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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume: 3 | Issue: 4 | May-Jun 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470
@ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 627
Structural and Vibration Analysis of a
Machine Shaft using Finite Element Analysis
Syed Minal Hussian Jafri1, Prof Amit Kaimkuriya2
1Student, 2Assistant Professor
1,2Department of Mechanical Engineering, Millennium Institute of Technology, Bhopal, Madhya Pradesh, India
How to cite this paper: Syed Minal
Hussian Jafri | Prof Amit Kaimkuriya
"Structural and Vibration Analysis of a
Machine Shaft using Finite Element
Analysis" Published in International
Journal of Trend in Scientific Research
and Development
(ijtsrd), ISSN: 2456-
6470, Volume-3 |
Issue-4, June 2019,
pp.627-632, URL:
https://www.ijtsrd.c
om/papers/ijtsrd23
844.pdf
Copyright © 2019 by author(s) and
International Journal of Trend in
Scientific Research and Development
Journal. This is an Open Access article
distributed under
the terms of the
Creative Commons
Attribution License (CC BY 4.0)
(http://creativecommons.org/licenses/
by/4.0)
ABSTRACT
The present study is a simulation of a machine shaft. The study will be done on
FEM simulation software called Ansys 14.5, where a modal would be developed
which will undergo a process of meshing. Meshing will divide the modal in
extremely small units without changing the shape of actual geometry which will
help the software to study the change at every small unit of the model. Then the
of the modal would be defined in terms of inlet and outlet thereafter the
boundary condition and design equation would be applied to get the desired
result.
Keywords: Ansys 14.5, FEM simulation software, Stability, Stiffness, Strength,
design equation
INTRODUCTION
Human consumption of the Earth's resources increases theneedfor asustainable
development as an important ecological, social, and economic theme. Re-
engineering of machine tools, in terms of design and failure analysis, isdefined as
steps performed on an obsolete machine to return it to a new machine with the
warranty that matches the customer requirement. To understand the future
fatigue behaviour of the used machine components, it is important to investigate
the possible causes of machine parts failure through design,surface, and material
inspections. Failure analysis is an indispensable tool that is used widely by
industry sector to develop or improve the productdesign. Thefailuresof machine
elements are studied extensively by scientists to find methodsin ordertoidentify
their causes and to prevent them from reoccurring. To determine the failure
modes, analytical, experimental, and finite element analysismethodscanbeused.
A structure as a whole, and each individualmember,must be
designed with reference to the three 'Ss’: strength, stiffness
and stability: Strength is the ability to carry the applied
loads without yielding or breaking. Examples of strength
failures are a cable which snaps, a vehicle body which'
crumples, and a glass panel being smashed.
Stiffness is the ability to carry the applied loads without too
much distortion. A material can only sustain stress at the
expense of some strain ( ). Sometimesthestrain, even
though very small, may be the limiting factor. For example,a
machine tool must be stiff enough to produce the required
accuracy in machining, and a camera tripod must be stiff
enough to prevent camera shake.
Stability is the ability to carry compressive loads without
collapsing or buckling out of shape. For example, ametalrod
in compression longitudinally will suddenly bow out of
shape under a compressive stress which is well below the
compressive yield stress.
The importance of the different types of failure, in
considering any particular member, depends on how the
loads are applied to it.
Tie: A member in tension.
Strut: A member in compression.
Beam: A member with loads that causes bending.
Shaft: A member in torsion.
In fact the members are categorized according to the way in
which the forces are applied. These four type of loading
define the four structural components: ties, struts, beams
and shafts. Real members often carryacombinationofloads.
Shaft The term shaft refers to a rotating machine element,
circular in cross section which supports elements like
rollers, gears, pulleys & it transmits power. The shaft is
always stepped with maximum diameter in the middle and
minimum at the ends, where Bearings are mounted. The
steps provide shoulders for positioning of gears, pulleys &
bearings. The fillet radius is provided to prevent stress
concentration due to abrupt changes in the cross section.
Shafts have various names depending on the application
such as Axle, Spindle, Countershaft, Jackshaft, Line Shaft etc.
Ordinary transmission shafts are made of medium carbon
steels with a carbon content from 0.15- 0.40 percent such as
30C8 or 40C8, for greater strengths high carbon steels are
used such 45C8 or 50C8. For applications where corrosion
and high wear takes place, shaft material used is alloy steel.
Commongradesare16Mn5Cr4,40Cr4Mo6.Overloadfailures
are caused by forces that exceed the yield strength or the
tensile strength of a material. Shaft failures do not happen
IJTSRD23844
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 628
every day, but when they do, it can be a challenge to
determine the cause of failure.Here'satechnicalexplanation
of what happens when the shaft bends or breaks.
1. Transverse Vibrations.
2. Torsional Vibrations.
3. Critical Speed Vibrations.
4. Component Failure.
Transverse vibrations are typically the result of an
unbalanced drive shaft.A transverse vibration willoccur
once per every revolution of the drive shaft. This could
be because of damage to the shaft, missing balance
weights or foreign material stuck to the drive shaft.
Torsional vibrations occur twice per revolution of the
drive shaft. They could be duetoexcessiveu-joint angles
or a shaft not in phase with its design specifications. A
yoke outside of its design phasing by just one spline can
cause torsional vibration issues.
Critical speed vibrations occur when a drive shaft
operates at an RPM too high in relation to its length,
diameter and mass.
Component failure of the drive shaft or the motor and
transmission mounts can cause vibration. A failing u-
joint is a prime example.
Figure1. Failure of a shaft.
Fatigue Failure
Fatigue is caused by cyclical stresses, and the forces that
cause fatigue failures are substantially less than those that
would cause plastic deformation. Confusing the situation
even further is the fact that corrosion will reduce the fatigue
strength of a material. The amountof reductionisdependent
on both the severity of the corrosion and the number of
stress cycles.
Once they are visible to the naked eye, cracks always grow
perpendicular to the plane of maximum stress. Figure 1.2
shows the fracture planes caused by four common fatigue
forces. Because the section properties will change as the
crack grows, it’s crucial for the analyst to look carefully at
the point where the failure starts to determine the direction
of the forces. For example, while it is common for torsional
fatigue forces to initiate a failure, the majority of the crack
propagation could be in tension. That’s becausetheshafthas
been weakened and the torsional resonant frequency has
changed.
Figure2. shows the fracture planes caused by four
common fatigue force
Figure3. Fracture Surface of a shaft under fatigue loading.
One of the more common causes of shaft failure is due to
fatigue. Metal fatigue is caused by repeated cycling of the
load. It is a progressive localized damage due to fluctuating
stresses and strains on the material. Metal fatigues cracks
initiate and propagate in regions where the strain is most
sever. The concept of fatigue is very simple when a motion is
repeated the object that is doing thework becomes weak.
Fatigue occurs when a material is subject to alternating
stresses, over a long period of time. Examples of where
Fatigue may occur are: springs, turbine blades, airplane
wings, bridges and bones. There are 3 stepsthatmaybeview
a failure of a material due to fatigue on a microscopic level.
1. Crack Initiation: The initial crack occurs in this stage.
The crack may be caused by surface scratchescaused by
handling or toolingof the material, threads(asinascrew
or bolt), slipbands or dislocations intersecting the
surface as a result of previous cyclic loadingor work
hardening.
2. Crack Propagation: The crack continues to grow during
this stage as a result of continuously applied stresses.
3. Failure: Failure occurs when the material that has not
been affected by the crack cannot withstand the applied
stress. This stagehappens very quickly. Locationof the3
steps in a fatigue fracture under axial stress. One can
determine that a material failed by fatigue byexamining
the fracture sight. A fatigue fracture will have two
distinctregions; one being smooth or burnished as a
result of the rubbing of the bottom and top of the crack
(steps 1 & 2).The second is granular, due to the rapid
failure of the material.The most effective method of
improving fatigue performance is improvements in
design.
A. Eliminate or reduce stress raisers by stream lining the
part
B. Avoid sharp surface tears resulting from punching,
stamping, shearing or other processes
C. Prevent the development of surface discontinuities
during processing. Reduce or eliminate tensile residual
stresses caused by manufacturing.
D. Improve the details of fabrication and fastening
procedures. Metal fatigue is a significant problem
because it can occur due to repeated loads below the
static yield strength. This can resultin an unexpected
and catastrophic failure in use because most
engineering materials contain discontinuities. Most
metal fatigue cracks initiate from discontinuities in
highly stressed regions of the component. The failure
may be due the discontinuity, design, improper
maintenance or other causes. A failure analysis can
determine the cause of the failure. Understanding
fatigue strength and endurance limits is important
because most shaft failures are related to fatigue
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 629
associated with cyclic loading. These limits are
expressed by an S–N diagram, as shown in Fig. 1.4. For
steel, these plots become horizontal after a certain
number of cycles. In this case, a failure will not occur as
long as the stressis below 27 klbf/in. No matter how
many cycles are applied. However, at 10 cycles,theshaft
will fail if the load is increased to40bf/in.Thehorizontal
line is known as the fatigue or endurance limit. For the
types of steels commonly used for motors, good design
practice dictates staying well below the limit. Problems
arise when the applied load exceeds its limits or there is
damage to the shaft that causes a stress raiser.
Figure.4 S-N Curve
Modes of Fracture (Monotonic Overload)
1. Brittle: Brittle fracture may occur at stresses for below
the yield strength. In case of materials subjected to
impact and shock loads and usually occur without
warning. Brittle fractures are most likely to occur on
large-sized components or structures as a result of
shock loading.
2. Ductile: If a material is subjected to load abovethe yield
point and the process of deformationcontinues,fracture
eventually occur. Ductile fractures require a
considerable amount of energy to plasticallydeformthe
material in necking region. Ductile fractures are very
important in metal working operations, such as deep
drawing, forging etc.
Subcritical Crack Growth
A. Failure under static load Parts under static loading
may fail due to:
1. Ductile behaviour: Failure is due to bulk yielding
causing permanent deformationsthatareobjectionable.
These failures may cause noise, loss of accuracy,
excessive vibrationsandeventualfracture.In machinery
bulk yielding is the criteria for failure. Tiny areas of
yielding are in ductile behaviour in static loading.
2. Brittle behaviour: Failure is due to fracture. This
occurs when the materials (or conditions) do not allow
much yielding such as ceramics, grey cast iron, or
heavily cold-worked parts.
B. Dynamic loading:
Under dynamic loading, materials fail by fatigue. Fatigue
failure is a familiar phenomenon fatigue life is measured by
subjecting the material to cyclic loading. The loading is
usually uniaxial tension, but other cycles such as torsion or
bending can be used as well.
Fatigue failures are causedbyslowcrack growth through the
material. The failure process involves four stages
1. Crack initiation
2. Micro-crack growth (with crack length less than the
materials grain size) (Stage I)
3. Macro crack growth (crack length between 0.1mm and
10mm) (Stage II)
4. Failure by fast fracture.
Cracks initially propagate along the slip bands at around 45
degrees to the principal stress direction this is known as
Stage I fatigue crack growth. When the cracks reach a length
comparable to the materialsgrain size,theychangedirection
and propagate perpendicular to the principal stress. This is
known as Stage II fatigue crack growth.
Theories of Failure
Unfortunately, thereisnouniversaltheoryof failure.Instead,
over the years several hypotheseshavebeenformulatedand
tested, leading to today’s accepted practices.Beingaccepted,
we will characterize these “practices” as theories as most
designers do. Structural metal behaviour is typically
classified as being ductile or brittle.
Theories have been developed for the static failureofmetals
based upon the two classes of material failure:
Ductile metals yield
Brittle metals fracture
The various theories are as follows:
maximum principal stress theory also known as
rankine’s theory
maximum shear stress theory or guest and tresca’s
theory
maximum principal strain theory also known as st.
venant’s theory
total strain energy theory or haigh’s theory
maximum distortion energy theory or vonmises and
hencky’s theory
Literature Review
Silva (2003) has investigated the crack produced in the two
crankshafts of diesel van which wereused for30,000 kmand
then grinding is done. After machining both the crankshafts
lasted only for 1000 km and resulting into the Journal
damage. Due to wrong grinding process small fatigue crack
developed along the centre of journal causing journal
damage.Xu Xiaolei et. al. (2009), this paper is an analysis of
failure of main shaft of locomotive turbo charger. The
fracture position is located at a groove between journals
with different diameter. The rotating bending fatigue is the
dominant failure mechanism of the shafts. Detailed
metallurgical analysis indicates that fillet region of the
groove had subjected to high temperature. Katari et al.
(2011), has considered 3 different crankshafts made up of
same material, i.e., forged steel which is used in train. The
investigation shows that crankshaft failure is due to fatigue
which is supported through examination of mechanical
properties of crankshaft material. Gys Van Zyl et. al. (2013),
the case study is based on the analysis of FailureofConveyor
Drive Pulley Shafts. This paper investigates the failure root
cause by visual examination, optical and scanning electron
microscope analysis, chemical analysis of the material and
mechanical tests. Applications of FEA to the mechanical
engineering industry:
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 630
Figure.5. Flowchart of FEM analysis
Geometry Description
The Geometrical model has been generated on Ansys 14.5
The figure shows the geometrical model of machine shaft.
Figure.6. Geometry of shaft in 2D and 3D with dimension
in mm.
Meshing
Meshing is a critical operation in FEM in this process the
CAD geometry is divided into numbers of small pieces. The
small pieces are called mesh. The analysis accuracy and
calculation duration depends on the mesh size and
orientations. By, default, a coarse mesh is generated by
ANSYS software. Mesh contains mixed cells per unit area
(ICEM Tetrahedral cells) having triangular faces at the
boundaries. Number of nodes-15086 and Number of
elements- 8430, Curvature- On and Smooth – Fine meshing.
Figure7. Meshing of Machine shaft
Boundary Condition
Table.1 Physical and mechanical properties of shaft
Material Steel
Mass density 7.85 Kg/cm3
Mass 2.44247 Kg
Area 37,098.1 mm2
Volume 311,143 mm3
Yield Strength 207 MPa
Ultimate Tensile strength 345 MPa
Young’s Modulus 210GPa
Poisson’s Ratio 0.3
Shear Modulus 80.7692 GPa
Center of Gravity
x= 158.425mm y=-
0.0472625mm z= 0 mm
Table.2 Loads on the shaft
Quantities Unit Value
Mass Mass 2.45 Kg
Length L 300 mm
Maximum Bending Stress 153. 25 MPa
Maximum Shear Stress s 29.55 MPa
Maximum Tension stress 0.00 MPa
Maximum Torsional stress 2.70 MPa
Maximum Reduced stress 158.93 MPa
Maximum Deflection fmax 178.92 µm
Angle of Twist φ 0.01
Maximum Torque applied: 72.00 N-m
Phase angle: 0 degree and 1 degree
RESULTS AND DISCUSSIONS
After putting the boundary conditions, the solution is
initialized and then iteration is applied so that the values of
all parameters can be seen in a curve or line graph. After the
For 30mm diameter machine shaft at phase angle zero
degree
Object Name Static Structural (A5)
State Solved
Definition
Physics Type Structural
Analysis Type Static Structural
Solver Target Mechanical APDL
Options
Environment Temperature 22. °C
Generate Input Only No
Alternating Stress MPa Cycles Mean Stress Pa
3999 10 0
2827 20 0
1896 50 0
1413 100 0
1069 200 0
441 2000 0
262 10000 0
214 20000 0
138 1.e+005 0
114 2.e+005 0
86.2 1.e+006 0
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 631
Figure Equivalent Von-mises stress at 0 degree phase
angle
Figure .8. Maximum Principal elastic strain at 0 degree
phase angle
Figure.9.Maximum PrincipalStress at 0 degree phase angle
Figure.10 Equivalent elastic strain at 0 degree phase angle
Figure.11. Equivalent Von-mises stress at 1degree phase
angle
Figure.12. Maximum Principal Stress at 1 degree phase
angle
Figure.13. Total Deformation at 1 degree phase angle.
Table.3. Alternating stress & mean stress act on shaft
The following bar chart indicates the frequency at each
calculated mode.
Figure.14. Damped frequencies [in Hz] at every mode
Table4. Tabular form of damped frequency in Hz
Mode
Damped
Frequency [Hz]
Stability
[Hz]
Logarithmic
Decrement
1. 1325.2 0. 0.
2. 1325.3
3. 2910.7
4. 3729.3
5. 3729.9
6. 6503.5
7. 7417.4
8. 7418.4
9. 11546
10. 11547
11. 11600
12. 15089
13. 16219
14. 16221
15. 17606
16. 19703
17. 19706
18. 21475
19. 24674
20. 25180
Conclusions
From the above results it can be concluded that the FEM
analysis of shaft, vibration analysis and fatigue life analysis
have been done.This shows thebetter resultsascompared to
previous work. In this study the maximum principal stress,
deformation, maximum von misses stress, fatigue life and
corresponding to their stress act on the shaft and vibration
analysis have been done. All thesethingsaredescribed inthe
previous chapter. According to the result stabilityfrequency
of design shaft is 0 Hz up to the 25000 Hz Damped
frequency. The maximum alternative stress occurs on the
shat after applying 10 Lac cycles of shaft is approximate 86
Mpa.
Scope of future work
Different material can also be trying for better performance
and surface refinement can be done for better and accurate
results. The results provided in this work can be
experimentally verified.
International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 632
References
[1] Modal analysis of a distributed parameter rotating
shaft. Vol. 122, Issue 1, 8 April 1988, Pages 119-130.
[2] Hydrodynamic lubrication analysis of journal bearing
consideringmisalignmentcausedbyshaftdeformation.
Vol. 37, Issue 10, October 2004, pp. 841-848.
[3] Krishnaraj, C., Mohanasundram, K. M.2012.Designand
Implementation Study of Knowledge Based Foundry
Total Failure Mode Effects Analysis Technique,
European Journal of Scientific Research. 71(2): 298-
311.
[4] Modal analysis of drive shaft using FEA, International
Journal of Engineering and Management Research,
Vol.-3, Issue-1, February 2013.
[5] Design of machine Elements by R.S. Khurmi. Design of
machine Elements by Dr. Vijayaragavan, Dr.
Vishnupriyan lakshimi publication.
[6] "Modal Analysis Of Spur Gear To Determine The
Natural Frequencies And It's EffectOverTheGeometry
Of The Gear", , International Journal of Advanced
Engineering Research and Studies, E-ISSN2249–8974,
Int. J. Adv. Engg. Res. Studies/III/III/April-
June,2014/76-78, 2014.
[7] "Analysis of Carbon/Epoxy Composite Drive Shaft for
Automotive Application", International Journal of
Latest Trends in EngineeringandTechnology(IJLTET),
ISSN: 2278-621X, Vol. 5 Issue 1 January 2015.
[8] www.google.com.

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Structural and Vibration Analysis of a Machine Shaft using Finite Element Analysis

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume: 3 | Issue: 4 | May-Jun 2019 Available Online: www.ijtsrd.com e-ISSN: 2456 - 6470 @ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 627 Structural and Vibration Analysis of a Machine Shaft using Finite Element Analysis Syed Minal Hussian Jafri1, Prof Amit Kaimkuriya2 1Student, 2Assistant Professor 1,2Department of Mechanical Engineering, Millennium Institute of Technology, Bhopal, Madhya Pradesh, India How to cite this paper: Syed Minal Hussian Jafri | Prof Amit Kaimkuriya "Structural and Vibration Analysis of a Machine Shaft using Finite Element Analysis" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-3 | Issue-4, June 2019, pp.627-632, URL: https://www.ijtsrd.c om/papers/ijtsrd23 844.pdf Copyright © 2019 by author(s) and International Journal of Trend in Scientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (CC BY 4.0) (http://creativecommons.org/licenses/ by/4.0) ABSTRACT The present study is a simulation of a machine shaft. The study will be done on FEM simulation software called Ansys 14.5, where a modal would be developed which will undergo a process of meshing. Meshing will divide the modal in extremely small units without changing the shape of actual geometry which will help the software to study the change at every small unit of the model. Then the of the modal would be defined in terms of inlet and outlet thereafter the boundary condition and design equation would be applied to get the desired result. Keywords: Ansys 14.5, FEM simulation software, Stability, Stiffness, Strength, design equation INTRODUCTION Human consumption of the Earth's resources increases theneedfor asustainable development as an important ecological, social, and economic theme. Re- engineering of machine tools, in terms of design and failure analysis, isdefined as steps performed on an obsolete machine to return it to a new machine with the warranty that matches the customer requirement. To understand the future fatigue behaviour of the used machine components, it is important to investigate the possible causes of machine parts failure through design,surface, and material inspections. Failure analysis is an indispensable tool that is used widely by industry sector to develop or improve the productdesign. Thefailuresof machine elements are studied extensively by scientists to find methodsin ordertoidentify their causes and to prevent them from reoccurring. To determine the failure modes, analytical, experimental, and finite element analysismethodscanbeused. A structure as a whole, and each individualmember,must be designed with reference to the three 'Ss’: strength, stiffness and stability: Strength is the ability to carry the applied loads without yielding or breaking. Examples of strength failures are a cable which snaps, a vehicle body which' crumples, and a glass panel being smashed. Stiffness is the ability to carry the applied loads without too much distortion. A material can only sustain stress at the expense of some strain ( ). Sometimesthestrain, even though very small, may be the limiting factor. For example,a machine tool must be stiff enough to produce the required accuracy in machining, and a camera tripod must be stiff enough to prevent camera shake. Stability is the ability to carry compressive loads without collapsing or buckling out of shape. For example, ametalrod in compression longitudinally will suddenly bow out of shape under a compressive stress which is well below the compressive yield stress. The importance of the different types of failure, in considering any particular member, depends on how the loads are applied to it. Tie: A member in tension. Strut: A member in compression. Beam: A member with loads that causes bending. Shaft: A member in torsion. In fact the members are categorized according to the way in which the forces are applied. These four type of loading define the four structural components: ties, struts, beams and shafts. Real members often carryacombinationofloads. Shaft The term shaft refers to a rotating machine element, circular in cross section which supports elements like rollers, gears, pulleys & it transmits power. The shaft is always stepped with maximum diameter in the middle and minimum at the ends, where Bearings are mounted. The steps provide shoulders for positioning of gears, pulleys & bearings. The fillet radius is provided to prevent stress concentration due to abrupt changes in the cross section. Shafts have various names depending on the application such as Axle, Spindle, Countershaft, Jackshaft, Line Shaft etc. Ordinary transmission shafts are made of medium carbon steels with a carbon content from 0.15- 0.40 percent such as 30C8 or 40C8, for greater strengths high carbon steels are used such 45C8 or 50C8. For applications where corrosion and high wear takes place, shaft material used is alloy steel. Commongradesare16Mn5Cr4,40Cr4Mo6.Overloadfailures are caused by forces that exceed the yield strength or the tensile strength of a material. Shaft failures do not happen IJTSRD23844
  • 2. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 628 every day, but when they do, it can be a challenge to determine the cause of failure.Here'satechnicalexplanation of what happens when the shaft bends or breaks. 1. Transverse Vibrations. 2. Torsional Vibrations. 3. Critical Speed Vibrations. 4. Component Failure. Transverse vibrations are typically the result of an unbalanced drive shaft.A transverse vibration willoccur once per every revolution of the drive shaft. This could be because of damage to the shaft, missing balance weights or foreign material stuck to the drive shaft. Torsional vibrations occur twice per revolution of the drive shaft. They could be duetoexcessiveu-joint angles or a shaft not in phase with its design specifications. A yoke outside of its design phasing by just one spline can cause torsional vibration issues. Critical speed vibrations occur when a drive shaft operates at an RPM too high in relation to its length, diameter and mass. Component failure of the drive shaft or the motor and transmission mounts can cause vibration. A failing u- joint is a prime example. Figure1. Failure of a shaft. Fatigue Failure Fatigue is caused by cyclical stresses, and the forces that cause fatigue failures are substantially less than those that would cause plastic deformation. Confusing the situation even further is the fact that corrosion will reduce the fatigue strength of a material. The amountof reductionisdependent on both the severity of the corrosion and the number of stress cycles. Once they are visible to the naked eye, cracks always grow perpendicular to the plane of maximum stress. Figure 1.2 shows the fracture planes caused by four common fatigue forces. Because the section properties will change as the crack grows, it’s crucial for the analyst to look carefully at the point where the failure starts to determine the direction of the forces. For example, while it is common for torsional fatigue forces to initiate a failure, the majority of the crack propagation could be in tension. That’s becausetheshafthas been weakened and the torsional resonant frequency has changed. Figure2. shows the fracture planes caused by four common fatigue force Figure3. Fracture Surface of a shaft under fatigue loading. One of the more common causes of shaft failure is due to fatigue. Metal fatigue is caused by repeated cycling of the load. It is a progressive localized damage due to fluctuating stresses and strains on the material. Metal fatigues cracks initiate and propagate in regions where the strain is most sever. The concept of fatigue is very simple when a motion is repeated the object that is doing thework becomes weak. Fatigue occurs when a material is subject to alternating stresses, over a long period of time. Examples of where Fatigue may occur are: springs, turbine blades, airplane wings, bridges and bones. There are 3 stepsthatmaybeview a failure of a material due to fatigue on a microscopic level. 1. Crack Initiation: The initial crack occurs in this stage. The crack may be caused by surface scratchescaused by handling or toolingof the material, threads(asinascrew or bolt), slipbands or dislocations intersecting the surface as a result of previous cyclic loadingor work hardening. 2. Crack Propagation: The crack continues to grow during this stage as a result of continuously applied stresses. 3. Failure: Failure occurs when the material that has not been affected by the crack cannot withstand the applied stress. This stagehappens very quickly. Locationof the3 steps in a fatigue fracture under axial stress. One can determine that a material failed by fatigue byexamining the fracture sight. A fatigue fracture will have two distinctregions; one being smooth or burnished as a result of the rubbing of the bottom and top of the crack (steps 1 & 2).The second is granular, due to the rapid failure of the material.The most effective method of improving fatigue performance is improvements in design. A. Eliminate or reduce stress raisers by stream lining the part B. Avoid sharp surface tears resulting from punching, stamping, shearing or other processes C. Prevent the development of surface discontinuities during processing. Reduce or eliminate tensile residual stresses caused by manufacturing. D. Improve the details of fabrication and fastening procedures. Metal fatigue is a significant problem because it can occur due to repeated loads below the static yield strength. This can resultin an unexpected and catastrophic failure in use because most engineering materials contain discontinuities. Most metal fatigue cracks initiate from discontinuities in highly stressed regions of the component. The failure may be due the discontinuity, design, improper maintenance or other causes. A failure analysis can determine the cause of the failure. Understanding fatigue strength and endurance limits is important because most shaft failures are related to fatigue
  • 3. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 629 associated with cyclic loading. These limits are expressed by an S–N diagram, as shown in Fig. 1.4. For steel, these plots become horizontal after a certain number of cycles. In this case, a failure will not occur as long as the stressis below 27 klbf/in. No matter how many cycles are applied. However, at 10 cycles,theshaft will fail if the load is increased to40bf/in.Thehorizontal line is known as the fatigue or endurance limit. For the types of steels commonly used for motors, good design practice dictates staying well below the limit. Problems arise when the applied load exceeds its limits or there is damage to the shaft that causes a stress raiser. Figure.4 S-N Curve Modes of Fracture (Monotonic Overload) 1. Brittle: Brittle fracture may occur at stresses for below the yield strength. In case of materials subjected to impact and shock loads and usually occur without warning. Brittle fractures are most likely to occur on large-sized components or structures as a result of shock loading. 2. Ductile: If a material is subjected to load abovethe yield point and the process of deformationcontinues,fracture eventually occur. Ductile fractures require a considerable amount of energy to plasticallydeformthe material in necking region. Ductile fractures are very important in metal working operations, such as deep drawing, forging etc. Subcritical Crack Growth A. Failure under static load Parts under static loading may fail due to: 1. Ductile behaviour: Failure is due to bulk yielding causing permanent deformationsthatareobjectionable. These failures may cause noise, loss of accuracy, excessive vibrationsandeventualfracture.In machinery bulk yielding is the criteria for failure. Tiny areas of yielding are in ductile behaviour in static loading. 2. Brittle behaviour: Failure is due to fracture. This occurs when the materials (or conditions) do not allow much yielding such as ceramics, grey cast iron, or heavily cold-worked parts. B. Dynamic loading: Under dynamic loading, materials fail by fatigue. Fatigue failure is a familiar phenomenon fatigue life is measured by subjecting the material to cyclic loading. The loading is usually uniaxial tension, but other cycles such as torsion or bending can be used as well. Fatigue failures are causedbyslowcrack growth through the material. The failure process involves four stages 1. Crack initiation 2. Micro-crack growth (with crack length less than the materials grain size) (Stage I) 3. Macro crack growth (crack length between 0.1mm and 10mm) (Stage II) 4. Failure by fast fracture. Cracks initially propagate along the slip bands at around 45 degrees to the principal stress direction this is known as Stage I fatigue crack growth. When the cracks reach a length comparable to the materialsgrain size,theychangedirection and propagate perpendicular to the principal stress. This is known as Stage II fatigue crack growth. Theories of Failure Unfortunately, thereisnouniversaltheoryof failure.Instead, over the years several hypotheseshavebeenformulatedand tested, leading to today’s accepted practices.Beingaccepted, we will characterize these “practices” as theories as most designers do. Structural metal behaviour is typically classified as being ductile or brittle. Theories have been developed for the static failureofmetals based upon the two classes of material failure: Ductile metals yield Brittle metals fracture The various theories are as follows: maximum principal stress theory also known as rankine’s theory maximum shear stress theory or guest and tresca’s theory maximum principal strain theory also known as st. venant’s theory total strain energy theory or haigh’s theory maximum distortion energy theory or vonmises and hencky’s theory Literature Review Silva (2003) has investigated the crack produced in the two crankshafts of diesel van which wereused for30,000 kmand then grinding is done. After machining both the crankshafts lasted only for 1000 km and resulting into the Journal damage. Due to wrong grinding process small fatigue crack developed along the centre of journal causing journal damage.Xu Xiaolei et. al. (2009), this paper is an analysis of failure of main shaft of locomotive turbo charger. The fracture position is located at a groove between journals with different diameter. The rotating bending fatigue is the dominant failure mechanism of the shafts. Detailed metallurgical analysis indicates that fillet region of the groove had subjected to high temperature. Katari et al. (2011), has considered 3 different crankshafts made up of same material, i.e., forged steel which is used in train. The investigation shows that crankshaft failure is due to fatigue which is supported through examination of mechanical properties of crankshaft material. Gys Van Zyl et. al. (2013), the case study is based on the analysis of FailureofConveyor Drive Pulley Shafts. This paper investigates the failure root cause by visual examination, optical and scanning electron microscope analysis, chemical analysis of the material and mechanical tests. Applications of FEA to the mechanical engineering industry:
  • 4. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 630 Figure.5. Flowchart of FEM analysis Geometry Description The Geometrical model has been generated on Ansys 14.5 The figure shows the geometrical model of machine shaft. Figure.6. Geometry of shaft in 2D and 3D with dimension in mm. Meshing Meshing is a critical operation in FEM in this process the CAD geometry is divided into numbers of small pieces. The small pieces are called mesh. The analysis accuracy and calculation duration depends on the mesh size and orientations. By, default, a coarse mesh is generated by ANSYS software. Mesh contains mixed cells per unit area (ICEM Tetrahedral cells) having triangular faces at the boundaries. Number of nodes-15086 and Number of elements- 8430, Curvature- On and Smooth – Fine meshing. Figure7. Meshing of Machine shaft Boundary Condition Table.1 Physical and mechanical properties of shaft Material Steel Mass density 7.85 Kg/cm3 Mass 2.44247 Kg Area 37,098.1 mm2 Volume 311,143 mm3 Yield Strength 207 MPa Ultimate Tensile strength 345 MPa Young’s Modulus 210GPa Poisson’s Ratio 0.3 Shear Modulus 80.7692 GPa Center of Gravity x= 158.425mm y=- 0.0472625mm z= 0 mm Table.2 Loads on the shaft Quantities Unit Value Mass Mass 2.45 Kg Length L 300 mm Maximum Bending Stress 153. 25 MPa Maximum Shear Stress s 29.55 MPa Maximum Tension stress 0.00 MPa Maximum Torsional stress 2.70 MPa Maximum Reduced stress 158.93 MPa Maximum Deflection fmax 178.92 µm Angle of Twist φ 0.01 Maximum Torque applied: 72.00 N-m Phase angle: 0 degree and 1 degree RESULTS AND DISCUSSIONS After putting the boundary conditions, the solution is initialized and then iteration is applied so that the values of all parameters can be seen in a curve or line graph. After the For 30mm diameter machine shaft at phase angle zero degree Object Name Static Structural (A5) State Solved Definition Physics Type Structural Analysis Type Static Structural Solver Target Mechanical APDL Options Environment Temperature 22. °C Generate Input Only No Alternating Stress MPa Cycles Mean Stress Pa 3999 10 0 2827 20 0 1896 50 0 1413 100 0 1069 200 0 441 2000 0 262 10000 0 214 20000 0 138 1.e+005 0 114 2.e+005 0 86.2 1.e+006 0
  • 5. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 631 Figure Equivalent Von-mises stress at 0 degree phase angle Figure .8. Maximum Principal elastic strain at 0 degree phase angle Figure.9.Maximum PrincipalStress at 0 degree phase angle Figure.10 Equivalent elastic strain at 0 degree phase angle Figure.11. Equivalent Von-mises stress at 1degree phase angle Figure.12. Maximum Principal Stress at 1 degree phase angle Figure.13. Total Deformation at 1 degree phase angle. Table.3. Alternating stress & mean stress act on shaft The following bar chart indicates the frequency at each calculated mode. Figure.14. Damped frequencies [in Hz] at every mode Table4. Tabular form of damped frequency in Hz Mode Damped Frequency [Hz] Stability [Hz] Logarithmic Decrement 1. 1325.2 0. 0. 2. 1325.3 3. 2910.7 4. 3729.3 5. 3729.9 6. 6503.5 7. 7417.4 8. 7418.4 9. 11546 10. 11547 11. 11600 12. 15089 13. 16219 14. 16221 15. 17606 16. 19703 17. 19706 18. 21475 19. 24674 20. 25180 Conclusions From the above results it can be concluded that the FEM analysis of shaft, vibration analysis and fatigue life analysis have been done.This shows thebetter resultsascompared to previous work. In this study the maximum principal stress, deformation, maximum von misses stress, fatigue life and corresponding to their stress act on the shaft and vibration analysis have been done. All thesethingsaredescribed inthe previous chapter. According to the result stabilityfrequency of design shaft is 0 Hz up to the 25000 Hz Damped frequency. The maximum alternative stress occurs on the shat after applying 10 Lac cycles of shaft is approximate 86 Mpa. Scope of future work Different material can also be trying for better performance and surface refinement can be done for better and accurate results. The results provided in this work can be experimentally verified.
  • 6. International Journal of Trend in Scientific Research and Development (IJTSRD) @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID - IJTSRD23844 | Volume – 3 | Issue – 4 | May-Jun 2019 Page: 632 References [1] Modal analysis of a distributed parameter rotating shaft. Vol. 122, Issue 1, 8 April 1988, Pages 119-130. [2] Hydrodynamic lubrication analysis of journal bearing consideringmisalignmentcausedbyshaftdeformation. Vol. 37, Issue 10, October 2004, pp. 841-848. [3] Krishnaraj, C., Mohanasundram, K. M.2012.Designand Implementation Study of Knowledge Based Foundry Total Failure Mode Effects Analysis Technique, European Journal of Scientific Research. 71(2): 298- 311. [4] Modal analysis of drive shaft using FEA, International Journal of Engineering and Management Research, Vol.-3, Issue-1, February 2013. [5] Design of machine Elements by R.S. Khurmi. Design of machine Elements by Dr. Vijayaragavan, Dr. Vishnupriyan lakshimi publication. [6] "Modal Analysis Of Spur Gear To Determine The Natural Frequencies And It's EffectOverTheGeometry Of The Gear", , International Journal of Advanced Engineering Research and Studies, E-ISSN2249–8974, Int. J. Adv. Engg. Res. Studies/III/III/April- June,2014/76-78, 2014. [7] "Analysis of Carbon/Epoxy Composite Drive Shaft for Automotive Application", International Journal of Latest Trends in EngineeringandTechnology(IJLTET), ISSN: 2278-621X, Vol. 5 Issue 1 January 2015. [8] www.google.com.