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5/13/2018 Power Axle V6 - slidepdf.com
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A Presentation on
Design Validation of Power Axle of a Rail Car by Finite Element Analysis
Department of Mechanical Engineering
DAYANANDA SAGAR COLLEGE OF ENGINEERINGShavige Malleshwara Hills, Kumaraswamy Layout, Bangalore ² 560 078
2011
In partial fulfillment of the requirements for the award of Degree of
Master of Technology in Design EngineeringBy
Gangadhar
USN: 1DS07MDE05
Under the guidance of
Mr. Mahesh G. S. Mr. Kiran M.Assistant Professor Design Engineer
Department of Mechanical Engg., DSCE IMAC Designs Bangalore.
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Contents
Introduction
Literature Review
Methods and Methodology Problem Definition and Scope of the work
Results and Discussions
Conclusions and Future work References
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Introduction
Rail Vehicles
Types of Rail Vehicles ± Railways
± Subways
± Tramways
Train under test track
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Parts of Rail Coach
Standard names used in Rail Coach Bogie Parts
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Introduction to Axle
It connects two wheels and givessame rotational speed.
The axle has two bearings at the axle boxes
Wheel axle set is dynamically loadedduring run It is a rotating component of bogie
subjected to heavy loads and fatigueloads
Types of wheel and axle sets ± Power wheel set ± Trailer wheel set ± Trailer wheel with out side brake disc ± Wheel set with three discs mounted
axle
Trailer wheel set
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Introduction to Axle (contd.)
Axle Manufacturing ± Axles are manufactured by forging technique through hydraulically operated
arms
± Oxy-acetylene cutter is used to get the required length of rod
± Normalizing, Quenching, Tempering and Ultrasonic testing
Wheel Manufacturing ± Wheels are prepared by sophisticated casting process
± The scrap steel is melted in Ultra high frequency Electric Arc Furnace ± Pouring the molten metal through controlled air pressure system
± Normalizing, Quenching, Tempering and Ultrasonic testing
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Accident data base
Sweden maintained a data base of railwayaccidents i.e Derailment
It started from year 1980 to till April 2009 theyfound 35 cases.
Which have been grouped in five categoriesaccording to their primary cause:1. broken rails or other track defects - 16 events
2. axle failure on inside of the wheel - 5 events
3. axle failure on outside of the wheel - 4 events
4. wheel defects - 4 events
5. other causes (impact with objects on track,unidentified causes etc.) - 6 events
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Importance of Power Axle Study
Railway axles are subjected to variable amplitude loads
The weight of railway vehicle is introduced through the
bearings During service additional loads like track interaction,
curving, asymmetric loading of axle
Other parameters like torsional axle strains, wheel flats,wheel out of roundness, passenger load spectrum,whether and breaking conditions.
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Importance of Power Axle Study (Contd.)
Distribution of Fracture Places in theRailway Traction Shafts and Axles
Typical Fractures of Traction Shafts-Axles in (a) Section1 (b) Section 2 (c) Section 3 (d) Section 4 (e) Section 5
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Importance of Power Axle Study (Contd.)
a bc
Different Cracks on (a) Axle in UK (b) Under break seat (c) Close to wheel Seat
a b
Cracks in Axle Centre (a) Radial Cracks (b) Volume Defect
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Literature Review
Tests to detect cracks at carriage axles and to evaluate the quality of axles surfaced
The periodicity for testing using probabilistic fracture mechanics
Traction of shafts and axle of railway vehicles under accidental andunpredictable conditions
Fatigue study of railway axles
The effects of corrosion on fatigue properties
Rotary bending and press fitting on stress intensity factor and crack
growth Crack propagation under rolling contact between wheel and track
Thermal and stress analysis of brake discs in railway vehicles
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Methods and Methodology
Introduction to FEM
Features of FEM
Basic steps involved in FEM
± Geometrical modeling ± Discretization
± Formulation of elemental equations
± Derivation of elemental properties
± Assembly of equations
± Boundary conditions
± Computation of strain
± Computation of stress
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Introduction to ANSYS
Evolution of ANSYS
Features of ANSYS
ANSYS modeling
Importing solid models from CAD systems
Mesh generation
Solving the problem
Reviewing the Results
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Problem Definition
Introduction
The objective of the problem
Methodology
Power axle CAD model Power axle with mounted members
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Material Properties
Property For Axle structure For Wheel structure
Material A4T Cast Steel
Young's modulus 200 GPa 200 GPa
Poisson's ratio 0.3 0.3
Density 7850 kg/m3 7833 kg/m3
Specific Heat 427 J/kg 0 C 465 J/kg 0 C
Thermal Conductivity 42W/m 0 C 42W/m 0 C
Allowable Stress 145 MPa --Thermal expansion coefficient -- 10.5e-6/ 0 C
Convection film coefficient -- 22.7 W/m2 0 C
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Stress and Moment Calculations
Section of axle considered for calculations
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Representation of Forces and Formulae's
For all axles defined in thescope of this standard
P1 = (0.625 + 0.0875 h1 / b) m1 g
P2 = (0.625 - 0.0875 h1 / b) m1 g
Y1 = 0.35 m1 g
Y2 = 0.175 m1 g
H = Y1 ± Y2 = 0.175 m1 g
Q1 = [ P1 (b + s) ± P2 (b ±s) + (Y1 ±Y2) R ± Fi (2s ± yi )]
Q2 = [ P2 (b + s) ± P1 (b ±s) - (Y1 ±Y2) R ± Fi yi ]
Formulae¶s Used for Theoretical Calculations as Per EN 13104
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Moment Calculations and Design inputs
Sl No Symbol Quantity Sl No Symbol Quantity
1 M1 7500 kg 9 Y0 250 mm
2 M1+M2 8500 kg 10 rb 210 mm
3 F1 4.41 kN 11 s 750 mm
4 H1 1040 mm 12 P=P¶ 41.69 kN
5 B 1000 mm 13 Brake Disc mass 200 Kg
6 g 9.81m/sec2 14 F1 4410 N
7 R 410 mm 15 Y1 1295 mm
8 R b 210 mm 16 Fi 55000 N
Design Input Values
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Sectional Moment and Stress calculations
At section 1
± y=0
± Moment Mx = P1 y=52700*0=0
At Section 2
± y=250 mm ± Mx= 23.7 kN
± M¶x = 1.232 kN-m
± M¶y= 5.128 kN-m
± M¶z=1.232 kN-m
±
MR =sqrt ((23.7 + 3.609)2
+ 5.1282
+ 1.2322
) = 27.8 kN-m ± Stress =1*32*27800/ (*.1583) = 72 MPa
± =1*32*23700/ (*.1583) = 61.3 MPa (without braking)
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Sectional Moment and Stress calculations (contd.)
At Section 3
± y=615 mm
± d=130 mm
± D=210 mm
± r=75 mm ± K=1.02
± Mx= 21.8 kN
± M¶x = 6.7 kN-m
± M¶y= 5.128 kN-m
±
M¶z=1.232 kN-m ± MR = 29 kN-m
± Stress = 137 MPa
± =105 MPa (without braking)
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Sectional Moment and Stress calculations (contd.)
At Section 4
± y=1000 mm
± K = 1
± d = 130 mm (0.13 m)
± Mx= 19.87 kN ± M¶x = 4.81 kN-m
± M¶y= 5.128 kN-m
± M¶z=1.232 kN-m
± MR = 25.24 kN-m
±
Stress = 117.3 MPa ± =93.7 MPa (without braking)
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FEM Representation
Geometry Model with Built Up Geometry
Element Representation of the Shaft with Axle
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FEM Representation (Contd.)
Bending Moment Diagr am for the Given Loading
Figure shows bending moment for the given load of power axle. The maximum bendingmoment value is around 23.8 kN-m which is exactly matching with theoreticallycalculated value of 23.7 kN-m
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FEM Representation (Contd.)
Bending Stress Diagram for the Loads
The bending stress diagram represents only half of the axle. The bendingStress at section 1 is zero which is matching with the theoretical calculations
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FEM Representation (Contd.)
Bending Stress at Section 2
The stress value is around 61.523 MPa which is very near to theoretically calculatedvalue of 62.3 MPa
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FEM Representation (Contd.)
Bending Stress at Section 3
The value is around 103.622 MPa which is calculated without considering the stressconcentration factor. If stress concentration factor is used for calculation, the stress valueequal to 1.02*103.622=105.69 MPa which is very close to the theoretical value of 105 MPa.
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FEM Representation (Contd.)
Bending Stress at Section 4
The maximum stress value equals to 94.815 MPa which is near to the theoretical value of 93.7 Mpa
So FEM values are matching with theoretically obtained values.
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FEM Representation (Contd.)
Maximum Stress in the Structure
Stress developed is only 42.461 MPa which is less than the allowable value of 145MPa for the given material
Starting Conditions
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FEM Representation (Contd.)Braking Conditions
Stress with One Brake Disc
Figure shows failure of shaft as the stress 156.479 MPa exceeds the allowable stresslimit 145 MPa of the problem
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FEM Representation (Contd.)Braking Conditions
Stress on Axle with two break disc
Figure shows the safety of the axle with two symmetric brake discs as the stressdeveloped is within the allowable range of the material which is 126.71 MPa
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Results and Discussion
Initially the axle is checked for self weight condition
And next axisymmetry approach of problem is checked for rotation, interference and thermal conditions
3DMesh of the Solid Axle
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Results for self weight condition
Deflection Due to Self Weight
Maximum deflection due to self weight is around 0.00268mm taking place at thecenter
The three dimensional has built and simply supported condition is given at wheel position
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Results for self weight condition
von Mises Stress Plot
Maximum von Mises stress is around 0.659035 MPa due to self weight of the problem
Maximum stress are taking place in the middle wheel position and brake pad position
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Axisymmetric Analysis
Section Extracted from the Axle Model
(Half Model)
Axisymmetric Map Mesh of Axle
The problem is analysed for 600 rpm rotational load considering 100KMPH maximumspeed
Area is extracted along the axis and map meshed using 4 noded plane42 elements
The geometry is divided to ease the map mesh of the problem
More divisions are considered across sharp geometrical variation regions
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Rotational loads
Deformation Under Rotational Load Radial Stress Distribution Under Rotational Load
Almost negligible deformation of around 0.00571mm is taking place in thestructure
Maximum 7.68 MPa stress is taking place due to rotational load of 600 rpm of theaxle
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Rotational loads (Contd)
Hoop Stress Plot of Wheel von Mises Stress Plot of the Wheel
Maximum Hoop stress is around 4.62 MPa stress taking place in the structure
Maximum von Mises stress is around 5.72 MPa is taking place in the structure
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Rotational loads (Contd)
Radial, Hoop and von Mises Stress Variationvon Mises Stress in the Axle
Maximum von Mises stress is around 1.7MPa at the middle of the axle
Wheel mounting position the stress variation for radial, hoop and von Misesstresses are represented. Here stresses are observed maximum at the web
position and negligible at the axle position
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Interference Analysis
Radial Stress Distribution of Wheel Hoop Stress Distribution of Wheel
Maximum compressive stress is around 34.227 MPa and maximum tensile stressof around 0.250181 MPa is taking place on the combined structure
Maximum hoop stress is around 53.185 MPa on the wheel structure and 35.255MPa of compressive stress on inner axle structure
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Interference Analysis (Contd.)
von Mises Stress Distribution in the Wheel von Mises Stress in the Shaft Due to
Contact Pressure
von Mises stress of around 67.689 MPa on the interface region of wheel and axle. Inthe problem an interference of 25microns is applied to increase load carrying capacity
Maximum von Mises stress is around 33.808 MPa taking place at the axis due tocontact pressure
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Thermal Analysis
Temperature Plot During Braking on the Wheel
Maximum temperature developed is around 174.8 0 C. This temperature is mainly onthe wheel face and almost room temperature can be observed across the wheel axle
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Thermal Analysis (Contd.)
von Mises Stress Due to the Thermal Loading von Mises Stress on the Axle Due to
Temperature Load
Maximum stress is around 47.4 MPa due to temperature load can be observed
von Mises stress in the structure. Maximum von Mises stress is around 27.5 MPaon the center of axle
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Modal Analysis
Set No Frequency(Hz)
1 487.56
2 487.72
3 1167.5
4 1168.1
5 1365.9
Modal Frequencies
Mode Shape for the I st Modal Frequency
Modal nature of the shaft. Maximum displacement in the member is around0.14788m taking place at the centre showing lateral vibration
Since this frequency is higher than the operational frequency of 10Hzcorresponding to 600 rpm
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Summary of LoadsDescription von Mises Stress (MPa)
Maximum stress at the centre under normal
running conditions
103.622
Static Torque conditions 42.461
Braking condition with single brake disc 156.429Braking condition with two brake disc
arranged symmetrically
126.171
Self weight 0.659
Rotation 1.7
Interference 33.08
Thermal loads 27.5
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Conclusions
Initially a free body diagram is represented for the power axle based on loadscoming on the structure during operation
Theoretical calculations are calculated for the loads
Totally 4 sections are considered for theoretical moment and stress calculations
Further Finite Element verification is carried out to check the stress condition
The axial model is built using CATIA software for the specified dimensions
Further analyses carried out with rotational load corresponding to 100KMPh
Interference effect is studied on the problem. The interference load of 25 microns isapplied
Transient thermal analysis is carried out to check the thermal effects on the axle
during braking The modal analysis results for axle shows, first natural frequency of 486Hz which
is very high compared to the operational frequency of 10Hz
All the results shows, a combination of these loads are by law of superposition alsoare within the allowable working stress of the material
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Further Scope
The analysis can be extended for harmonic loads which will come across junction of rails.
The structure can be optimized with reference to weight and for stressconcentration at the flange region.
The shape of the wheel can be further optimized to reduce thermal effects The structure can be tested composites for better strength to weight ratio
and possible reduction of heat effects
Any possible residual stress effects can be explored.
Seismic effects on wheel and rail also can be explored.
Rail curvature effects can be considered. Rail surface irregularities effect also can be considered
Wear out wheel surface imperfections also can be studied for functionalsafety of the axle.
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References1. A.S. Watson, K. Timmis , ³A Method Of Estimating Railway Axle Stress Spectra´ Engineering Fracture Mechanics, 2010.
2. M. Ognjanovic, A. Simonovic, M. Ristivojevic, T. Lazovic, ³Research of Rail Traction Shafts and Axles Fractures TowardsImpact of Service Conditions and Fatigue Damage Accumulation´, Engineering Failure Analysis 17 (2010) 1560±1571
3. Viktor Jemec, Joe Jurman & Janez Grum, ³Evaluation of Defects and Cracks In Carriage Axles Using Non-DestructiveTesting´, Ndt For Safety November 07±09, 2007, Prague, Czech Republic
4. J Rudlin, A Muhammed and C Schneider, ³Inspection Reliability and Periodicity For Rail Axle Inspection , Rail AxleInspection
5. S. Beretta , A. Ghidini, F. Lombardo, ³Fracture Mechanics and Scale Effects In The Fatigue of Railway Axles´, EngineeringFracture Mechanics 72 (2005) 195±208
6. S. Beretta, M. Carboni, G. Fiore, A. Lo Conte, ³Corrosion±Fatigue of A1n Railway Axle Steel Exposed to Rainwater´,
International Journal of Fatigue 32 (2010) 952±961
7. M. Madia a, S. Beretta, U. Zerbst, ³An Investigation On The Influence of Rotary Bending and Press Fitting On StressIntensity Factors and Fatigue Crack Growth In Railway Axles´, Engineering Fracture Mechanics 75 (2008) 1906±1920
8. M. Luke, I. Varfolomeev a, K. Lütkepohl, A. Esderts, ³Fatigue Crack Growth In Railway Axles: Assessment Concept AndValidation Tests´, Engineering Fracture Mechanics (2010)
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References (Contd.)9. Yongming Liu, Liming Liu, Sankaran Mahadevan, ³Analysis Of Subsurface Crack Propagation Under Rolling Contact
Loading In Railroad Wheels Using FEM´, Engineering Fracture Mechanics 74 (2007) 2659±2674
10. Reibenschuh, M.; Lerher, T.; raml, M.; amec, B.; Potrè, I, ³Thermal and Stress Analysis of Brake Discs In RailwayVehicles´, Advanced Engineering 3(2009)1, Issn 1846-5900
11. Aar Manual Of Standards and Recommended Practices Wheels and Axles,S-600, 1981railway Applications ± Wheelsets And
Bogies, Powered Axles ± Design Method, English Version Of Din En 13104,Feb, 2002
12. University Of Cambridge, Department Of Engineering, ³Dynamics And Vibrations´, Annual Report-1996\1997.
13. Norton, Robert L., Machine Design ± An Integrated Approach, Prentice-Hall: New Jersey, 1998, 2 nd printing
14. Kelley,´ Fundamentals Of Mechanical Vibration´, Tata- McGraw Hill Publishing Company Limited, 2000.
15. Groover,´ Mechanical Vibration´, New Chand & Bros, 2000.
16. Klaus-Jurgen Bathe ³Finite Element Procedures , Prentice Hall of India Pvt. Ltd.- Sixth Edition 2002
17. Introuduction to the Finite Element Method, Desai/Abel ± CBS publishers 200218. Rober D. Cook, David S ³Concepts and Application of Finite Element Analysis´ Joh Wiely & Sons Pte. Ltd. Fourth
Edition 2003
19. Tirupathi R. Chandrupatla, Ashok D. Belegundu, ³Finite Elements in Engineering Prentice- Hall of India Pvt. Ltd, 2003
20. User Guide, ANSYS 10.0, Reference Mannual, 2010
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THANK YOU