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EXPERIMENTAL INVESTIGATION OF A INIMITABLE PLATFORM ON HEAVY
VEHICLE CHASSIS
DEULGAONKAR VIKAS RADHAKRISHNA & MATANI ASHOK GURMUKHDAS
Mechanical Engineering, Government College of Engineering, Sant Gadge Baba Amravati University, Amravati,
Maharashtra, India
ABSTRACT
This research paper deals with the experimental investigation of a unique platform structure by evaluation of
strain through experimental technique. Strain characteristics at critical locations on the structure are evaluated for dynamic
load. Strain gauge categorization for experimentation of the platform structure is described. Different nature of stresses at
significant locations is evaluated with the aid of linear and rosette gauges. Present-day data acquisition systems are utilized
for acquiring the strain values. Static and dynamic strain values are evaluated for constant speeds on cross-country track.
The experimentation reveals exact strain values, as there are no assumptions for measurement. Cross-country road
characteristics are exactly simulated for this measurement process. The optimum vehicle speed is maintained for the entire
measurement process. Tri-axial values of strains are calculated using rosette reduction technique. Linear strain values are
evaluated on longitudinal members of the platform structure. Values of strain acquired different locations reveal the critical
areas of the structure for possible design modifications
KEYWORDS: Platform Structure, Strain Signal, Data Acquisition Systems, Tri-Axial Stresses, Dynamic Strain
INTRODUCTION
Experimentation in present-days has acquired a vital significance as alomost all mechanical systems can be
computer simulated. Present vehemence on product accountability, new anticipated designs must be lighter and stronger,
and more conscientiously tested. This places pioneering importance on the experimental strain measurement techniques.
Mechanical strain is a term that relates to the dimensional transformation in component under contemplation.
Category of freight is the key factor, which decides the nature of strain induced in the structure on chassis. The
economic and industrial progress of a nation depends on transportation and unswerving use of a road vehicle. The
continual adjustment of vehicle speed and distance in response to change in traffic conditions generates various forces
which remain unbalanced, causing a great impact on transportation system.
A transportation vehicle is subjected to innumerable types of static and dynamic loads during its travel. The
structure under consideration is especially designed for intense load. The structure is made of structural steel. Light weight
channel sections are utilized for the manufacturing of this structure. These members are termed as longitudinal and cross
members of the platform.
All these structural steel members are welded to each other using oxy-acetylene welding process. A prototype of
the steel structure is shown in figure 1 below. The strain measurement locations on the structure are shown using white
chalk marks.
International Journal of Automobile Engineering
Research & Development (IJAuERD)
ISSN 2277-4785
Vol. 3, Issue 3, Aug 2013, 7-12
© TJPRC Pvt. Ltd.
8 Deulgaonkar Vikas Radhakrishna & Matani Ashok Gurmukhdas
Figure 1: The Steel Structure Physical Prototype
THE EXPERIMENTAL STRAIN COMPUTATION
The beginning step in for any strain gauge installation is the selection of pertinent gauge for the task. The gauge
selection process passes through various phases as assessment of exact strain sensing alloy, that determines the operating
characteristics for gauge, backing materials, gauge series, gauge length and gauge pattern. The most crucial parameter is
heat dissipation and this is accounted during gage length and gage pattern selection. In the present analysis locations have
been selected both at longitudinal and cross-members. The stresses at several locations on cross members are not
unidirectional hence rosettes have been used to acquire tri-axial strain values. Linear strain gauges are employed at
locations on longitudinal members to acquire strain values in linear direction. The loading pattern of actual loading
condition has been followed while placing the dummy load on the platform. Dynamic strain measurement has been carried
out while driving the vehicle on cross-country tracks at constant speed. The portions of tracks have been selected such that
they exhibit approximately uniform characteristics. Dynamic measurement has been made with zero stationary orientation.
The acquired signals have been investigated and the dynamic components have been obtained.
Strain Gauge Installation Process for Experimentation
Preceding to strain gauge installation, surface preparation is of immense significance. The phases of surface
preparation are solvent degreasing, surface abrading, gauge location layout lines and surface conditioning. Solvent
degreasing removes oil, grease, unrefined impurities and soluble compound sediments. For present experiment isopropyl
alcohol is employed as degreaser. Surface abrading seizes scale, tarnishes, paints and constructs a surface for suitable
gauge bonding. For surface grazing, a silicon carbide paper of fine girt is utilized. Further gauge location layout lines are
constructed at right angles to each other with one line leaning in the direction of strain measurement. To remove remains
from burnishing operation, surface conditioning is employed. The final step is neutralizing which brings the surface to an
alkalinity of 7 to 7.5 pH, appropriate for micro-measurements. M-Prep 5A is neutralizer in this investigation. Further in
this research strain gauges are bonded to the structure using M-bond 200 catalyst and further soldered. Extreme care is
taken during soldering operation as this would disturb all the above mentioned operations. The gauges installed and the
data acquisition systems are shown in figure 2 below
Figure 2: Strain Rosettes and Data Acquisition System on the Structure
Experimental Investigation of a Inimitable Platform on Heavy Vehicle Chassis 9
Static strain measurement has been conceded out for various design load conditions. Dynamic strain measurement
has been carried out while driving the vehicle on cross-country track at a constant speed of 20km/hr. The track segments
demonstrating approximately regular characteristics are selected. Dynamic measurement has been made with zero static
reference. The acquired signals have been evaluated and the dynamic components of strain have been obtained. In present
strain measurement the strain gauge locations and positions are enlisted in table 1 below
Table 1: Locations of Strain Gauges on the Structure
Rosette Gauges Linear Gauges
Second cross-member: 2 (RCM-2) Front longitudinal member : (LLM-F)
Mid cross-member: 5 (RCM-5) Mid longitudinal member (LLM-M)
Rear cross-member: 6 (RCM-6) Cross member: 5 (LCM-5)
Rear cross-member: 7 (RCM-7) Rear longitudinal member: (LLM-R)
DYNAMIC STRAIN MEASUREMENT AND STRAIN SIGNAL ANALYSIS
The intensity of load acting on the structure is of vital implication during the vehicle in motion especially when
the vehicle travels on a rough road territory. The prospect to damage the urbane cargo present in the shelter/container
mounted on the structure is significantly increased due to indiscriminate nature of load on cross-country tracks. Strain
signals on the novel structure for abovementioned dynamic load conditions are acquired for a truck travelling a speed of
20kmph.
The strain-acceleration signals are acquired in time domain. These strain-acceleration signals are further analyzed
using a DOS mode operating software. Root mean square (RMS) values of the signals are contrived in micro-strain (μe).
The rms values of signals measured at various locations on the structure are given in table 2 below
Table 2: Dynamic Strain RMS Values for Strain Signals on Paved Track at 20 km/hr
Gauge
Location
RMS (μe)
Strain Value
Gauge
Location
RMS (μe)
Strain Value
RCM2-A (+)38.05 RCM5-A (+)89.18
RCM2-B (+)86.60 RCM5-B (+)254.30
RCM2-C (+)37.74 RCM5-C (+)80.20
LLLF (-)64.13 LCM5 (-)24.81
RCM7-A (-)8.57 RCM6-A (+)153.42
RCM7-B (+)21.906 RCM6-B (+)131.07
RCM7-C (-)7.25 RCM6-C (-)65.62
LLLR (-)25.88 LLLM (+)77.25
Using the subsequent reduction technique for linear and rosette strain gauges, the dynamic values of strain are
computed. The stress values calculated based on Von-Mises criteria are tabulated below in table 3.
Table 3: Stress Values after Analysis of Experimental Strain Signals
Sr.
No
Gauge
Location
Stress Magnitude
(MPa)
01 RCM: 2 1.77
02 LLL:F -1.34
03 RCM: 7 0.867
04 LLL:R -0.543
05 RCM: 5 5.38
06 LCM: 5 -0.521
07 RCM: 6 4.13
08 LLL:M 1.62
10 Deulgaonkar Vikas Radhakrishna & Matani Ashok Gurmukhdas
CONCLUSIONS
The interior portion where a rectangular rosette is placed on second cross-member is subjected to a stress value of
0.92 MPa when the load applied is half the total load and is 1.7 MPa for full load. The maximum stress values occurred for
fifty and hundred percent loads on the exterior portion of the mid cross-member of the platform are 2.48 MPa and 5.38
MPa.The stress experienced on the rear of the platform on outer longitudinal member is 27% more than that of the stress
experienced on the mid portion on outer longitudinal member of the platform. The stress experienced on the rear of the
platform on outer longitudinal member is 23% more than that of the stress on the front of the platform on same longitudinal
member. The stress experienced on the mid cross-members of the platform varies from 2.5 to 3.6 MPa for 50% load case.
The strain measurement at critical locations is carried out for the evaluation of stress to which the individual
longitudinal and cross-members are subjected, to depict the behavior of the structure due to the load applied on platform
and for the design validation of the platform. The cross-members of the platform are subjected to bending stress due to
application of the load.
ACKNOWLEDGEMENTS
Authors are grateful to Prof. Dr.S.P Kallurkar for his continuous and untiring support for present research work.
REFERENCES
1. Bastawros A.F., Voloshin A.S., (2008). Thermal Strain Measurements in Electronic Packages through Fractional
Fringe Moiré Interferometry. ASME Journal of Electronic packaging, 112, 303-308.
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Engineering and Technology, 4, 115-122
3. Blum A.E., (1977) .The use and understanding of Photoelastic coatings, Strain, Journal of British Society for
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Experimental Investigation of a Inimitable Platform on Heavy Vehicle Chassis 11
11. Karl Hoffmann, Applying the Wheatstone Bridge Circuit, Hottinger Baldwin Messtechnik GmbH
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Microelectromechanical Systems, 6, 313-321
15. Prof.Deulgaonkar V.R, Prof.Dr. Kallurkar S.P, Prof.Dr.Matani A.G, (2013) An Investigation and Mathematical
Stress Analysis of Structural Integrity of Chassis Mounted Platform Subjected to Concentrated Load During
Gradient Travel, International Conference on Advances in Mechanical Engineering held at College of
Engineering, Pune,
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20. Yan.B, Waechter.D, Balcow.R & Prasad S.E, (2002). Measurement of Strain and polarization and electrostrictive
actuators Smart materials and structures Montreal, Quebec, Canada. 2nd Canada-US Can Smart Workshop
Experimental investigation of inmitiable platform on heavy vehicle chassis ij au erd 2013

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Experimental investigation of inmitiable platform on heavy vehicle chassis ij au erd 2013

  • 1. EXPERIMENTAL INVESTIGATION OF A INIMITABLE PLATFORM ON HEAVY VEHICLE CHASSIS DEULGAONKAR VIKAS RADHAKRISHNA & MATANI ASHOK GURMUKHDAS Mechanical Engineering, Government College of Engineering, Sant Gadge Baba Amravati University, Amravati, Maharashtra, India ABSTRACT This research paper deals with the experimental investigation of a unique platform structure by evaluation of strain through experimental technique. Strain characteristics at critical locations on the structure are evaluated for dynamic load. Strain gauge categorization for experimentation of the platform structure is described. Different nature of stresses at significant locations is evaluated with the aid of linear and rosette gauges. Present-day data acquisition systems are utilized for acquiring the strain values. Static and dynamic strain values are evaluated for constant speeds on cross-country track. The experimentation reveals exact strain values, as there are no assumptions for measurement. Cross-country road characteristics are exactly simulated for this measurement process. The optimum vehicle speed is maintained for the entire measurement process. Tri-axial values of strains are calculated using rosette reduction technique. Linear strain values are evaluated on longitudinal members of the platform structure. Values of strain acquired different locations reveal the critical areas of the structure for possible design modifications KEYWORDS: Platform Structure, Strain Signal, Data Acquisition Systems, Tri-Axial Stresses, Dynamic Strain INTRODUCTION Experimentation in present-days has acquired a vital significance as alomost all mechanical systems can be computer simulated. Present vehemence on product accountability, new anticipated designs must be lighter and stronger, and more conscientiously tested. This places pioneering importance on the experimental strain measurement techniques. Mechanical strain is a term that relates to the dimensional transformation in component under contemplation. Category of freight is the key factor, which decides the nature of strain induced in the structure on chassis. The economic and industrial progress of a nation depends on transportation and unswerving use of a road vehicle. The continual adjustment of vehicle speed and distance in response to change in traffic conditions generates various forces which remain unbalanced, causing a great impact on transportation system. A transportation vehicle is subjected to innumerable types of static and dynamic loads during its travel. The structure under consideration is especially designed for intense load. The structure is made of structural steel. Light weight channel sections are utilized for the manufacturing of this structure. These members are termed as longitudinal and cross members of the platform. All these structural steel members are welded to each other using oxy-acetylene welding process. A prototype of the steel structure is shown in figure 1 below. The strain measurement locations on the structure are shown using white chalk marks. International Journal of Automobile Engineering Research & Development (IJAuERD) ISSN 2277-4785 Vol. 3, Issue 3, Aug 2013, 7-12 © TJPRC Pvt. Ltd.
  • 2. 8 Deulgaonkar Vikas Radhakrishna & Matani Ashok Gurmukhdas Figure 1: The Steel Structure Physical Prototype THE EXPERIMENTAL STRAIN COMPUTATION The beginning step in for any strain gauge installation is the selection of pertinent gauge for the task. The gauge selection process passes through various phases as assessment of exact strain sensing alloy, that determines the operating characteristics for gauge, backing materials, gauge series, gauge length and gauge pattern. The most crucial parameter is heat dissipation and this is accounted during gage length and gage pattern selection. In the present analysis locations have been selected both at longitudinal and cross-members. The stresses at several locations on cross members are not unidirectional hence rosettes have been used to acquire tri-axial strain values. Linear strain gauges are employed at locations on longitudinal members to acquire strain values in linear direction. The loading pattern of actual loading condition has been followed while placing the dummy load on the platform. Dynamic strain measurement has been carried out while driving the vehicle on cross-country tracks at constant speed. The portions of tracks have been selected such that they exhibit approximately uniform characteristics. Dynamic measurement has been made with zero stationary orientation. The acquired signals have been investigated and the dynamic components have been obtained. Strain Gauge Installation Process for Experimentation Preceding to strain gauge installation, surface preparation is of immense significance. The phases of surface preparation are solvent degreasing, surface abrading, gauge location layout lines and surface conditioning. Solvent degreasing removes oil, grease, unrefined impurities and soluble compound sediments. For present experiment isopropyl alcohol is employed as degreaser. Surface abrading seizes scale, tarnishes, paints and constructs a surface for suitable gauge bonding. For surface grazing, a silicon carbide paper of fine girt is utilized. Further gauge location layout lines are constructed at right angles to each other with one line leaning in the direction of strain measurement. To remove remains from burnishing operation, surface conditioning is employed. The final step is neutralizing which brings the surface to an alkalinity of 7 to 7.5 pH, appropriate for micro-measurements. M-Prep 5A is neutralizer in this investigation. Further in this research strain gauges are bonded to the structure using M-bond 200 catalyst and further soldered. Extreme care is taken during soldering operation as this would disturb all the above mentioned operations. The gauges installed and the data acquisition systems are shown in figure 2 below Figure 2: Strain Rosettes and Data Acquisition System on the Structure
  • 3. Experimental Investigation of a Inimitable Platform on Heavy Vehicle Chassis 9 Static strain measurement has been conceded out for various design load conditions. Dynamic strain measurement has been carried out while driving the vehicle on cross-country track at a constant speed of 20km/hr. The track segments demonstrating approximately regular characteristics are selected. Dynamic measurement has been made with zero static reference. The acquired signals have been evaluated and the dynamic components of strain have been obtained. In present strain measurement the strain gauge locations and positions are enlisted in table 1 below Table 1: Locations of Strain Gauges on the Structure Rosette Gauges Linear Gauges Second cross-member: 2 (RCM-2) Front longitudinal member : (LLM-F) Mid cross-member: 5 (RCM-5) Mid longitudinal member (LLM-M) Rear cross-member: 6 (RCM-6) Cross member: 5 (LCM-5) Rear cross-member: 7 (RCM-7) Rear longitudinal member: (LLM-R) DYNAMIC STRAIN MEASUREMENT AND STRAIN SIGNAL ANALYSIS The intensity of load acting on the structure is of vital implication during the vehicle in motion especially when the vehicle travels on a rough road territory. The prospect to damage the urbane cargo present in the shelter/container mounted on the structure is significantly increased due to indiscriminate nature of load on cross-country tracks. Strain signals on the novel structure for abovementioned dynamic load conditions are acquired for a truck travelling a speed of 20kmph. The strain-acceleration signals are acquired in time domain. These strain-acceleration signals are further analyzed using a DOS mode operating software. Root mean square (RMS) values of the signals are contrived in micro-strain (μe). The rms values of signals measured at various locations on the structure are given in table 2 below Table 2: Dynamic Strain RMS Values for Strain Signals on Paved Track at 20 km/hr Gauge Location RMS (μe) Strain Value Gauge Location RMS (μe) Strain Value RCM2-A (+)38.05 RCM5-A (+)89.18 RCM2-B (+)86.60 RCM5-B (+)254.30 RCM2-C (+)37.74 RCM5-C (+)80.20 LLLF (-)64.13 LCM5 (-)24.81 RCM7-A (-)8.57 RCM6-A (+)153.42 RCM7-B (+)21.906 RCM6-B (+)131.07 RCM7-C (-)7.25 RCM6-C (-)65.62 LLLR (-)25.88 LLLM (+)77.25 Using the subsequent reduction technique for linear and rosette strain gauges, the dynamic values of strain are computed. The stress values calculated based on Von-Mises criteria are tabulated below in table 3. Table 3: Stress Values after Analysis of Experimental Strain Signals Sr. No Gauge Location Stress Magnitude (MPa) 01 RCM: 2 1.77 02 LLL:F -1.34 03 RCM: 7 0.867 04 LLL:R -0.543 05 RCM: 5 5.38 06 LCM: 5 -0.521 07 RCM: 6 4.13 08 LLL:M 1.62
  • 4. 10 Deulgaonkar Vikas Radhakrishna & Matani Ashok Gurmukhdas CONCLUSIONS The interior portion where a rectangular rosette is placed on second cross-member is subjected to a stress value of 0.92 MPa when the load applied is half the total load and is 1.7 MPa for full load. The maximum stress values occurred for fifty and hundred percent loads on the exterior portion of the mid cross-member of the platform are 2.48 MPa and 5.38 MPa.The stress experienced on the rear of the platform on outer longitudinal member is 27% more than that of the stress experienced on the mid portion on outer longitudinal member of the platform. The stress experienced on the rear of the platform on outer longitudinal member is 23% more than that of the stress on the front of the platform on same longitudinal member. The stress experienced on the mid cross-members of the platform varies from 2.5 to 3.6 MPa for 50% load case. The strain measurement at critical locations is carried out for the evaluation of stress to which the individual longitudinal and cross-members are subjected, to depict the behavior of the structure due to the load applied on platform and for the design validation of the platform. The cross-members of the platform are subjected to bending stress due to application of the load. ACKNOWLEDGEMENTS Authors are grateful to Prof. Dr.S.P Kallurkar for his continuous and untiring support for present research work. REFERENCES 1. Bastawros A.F., Voloshin A.S., (2008). Thermal Strain Measurements in Electronic Packages through Fractional Fringe Moiré Interferometry. ASME Journal of Electronic packaging, 112, 303-308. 2. Prof.Dr.Matani, Prof.Deulgaonkar V.R, Prof.Dr. Kallurkar S.P, (2013), An Investigation of Structural Integrity of Chassis Mounted Platform Subjected to Concentrated Load During Braking, International Journal of Mechanical Engineering and Technology, 4, 115-122 3. Blum A.E., (1977) .The use and understanding of Photoelastic coatings, Strain, Journal of British Society for Strain Measurement, 13,96-101 4. Bruins D.E, Garland C.W and Greytak T.K, Revised Science. Instrumentation, 46 ,1167-1170 5. Choi D., Thorpe J.L., Hanna R.B (1991). Image analysis to measure strain in wood and paper. Wood Science and Technology, 25, 251-262 6. Dally J.W and Rally W.F (1978). Experimental Stress Analysis, Mc-Graw Hill. 7. Hawley R.L, Waddington E.D, Gregg W.L, Kendrick Y, Taylor C (2004). Vertical-strain measurements in firn at Siple Dôme Antarctica. Journal of Glaciology, 50,447-452 8. Prof.Deulgaonkar V.R, Prof.Dr. Kallurkar S.P, Prof.Dr.Matani A.G,(2012), Advanced Mathematical Analysis of Chassis Integrated Platform Designed for Unconventional loading by using simple technique for static load, International Journal of Engineering and Innovative Technology ,1, 26-28 9. Karl Hoffmann (1996). Practical hints for the installation of strain gauges, Hottinger Baldwin Messtechnik GmbH. 10. Prof.Deulgaonkar V.R, Prof.Dr. Kallurkar S.P, Prof.Dr.Matani A.G, (2012), Mathematical Analysis of Section Properties Of A Platform Integrated With Vehicle Chassis, International Journal of Scientific and Research Publications, 2,87-90
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