restricts us                                    16
about the vehicle weight, shape and size, and             where, T= twisting moment or torque applied;
dimensions. The objective of SAE BAJA                     τ = shear strength of the material;
competition is to simulate real world engineering         d = diameter of the pipe section;
design projects and their related challenges. The
objective is to develop not only the best performing      Material and Modelling of Vehicle Frame
vehicle but also the rugged and economical vehicle                  The weight of the material is also a limiting
frame that will comply all the SAE BAJA design            parameter for the SAE BAJA vehicle, because if a
requirements [1]. During actual road performance,         higher weight material is used, it could raise the
any vehicle is subjected to loads that cause stresses,    overall weight of the vehicle frame. The
vibrations and noise in the different components of       specifications of the material used for the vehicle
its structure. This requires appropriate strength,        frame development are tabled below in table 1, at
stiffness and fatigue properties of the components to     25°C reference temperature
be able to stand these loads. On top of that, quality     Properties                             Value
of a vehicle, as a system, which includes efficient       Density(x1000 kg/m3)                   7.7-8.3
energy consumption, safety, riding dampness and           Poisson’s Ratio                        0.27-0.30
provision of comfort to the driver is highly desired.     Elastic Modulus (GPa)                  190-210
           Frame forms the structural base of a racing    Tensile Strength (MPa)                 394.7
off road vehicle. The frame here developed for the        Yield Strength (MPa)                   294.8
event is of O section type. The strength and rigidity     Hardness (HB)                          111
of the O section is higher than any other form like I,    Impact Strength(J) (Izod)              123.4
T, C section. The theory of the bending and torsion       Table 1, Mechanical Properties of AISI 1020
explains that circular section is always a perfect one    Steel [2]
to resist the twisting and the rolling effects. Cross
section of the pipe element of the frame is shown in      The dimension of the pipe frame is given in table 2.
the fig 1.                                                Pipe diameter (mm)                25.4
                                                          Wall thickness (mm)               3.05
                                                          Table 2, Dimensions of pipe section
                                                          Vehicle Frame modelling for SAE BAJA is done in
                                                          ANSyS Mechanical, with structural discipline of
                                                          testing. The use of pipe-16 element which is a


                                                                                                 348 | P a g e
Yogendra S. Rajput, Vikas Sharma, Shivam Sharma, Gaurav Saxena / International Journal of
     Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                       Vol. 3, Issue 2, March -April 2013, pp.348-350
uniaxial element with tension-compression, torsion,     This model is then solved for the modal analysis to
and bending capabilities and has six degrees of         know the natural frequency of the model under its
freedom at two nodes: translations in the nodal x, y,   self weight. In general the natural frequency can be
and z directions and rotations about the nodal x, y,    calculated using the equation
and z axes [3] is used in the pre-processing steps of
the ANSyS. The other properties of the material and                          𝑘      𝑔
                                                                           𝑊𝑛 ==
the size of section frame are provided in the real                           𝑚      𝛿
constant and material menu of pre-processing steps.     where, k and m stand for stiffness and mass
Modelling is done via co-ordinates plotted, followed    respectively.
by the lines joining the points to develop the
geometric model of frame [4] shown below in fig 2.      Results
                                                                 Diesel engine provided for the SAE Baja
                                                        vehicle, is known to have the operating speed
                                                        varying from 10 to 330 revolutions per second (rps)
                                                        [6] for the different interval, as at idling it rolls at
                                                        10-20 rps where as at full throttle it runs at 250-300
                                                        rps.




                                                        Figure 4, List of frequencies w.r.t. mode shapes

                                                        The first mode shape explains the deformation
Figure 2, Geometric Model of vehicle rollcage           phenomenon on the upper part of the frame
                                                        acquiring the longitudinal vibrations of natural
Theory of boundary conditions applied to                frequency 26.155Hz, which is the lowest natural
Vehicle Frame                                           frequency where as the highest value is 55.264 Hz
         The natural frequency of vibration of a        under the effect of gravity and deformation under
machine or structure or frame, when coincides with      the self weight.
the excitation frequency of the forced vibration,
there occurs a phenomenon known as resonance,
which leads to excessive deflections and failure. A
lot of failures brought about by resonance and
excessive vibration of components and systems [5].
The frame is fixed at the lower base of the vehicle
frame to know the different mode shapes of the
upper substructure. As the wheels and suspension is
mounted at the axles, so it will have no motion and
hence the DOF of the lower base is restricted to
zero.




                                                        Figure 5, First mode shape of vibration




Figure 3,     Meshed     model    with    boundary
conditions


                                                                                                349 | P a g e
Yogendra S. Rajput, Vikas Sharma, Shivam Sharma, Gaurav Saxena / International Journal of
     Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com
                       Vol. 3, Issue 2, March -April 2013, pp.348-350




Figure 6, Second mode shape of vibration       Figure 9, Fifth mode shape of vibration
                                               Conclusion
                                                         The results developed states that the
                                               frame’s dynamic behaviour caused by change in
                                               usage with finite element method using ANSyS.
                                               Frequency modes of the frame that determine its
                                               dynamic behaviour are below100 Hz and vary from
                                               26.156 to 56.254 Hz. For the first two modes, the
                                               frame experienced longitudinal vibration on the roof
                                               pillars. The vibrations of the vehicle frame include
                                               longitudinal, transverse and torsion at different
                                               nodal points. The local bending vibration occurs at
                                               the top hat cross member where the engine is
                                               mounted on it. Since the installation of other
Figure 7, Third mode shape of vibration        components and accessories will be mounted, which
                                               will increase the total mass, therefore the natural
                                               frequencies will fall out of the natural range that can
                                               be compensated with increasing the chassis stiffness
                                               and will place the excited frequencies below natural
                                               range. This concept value implies the safe value of
                                               applied loads vibrations and deformations.

                                               References:
                                                 [1]    BAJA SAEINDIA rule book 2012.
                                                 [2]    http://www.efunda.com/materials/alloys/ca
                                                        rbon_steels/show_carbon.cfm?id=aisi_102
                                                        0&prop=all&page_title=aisi%201020
                                                 [3]    Ansys element reference library, Ansys12.1
                                                 [4]    Vikas Sharma, Divyanshu Purohit,
Figure 8, Fourth mode shape of vibration                “Simulation of an off-road vehicle roll cage
                                                        a static analysis”, International Journal of
                                                        Engineering Research and Applications
                                                        (IJERA) ISSN: 2248-9622, Vol. 2, Issue 4,
                                                        July-August 2012, pp.126-128
                                                 [5]    Rao, S. S., Mechanical Vibration, 4 th
                                                        Edition, pearson education press, 2004
                                                 [6]     Johansson, I., Edlund, S., Optimization of
                                                        Vehicle Dynamics in Cars by Use of Full
                                                        Vehicle FE- Models, Göteborg, Sweden,
                                                        Department of Vehicle Dynamics &
                                                        Chassis     Technology,       Volvo      Car
                                                        Corporation,                           1993.




                                                                                      350 | P a g e

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  • 1. Yogendra S. Rajput, Vikas Sharma, Shivam Sharma, Gaurav Saxena / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 2, March -April 2013, pp.348-350 A Vibration Analysis Of Vehicle Frame Yogendra S. Rajput1; Vikas Sharma1; Shivam Sharma1; Gaurav Saxena2 M. Tech. Scholar, RJIT, Tekanpur1 Asst. Prof., Dep’t of Automobile Engineering, RJIT, Tekanpur2 Abstract Importance in the development of off- road racing vehicle for the SAEINDIA’s BAJA competition has raised the value of dynamic analysis under severe uneven loading. The dynamic analysis is carried out by the finite element method simulation thereby predicting failure modes of the vehicle frame under vibration analysis. This work investigates the vibration characteristics of the frame including the natural frequencies and mode shapes. Keywords: Finite element method, dynamic analysis, failure modes, mode shapes. Introduction to SAE BAJA & Vehicle Frame Figure 1, Cross section of frame used Baja is a collegiate competition sponsored Circular section is preferred comparatively for by the Society of Automotive Engineers, India torsional rigidity for its higher polar moment of (SAEINDIA). The object for the team of students to inertia compared than any other section as per the develop a dynamically balanced vehicle to following formula 𝜋 withstand all kind of terrain during its mobility. The 𝑇= 𝜏𝑑3 SAE BAJA vehicle development manual restricts us 16 about the vehicle weight, shape and size, and where, T= twisting moment or torque applied; dimensions. The objective of SAE BAJA τ = shear strength of the material; competition is to simulate real world engineering d = diameter of the pipe section; design projects and their related challenges. The objective is to develop not only the best performing Material and Modelling of Vehicle Frame vehicle but also the rugged and economical vehicle The weight of the material is also a limiting frame that will comply all the SAE BAJA design parameter for the SAE BAJA vehicle, because if a requirements [1]. During actual road performance, higher weight material is used, it could raise the any vehicle is subjected to loads that cause stresses, overall weight of the vehicle frame. The vibrations and noise in the different components of specifications of the material used for the vehicle its structure. This requires appropriate strength, frame development are tabled below in table 1, at stiffness and fatigue properties of the components to 25°C reference temperature be able to stand these loads. On top of that, quality Properties Value of a vehicle, as a system, which includes efficient Density(x1000 kg/m3) 7.7-8.3 energy consumption, safety, riding dampness and Poisson’s Ratio 0.27-0.30 provision of comfort to the driver is highly desired. Elastic Modulus (GPa) 190-210 Frame forms the structural base of a racing Tensile Strength (MPa) 394.7 off road vehicle. The frame here developed for the Yield Strength (MPa) 294.8 event is of O section type. The strength and rigidity Hardness (HB) 111 of the O section is higher than any other form like I, Impact Strength(J) (Izod) 123.4 T, C section. The theory of the bending and torsion Table 1, Mechanical Properties of AISI 1020 explains that circular section is always a perfect one Steel [2] to resist the twisting and the rolling effects. Cross section of the pipe element of the frame is shown in The dimension of the pipe frame is given in table 2. the fig 1. Pipe diameter (mm) 25.4 Wall thickness (mm) 3.05 Table 2, Dimensions of pipe section Vehicle Frame modelling for SAE BAJA is done in ANSyS Mechanical, with structural discipline of testing. The use of pipe-16 element which is a 348 | P a g e
  • 2. Yogendra S. Rajput, Vikas Sharma, Shivam Sharma, Gaurav Saxena / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 2, March -April 2013, pp.348-350 uniaxial element with tension-compression, torsion, This model is then solved for the modal analysis to and bending capabilities and has six degrees of know the natural frequency of the model under its freedom at two nodes: translations in the nodal x, y, self weight. In general the natural frequency can be and z directions and rotations about the nodal x, y, calculated using the equation and z axes [3] is used in the pre-processing steps of the ANSyS. The other properties of the material and 𝑘 𝑔 𝑊𝑛 == the size of section frame are provided in the real 𝑚 𝛿 constant and material menu of pre-processing steps. where, k and m stand for stiffness and mass Modelling is done via co-ordinates plotted, followed respectively. by the lines joining the points to develop the geometric model of frame [4] shown below in fig 2. Results Diesel engine provided for the SAE Baja vehicle, is known to have the operating speed varying from 10 to 330 revolutions per second (rps) [6] for the different interval, as at idling it rolls at 10-20 rps where as at full throttle it runs at 250-300 rps. Figure 4, List of frequencies w.r.t. mode shapes The first mode shape explains the deformation Figure 2, Geometric Model of vehicle rollcage phenomenon on the upper part of the frame acquiring the longitudinal vibrations of natural Theory of boundary conditions applied to frequency 26.155Hz, which is the lowest natural Vehicle Frame frequency where as the highest value is 55.264 Hz The natural frequency of vibration of a under the effect of gravity and deformation under machine or structure or frame, when coincides with the self weight. the excitation frequency of the forced vibration, there occurs a phenomenon known as resonance, which leads to excessive deflections and failure. A lot of failures brought about by resonance and excessive vibration of components and systems [5]. The frame is fixed at the lower base of the vehicle frame to know the different mode shapes of the upper substructure. As the wheels and suspension is mounted at the axles, so it will have no motion and hence the DOF of the lower base is restricted to zero. Figure 5, First mode shape of vibration Figure 3, Meshed model with boundary conditions 349 | P a g e
  • 3. Yogendra S. Rajput, Vikas Sharma, Shivam Sharma, Gaurav Saxena / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 2, March -April 2013, pp.348-350 Figure 6, Second mode shape of vibration Figure 9, Fifth mode shape of vibration Conclusion The results developed states that the frame’s dynamic behaviour caused by change in usage with finite element method using ANSyS. Frequency modes of the frame that determine its dynamic behaviour are below100 Hz and vary from 26.156 to 56.254 Hz. For the first two modes, the frame experienced longitudinal vibration on the roof pillars. The vibrations of the vehicle frame include longitudinal, transverse and torsion at different nodal points. The local bending vibration occurs at the top hat cross member where the engine is mounted on it. Since the installation of other Figure 7, Third mode shape of vibration components and accessories will be mounted, which will increase the total mass, therefore the natural frequencies will fall out of the natural range that can be compensated with increasing the chassis stiffness and will place the excited frequencies below natural range. This concept value implies the safe value of applied loads vibrations and deformations. References: [1] BAJA SAEINDIA rule book 2012. [2] http://www.efunda.com/materials/alloys/ca rbon_steels/show_carbon.cfm?id=aisi_102 0&prop=all&page_title=aisi%201020 [3] Ansys element reference library, Ansys12.1 [4] Vikas Sharma, Divyanshu Purohit, Figure 8, Fourth mode shape of vibration “Simulation of an off-road vehicle roll cage a static analysis”, International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622, Vol. 2, Issue 4, July-August 2012, pp.126-128 [5] Rao, S. S., Mechanical Vibration, 4 th Edition, pearson education press, 2004 [6] Johansson, I., Edlund, S., Optimization of Vehicle Dynamics in Cars by Use of Full Vehicle FE- Models, Göteborg, Sweden, Department of Vehicle Dynamics & Chassis Technology, Volvo Car Corporation, 1993. 350 | P a g e