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MADAN MOHAN MALAVIYA
UNIVERSITY OF TECHNOLOGY
GORAKHPUR
HYDRODYNAMIC JOURNAL BEARINGS
Presented By:-
Shiv Prasad 1204240048
Shubham Shukla 1204240050
Suraj Gupta 1204240054
Swapnil Jain 1204240055
Swati Srivastava 1204240056
Swati Singh 1204240057
Vareesh Pratap 1204240058
CONTENTS
 Introduction
 Terminology
 Causes of failure
 Assumptions
 Problem statement
 Design procedure and calculation
 Graphs
 Applications
 Conclusion
 References
INTRODUCTION
 Bearings are machine elements that constrain
relative motion and reduce friction between
moving parts to only the desired motion.
 In sliding contact bearing, surface of the shaft
slides over surface of the bush.
 In order to reduce frictional resistance, wear
and to carry away the heat generated, a layer
of fluid i.e. lubricant is provided.
TERMINOLOGY
 D= diameter of bearing
 d= diameter of journal
 l= length of bearing
 c= radial clearance
 e= eccentricity
 h0 = minimum oil film
thickness.
 ε= eccentricity ratio= e-
c
CAUSES OF FAILURE
 Lubricant failure due to high operating
temperature.
 Corrosion
 Excessive loading
 Misalignment
 Improper mounting
Fig1: Failure chances in percentage of
a hydrodynamic bearing [2]
ASSUMPTIONS
 The bearing is subjected to static loads
only.
 Bearing is assumed to be made of babbitt
material.
 Lubricant carried away all the heat
generated during the operation.
 The lubricant obeys Newton's law of
viscous flow.
 The pressure is constant throughout the
film thickness.
 The flow is one dimensional, i.e. the side
leakage is neglected.
 The lubricant is incompressible.
 The viscosity is constant throughout the
film.
 There is continuous supply of lubricant.
 No dynamic forces acting on both shaft
and bearing.
 l=d
 c=0.001r
 h0 /c=0.6
PROBLEM STATEMENT
To design a full hydrodynamic journal bearing
with the following specification for high speed
machine tool application:[1]
• Journal diameter= 75mm
• Radial load=10kN
• Journal speed = 1440rpm
• Minimum oil film thickness=22.5microns
• Inlet temperature=400C
• Bearing material= Babbitt
Determine the length of the bearing and select a
suitable oil for this application.
DESIGN PROCEDURE
AND CALCULATION
Given: W=10kN, N=1440rpm, d=75mm,
h0= 22.5 microns, T= 40˚C
STEP 1: Length of bearing
For machine tool application , the
permissible bearing pressure, p=2N/mm²
l=W/(p*d) = 10000/(2*75) = 66.67mm
l/d= 66.67/75 =0.89 ≈1(standard value)
l=d=75mm
 STEP 2: Selection of lubricant
p=W/(l*d)
=10000/(75*75)
= 1.78N/mm²
c=0.001r
=0.001*37.5
=0.0375mm
l/d=1 and h0/c = 0.0225/0.0375=0.6( high
speed application)
From table[1], for the above values,
S=0.264,
(r/c)f=5.79,
Q/(r*c*n*l)=3.99,
n=1440/60
=24rps
S=(r/c)²(µn/p)
0.264=(1000)²(µ*24/1.78)
µ=19.58cP
∆t={8.3p(CFV)}/(FV)
= (8.3*1.78*5.79)/3.99
= 21.44˚C
We know that,
Average temperature=Ti + (∆t/2)
= 40+(21.44/2)
=50.72˚C
RESULT :
1) Length of bearing= 75mm
2)The viscosity of SAE-10 oil is 22cP at 50˚C
.So we select SAE-10 oil for this application from
the graph.
Fig 2: Viscosity temperature
Fig 3: Variation between h0 and
frequency of rotation N [1],[6]
0
5
10
15
20
25
30
35
0 5 10 15 20 25 30 35 40 45 50
h0(micron)-->
Ns (Revolution per second) -->
µ= 12.9 cP µ = 18.9 cP µ = 27.52 cP
Fig 4: Variation between temperature
and frequency of rotation N[1]
0
20
40
60
80
100
120
0 10 20 30 40 50 60 70
Temperature(°C)-->
Ns (Revolution per second) -->
Ti Tmax Tavg
Fig 4:Variation between maximum load
with frequency of rotation[8]
APPLICATIONS
 Crankshaft bearings in petrol and diesel
engine
 Turbines
 Centrifugal pumps
 Rope conveyors
 Large electric motors
CONCLUSION
From the graph it can be concluded
that it is in agreement with a numerical
solution. Further it can be used to
select lubricating oil for a particular
speed and permissible limit of
temperature rise.
REFERENCES
1. Bhandari V B , “Design of machine element” McGraw-Hill
third edition 2014
2. Thakar Dutt “Bearing failure its causes and
countermeasures” 2014
3. Pickering Steve, “ Tribology of journal bearing subjected to
boundary and mixed lubrication” Department of mechanical
& industrial engineering Northeastern university 2011
4. “Bearing failure causes and curses” by Wilcoxon Research
5. Temiz Vedat “sliding contact bearing” 1995
6. http://www.viscopedia.com/viscosity-tables/substances/iso-
viscosity-classification/
7. http://www.engineeringtoolbox.com/iso-grade-oil-
d_1207.html
8. tribolab.mas.bg.ac.rs/radovi/2005_02.pdf
9. https://www.google.co.in/url?sa=t&rct=j&q=&esrc=s&sourc
e=web&cd=1&cad=rja&uact=8&ved=0CB4QFjAA&url=http
%3A%2F%2Ffaculty.ksu.edu.sa%2Fessam%2FDocuments
%2FME301chapter12.pdf&ei=G7IZVZeHDYKjuQTPyIDAD
g&usg=AFQjCNHG1H5YGbDUxgWliwf43TtosWRA1A
hydrodynamic journal bearing
hydrodynamic journal bearing

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hydrodynamic journal bearing

  • 1. MADAN MOHAN MALAVIYA UNIVERSITY OF TECHNOLOGY GORAKHPUR HYDRODYNAMIC JOURNAL BEARINGS Presented By:- Shiv Prasad 1204240048 Shubham Shukla 1204240050 Suraj Gupta 1204240054 Swapnil Jain 1204240055 Swati Srivastava 1204240056 Swati Singh 1204240057 Vareesh Pratap 1204240058
  • 2. CONTENTS  Introduction  Terminology  Causes of failure  Assumptions  Problem statement  Design procedure and calculation  Graphs  Applications  Conclusion  References
  • 3. INTRODUCTION  Bearings are machine elements that constrain relative motion and reduce friction between moving parts to only the desired motion.  In sliding contact bearing, surface of the shaft slides over surface of the bush.  In order to reduce frictional resistance, wear and to carry away the heat generated, a layer of fluid i.e. lubricant is provided.
  • 4. TERMINOLOGY  D= diameter of bearing  d= diameter of journal  l= length of bearing  c= radial clearance  e= eccentricity  h0 = minimum oil film thickness.  ε= eccentricity ratio= e- c
  • 5. CAUSES OF FAILURE  Lubricant failure due to high operating temperature.  Corrosion  Excessive loading  Misalignment  Improper mounting
  • 6. Fig1: Failure chances in percentage of a hydrodynamic bearing [2]
  • 7. ASSUMPTIONS  The bearing is subjected to static loads only.  Bearing is assumed to be made of babbitt material.  Lubricant carried away all the heat generated during the operation.  The lubricant obeys Newton's law of viscous flow.  The pressure is constant throughout the film thickness.
  • 8.  The flow is one dimensional, i.e. the side leakage is neglected.  The lubricant is incompressible.  The viscosity is constant throughout the film.  There is continuous supply of lubricant.  No dynamic forces acting on both shaft and bearing.  l=d  c=0.001r  h0 /c=0.6
  • 9. PROBLEM STATEMENT To design a full hydrodynamic journal bearing with the following specification for high speed machine tool application:[1] • Journal diameter= 75mm • Radial load=10kN • Journal speed = 1440rpm • Minimum oil film thickness=22.5microns • Inlet temperature=400C • Bearing material= Babbitt Determine the length of the bearing and select a suitable oil for this application.
  • 10. DESIGN PROCEDURE AND CALCULATION Given: W=10kN, N=1440rpm, d=75mm, h0= 22.5 microns, T= 40˚C STEP 1: Length of bearing For machine tool application , the permissible bearing pressure, p=2N/mm² l=W/(p*d) = 10000/(2*75) = 66.67mm l/d= 66.67/75 =0.89 ≈1(standard value) l=d=75mm
  • 11.  STEP 2: Selection of lubricant p=W/(l*d) =10000/(75*75) = 1.78N/mm² c=0.001r =0.001*37.5 =0.0375mm l/d=1 and h0/c = 0.0225/0.0375=0.6( high speed application)
  • 12. From table[1], for the above values, S=0.264, (r/c)f=5.79, Q/(r*c*n*l)=3.99, n=1440/60 =24rps S=(r/c)²(µn/p) 0.264=(1000)²(µ*24/1.78) µ=19.58cP
  • 13. ∆t={8.3p(CFV)}/(FV) = (8.3*1.78*5.79)/3.99 = 21.44˚C We know that, Average temperature=Ti + (∆t/2) = 40+(21.44/2) =50.72˚C RESULT : 1) Length of bearing= 75mm 2)The viscosity of SAE-10 oil is 22cP at 50˚C .So we select SAE-10 oil for this application from the graph.
  • 14. Fig 2: Viscosity temperature
  • 15. Fig 3: Variation between h0 and frequency of rotation N [1],[6] 0 5 10 15 20 25 30 35 0 5 10 15 20 25 30 35 40 45 50 h0(micron)--> Ns (Revolution per second) --> µ= 12.9 cP µ = 18.9 cP µ = 27.52 cP
  • 16. Fig 4: Variation between temperature and frequency of rotation N[1] 0 20 40 60 80 100 120 0 10 20 30 40 50 60 70 Temperature(°C)--> Ns (Revolution per second) --> Ti Tmax Tavg
  • 17. Fig 4:Variation between maximum load with frequency of rotation[8]
  • 18. APPLICATIONS  Crankshaft bearings in petrol and diesel engine  Turbines  Centrifugal pumps  Rope conveyors  Large electric motors
  • 19. CONCLUSION From the graph it can be concluded that it is in agreement with a numerical solution. Further it can be used to select lubricating oil for a particular speed and permissible limit of temperature rise.
  • 20. REFERENCES 1. Bhandari V B , “Design of machine element” McGraw-Hill third edition 2014 2. Thakar Dutt “Bearing failure its causes and countermeasures” 2014 3. Pickering Steve, “ Tribology of journal bearing subjected to boundary and mixed lubrication” Department of mechanical & industrial engineering Northeastern university 2011 4. “Bearing failure causes and curses” by Wilcoxon Research 5. Temiz Vedat “sliding contact bearing” 1995 6. http://www.viscopedia.com/viscosity-tables/substances/iso- viscosity-classification/ 7. http://www.engineeringtoolbox.com/iso-grade-oil- d_1207.html 8. tribolab.mas.bg.ac.rs/radovi/2005_02.pdf 9. https://www.google.co.in/url?sa=t&rct=j&q=&esrc=s&sourc e=web&cd=1&cad=rja&uact=8&ved=0CB4QFjAA&url=http %3A%2F%2Ffaculty.ksu.edu.sa%2Fessam%2FDocuments %2FME301chapter12.pdf&ei=G7IZVZeHDYKjuQTPyIDAD g&usg=AFQjCNHG1H5YGbDUxgWliwf43TtosWRA1A