UNIT I
Journal and Roller Bearing 
Bearings: 
  The main function of bearing is to permit constrained relative motion of rigid parts. It 
is the machine part which supports the rotating shaft, axles etc. Shaft rotates smoothly in the 
bearing. Hence, loss of power due to friction is reduced. Bearing also confines the motion of 
shaft. 
Types of bearings  
Bearings are classified into two types. They are  
1.  Sliding contact bearings (plain bearings). 
2.  Rolling contact bearings (Anti-friction bearings). 
Sliding contact bearings 
  They are also called as plain bearings. Lubricant oil flim is kept between shaft and the 
bearing.  The  mating  surfaces  are  in  sliding  contact.  Hence,  it  is  known  as  sliding  contact 
bearing. 
  It is classified into two  
1.  Based on oil film thickness. 
2.  Based on direction of load. 
1. Based on thickness of lubricant oil film 
  It further classified into four types 
a)  Zero  film bearing 
b)  Thin  film bearing 
c)  Thick  film bearing (or) hydro dynamic bearing 
d)  Externally pressurised bearing (or) hydro static bearing. 
Zero  film bearing 
  It  does  not  use  lubricant  oil.  Metal  to  metal  contact  take  place.  So,  its  application  is 
limited. 
Thin  film bearing  
  It  is  also  named  as  boundary  lubricated  bearing.  Even  though  thin  oil  film  is  lying 
between mating surfaces, metal to metal contact take place. 
Thick  film bearing  
  It  is  also  named  as  hydrodynamic  bearing.  Thick  oil  film  is  lying  between  mating 
surfaces. During running position, metal to metal contact does not occur. The relative motion 
between  shaft  and  bearing  creates  positive  oil  pressure  which  supports  the  load.  Hence 
separate pump is not required. But at the starting position, metal to metal contacts take place.  
Externally pressurised bearing 
  It is also named as hydro static bearing. External pump supplies oil to the bearing at 
high  pressure.  This  high  pressure  oil  supports  the  load.  At  any  position,  metal  to  metal 
contact does not occur. 
2. Based on direction of load 
a.  Radial bearings (or) Journal bearing 
b.  Thrust bearings 
In  sliding  contact  bearing  if  load  acts  perpendicular  to  the  axis  of  shaft,  it  is  called  journal 
bearing.  
Shaft: Rotating part is called shaft. 
Bearing: Shaft supporting member is called bearing. 
Journal: The enclosed portion of shaft by the bearing is called journal. 
Journal bearings 
Hydrodynamic  journal  bearings  are  a  bearing  operating  with  hydrodynamic 
lubrication  in  which  the  bearing  surfaces  are  separated  from  the  journal  surface  by  the 
lubricant film.  
Hydrodynamic journal bearing and a journal rotating in a clockwise direction. Journal 
rotation  causes  pumping  of  the  lubricant  (oil)  flowing  around  the  bearing  in  the  rotation 
direction. If there is no force or load applied to the journal, its position will remain concentric 
to  the  bearing  position.  However,  a  loaded  journal  will  be  displaced  from  the  concentric 
position and forms a converging gap between the bearing and journal surfaces. The pumping 
action  of  the  journal  forces  the  oil  to  squeeze  through  the  wedge  shaped  gap  generating  a 
pressure. The pressure falls to the cavitations pressure (close to the atmospheric pressure) in 
the diverging gap zone where cavitations forms. 
The  displacement  of  the  shaft  centre  with  respect  to  the  bearing  centre  is  known  as 
eccentricity.  The  eccentric  position  of  the  shaft  is  governed  by  the  radial  load  carried  by  it 
and is adjusted by itself until the load is balanced by the pressure generated in the converging 
lubricant film between the bearing and the journal.  
The line joining the centre joining the shaft and the sleeve centre is known as the line 
of centre. The load carrying capacity depends on the amount of eccentricity (e), angular speed 
(), viscosity of lubricant (), bearing dimensions and the clearance. 
Types of Journal Bearings 
i.  Full Journal bearing 
ii.  Partial Journal bearing 
Full journal bearing 
  Journal  is  surrounded  by  bearing  fully.  Covered  angle  is  360
o
.  It  may  be 
represented  as  a  cylindrical  sleeve  (bearing)  wrapped  around  shaft.  If  the  wrapping  extends 
around the full 360
o
 of the journal, it is termed as full journal bearing.   
Partial journal bearing 
  Journal is surrounded by bearing partially. Covered angle is 120
o 
.  
Application of journal bearing 
      [Refer to PSGDB   P.NO: 7.30] 
  Conveyors 
  Cam shafts 
  Motor shafts 
  Turbine shaft  
Materials Used For Sliding Contact Bearings 
          [Refer to PSGDB   P.NO: 7.30] 
  All the desirable characteristics of bearing materials are not to be found to a high 
degree in any particular bearing material. Hence the choice of a material for any application 
must represent a compromise. 
1.  Tine base Babbit and lead- base babbit are in widespread use since they satisfy most 
requirements for general application. 
2.  Where loads are very high, bronze or brass bearings may be used. Bronze is an alloy 
of copper and tin. This bronze bearing is suitable for heavy loads at slow speeds. 
3.  Where high compressive and fatigue strength are required, copper, lead, and tin alloys 
may be used.  
4.  Gun metal is an alloy of copper, tin, and zinc. Gun metal bearing is suitable for high 
speeds. 
5.  Nylon and rubber are used as bearing materials. It is used in water turbine bearings 
and water pump bearings.   
Properties of good sliding contact bearing materials 
          [Refer to PSGDB   P.NO: 7.30] 
  Required properties of good bearing material are given below 
1.  To reduce wear, co-efficient of friction must be less. 
2.  To maintain the clearance between shaft and bearing, co-efficient of thermal 
expansion must be less. 
3.  Low cost 
4.  To adjust the alignment error, youngs modulus must be less. 
5.  To remove the heat generated due to friction, thermal conductivity must be more. 
6.  To prevent rusting, corrosion resistance must be high. 
7.  To withstand hydro-dynamic pressure, compression strength must be high. 
8.  To withstand varying load, fatigue strength must be high. 
Lubricant 
A  lubricant  (sometimes  referred  to  as  "lube")  is  a  substance  (often  a  liquid)  introduced 
between two moving surfaces to reduce the friction between them, improving efficiency and 
reducing  wear.  It  may  also  have  the  function  of  dissolving  or  transporting  foreign  particles 
and of distributing heat. 
Lubricants perform the following key functions. 
-  Keep moving parts apart 
-  Reduce friction 
-  Transfer heat 
-  Carry away contaminants & debris 
-  Transmit power 
-  Protect against wear 
-  Prevent corrosion 
-  Seal for gasses 
-  Stop the risk of smoke and fire of objects 
Types of lubricants 
-  Solid 
-  Semi-solid 
-  Liquid 
Lubrication 
Lubrication is the process, or technique employed to reduce wear of one or both surfaces 
in  close  proximity,  and  moving  relative  to  each  another,  by  interposing  a  substance  called 
lubricant  between  the  surfaces  to  carry  or  to  help  carry  the  load  between  the  opposing 
surfaces. The interposed lubricant film can be a solid, a liquid, and gas. 
Types of Lubrication  
o  Hydrodynamic Lubrication 
o  Hydrostatic Lubrication 
o  Elastro hydrodynamic Lubrication 
o  Boundary Lubrication  
The regimes of lubrication 
As the load increases on the contacting surfaces three distinct situations can be observed with 
respect to the mode of lubrication, which are called regimes of lubrication: 
-  Fluid film lubrication is the lubrication regime in which through viscous forces the 
load is fully supported by the lubricant within the space or gap between the parts in 
motion relative to one another (the lubricated conjunction) and solid-solid contact is 
avoided.
[2]  
o  Hydrostatic lubrication is when an external pressure is applied to the 
lubricant in the bearing, to maintain the fluid lubricant film where it would 
otherwise be squeezed out. 
o  Hydrodynamic lubrication is where the motion of the contacting surfaces 
and the exact design of the bearing is used to pump lubricant around the 
bearing to maintain the lubricating film. This design of bearing may wear 
when started or stopped, as the lubricant film breaks down. 
-  Elastohydrodynamic lubrication: The opposing surfaces are separated but there 
occurs some interaction between the raised solid features called asperities, and there 
is an elastic deformation on the contacting surface enlarging the load bearing area 
whereby the viscous resistance of the lubricant becomes capable of supporting the 
load. 
-  Boundary lubrication (also called boundary film lubrication): The bodies come into 
closer contact at their asperities; the heat developed by the local pressures causes a 
condition which is called stick-slip and some asperities break off. At the elevated 
temperature and pressure conditions chemically reactive constituents of the lubricant 
react with the contact surface forming a highly resistant tenacious layer, or film on the 
moving solid surfaces (boundary film) which is capable of supporting the load and 
major wear or breakdown is avoided. Boundary lubrication is also defined as that 
regime in which the load is carried by the surface asperities rather than by the 
lubricant.  
Besides supporting the load the lubricant may have to perform other functions as well, for 
instance it may cool the contact areas and remove wear products. While carrying out these 
functions the lubricant is constantly replaced from the contact areas either by the relative 
movement (hydrodynamics) or by externally induced forces. 
Lubrication is required for correct operation of mechanical systems pistons, pumps, cams, 
bearings, turbines, cutting tools etc where without lubrication the pressure between the 
surfaces in close proximity would generate enough heat for rapid surface damage which in a 
coarsened condition may literally weld the surfaces together, causing seizure. 
Lubrication of bearings 
  Journal bearing is lubricated for the following reasons. 
1.  To reduce friction 
2.  To reduce wear 
3.  To transfer the heat due to friction 
4.  To prevent the rusting of bearing surface. 
5.  To prevent the damage of bearing surface. 
Properties of good lubricant 
  The essential properties required for lubricant are 
1.  High viscosity index 
2.  High flash point 
3.  High fire point 
4.  High corrosion resistance 
5.  Low freezing point  
6.  Low cost. 
Factor to be considered for the selection of type of bearing 
  While selecting the type of bearing, the following factors are considered 
1.  Type of load 
2.  Speed of shaft 
3.  Space required 
4.  Vibrations 
5.  Temperature  
6.  Stating torque  
Advantages of sliding contact bearing 
  Low cost  
  Silent in operation 
  Long life 
  Withstands shocks 
  Not breaks easily 
  Not affected by fatigue load 
  Simple design 
  Less radial space is enough 
  Not damaged by impurities.  
Disadvantages of sliding contact bearing 
  More friction 
  More loss of power 
  High maintenance cost 
  Large amount of lubricant is required 
  Replacement is not easier 
  Not operate in inclined position 
  Less accuracy  
Application of sliding contact bearing 
  Diesel engine 
  Gas engines 
  Pumps 
  Compressors 
  Turbines  
  Aircraft engines 
  Conveyors 
  Typewriters  
Terminology of hydro-dynamic journal bearing  
When shaft is running at high speed, some terms are defined  
  Diameteral clearance (C) = bearing diameter  journal diameter 
Where  
  D= Diameter of journal in mm 
  C= Diameteral clearance in mm   
  D + C = Diameter of bearing in mm 
  L= length of bearing in mm 
  N= speed of journal in RPM 
  N= speed of journal in RPS 
  O= Centre of journal 
  O=Centre of bearing  
Diametral clearance (C) 
  It is the difference between bearing diameter and journal diameter. 
Radial clearance (C
r
) 
  Radial clearance = diameteral clearance 
                   2  
2
r
C
C =   
Diametral Clearance Ratio (D.C.R) 
It is the ratio of diametral clearance to diameter of journal.  
D.C.R = 
Diameteral clearance
Diameter of journal  
D.C.R = 
C
D 
Generally ,   
D.C.R = 0.001 
Eccentricity (e)  
  It is the radial distance between centre of bearing and centre of journal. 
    Eccentricity (e) = 
0
2
C
h    
Minimum oil film thickness (h
0
) 
  In completely lubricanted condition, the minium distance between bearing and journal 
is called h
0 
0
2
C
h   e =      
Eccentricity ratio ( c )   
  It is the ratio of eccentricity to radial clearance.   
(   )
2
e
C
c =  or 
2e
C 
Short, square, long bearing  
L= length of journal  
D= diameter of journal  
If 
L
D
< 1, bearing is called short bearing 
If 
L
D
= 1, bearing is called square bearing 
If 
L
D
> 1, bearing is called long bearing.  
Bearing characteristic number  
  In the design of journal bearing, calculation of loss of power due to friction is very 
important. Loss of power depends on the amount of bearing friction.  
  It is experimentally found that co-efficient of friction depends on three variables.  
1. 
b
ZN
p
       2. 
D
C
    3. 
L
D  
Z = Absolute viscosity of lubricant  
N = Speed of journal  
b
p = Bearing pressure  
Sommer Field Number  
  It  is  a  dimensionless  quantity.  It  is  an  important  parameter  in  the  design  of  journal 
bearing.  
  Sommer Field Number, 
2
6
'
10
b
ZN   D
S   X
p   C
|   |
=
     |
\   .  
  Where, 
    Z  = Absolute viscosity of oil in Kg/m-s 
    N= speed of journal in RPS 
    p
b 
 = bearing pressure in N/mm
2     
D = diameter of journal in mm 
    C = diameter clearance in mm. 
Values of sommerfield number is taken from table  
Note: 
  If  other  parameters  are  not  given  to  calculate  sommerfield  number,  table  cannot  be 
used. 
   In such case, sommerfield number is calculated as follows  
2
6
'
14.3
10
b
ZN   D
X
p   C
|   |
 =
   |
\   . 
Critical pressure of the journal bearing [p
c
]  
  The minimum pressure at which oil film breaks and metal to metal contact takes place 
is called critical pressure (or) minimum operating pressure of the bearing.  
Critical pressure, 
2
2
6
X
/
4.75 10
  X
c
ZN   D   L
p   N   mm
C   L   D
|   | |   |
   |    |
+
\   . \   .  
  L = Length of journal in mm  
Co- efficient of friction for journal bearing 
            [McKees equation] 
McKee  brothers  conducted  many  experiments  on  hydrodynamic  journal  bearing  and 
established a relationship between co-efficient of friction and other parameters as follows. 
6
0.326
10
  X   X
b
ZN   D
K
p   C
  |   |
=   +
   |
\   .
 
This is called McKees equation 
  K= correction factor for end leakage 
  Value of k is noted from graph 
Generally, K=0.002 for 
L
D
 ratio of from 0.75 to 2.8 
            [Refer to PSGDB   P.NO: 7.34] 
Heat generated in journal bearing 
  In journal bearing, power lost due to friction is generated in the form of heat. 
Temperature of lubricant oil and bearing surface is increased. 
  Heat generated, 
g
Q =   P V      J/sec (or) watts  
  Where,  
    Q
g 
= heat generated 
     = co-effecient of friction (calculated from McKees equation) 
    P or W = load on the bearing in Newton 
    V= rubbing velocity of journal in m/sec 
  Where, 
   
60 1000 X
DN
V
  t
= m/sec 
Heat dissipated by journal bearing  
  In journal bearing, heat is generated due to friction. Heat generated must be removed. 
Otherwise, babbit liner melts due to high temperature. 
  Heat dissipated by journal bearing depends on the following factors. 
1.  Temperature difference between bearing and surrounding air 
2.  Area of bearing surface exposed to air. 
3.  Amount of air contacting the bearing surface. 
Heat dissipated naturally is, 
. . .
6
10
C   L D   t
d
Q
d
A
=      J/sec (or) watts 
  Where,      
    Q
d 
= heat dissipated  
    C
d 
= heat dissipation co-efficient in  W/m
2
/
0
C 
        L x D = projected area of bearing in mm
2 
  (   )
0
1
2
b   a   a
t   t   t   t   t A =      =     
 
Where, 
 
b
t = bearing surface temp in 
0
C 
 
0
t = operating temp of oil film in 
0
C (60
0 
to 70
0
C) 
 
a
t = ambient temp in 
0
C 
Another method 
  By lasches equation 
     
2
6
( 18)
10
d
X
d
LD   t
Q
K
A +
=  J/sec or watts 
  K
d
= constant for heat dissipation in 
0
C/m
2
/W 
Design procedure for journal bearings 
1.  Calculation of torque (T) from power (P
0
) 
0
2
60 1000 X
NT
P
  t
=  
  Where, 
    P
0
= power transmitted in watts 
    N= speed of journal in RPM 
2.  Calculation of diameter of journal (D) 
3
16
T   D
t
  t =     N-mm 
t = shear stress in N/mm
2
 
3.  Suitable 
L
D
ratio is selected and bearing length L is determined. 
4.  Calculation of bearing pressure (p
d
) 
Load in newtons
Projected area of bearing
b
p =  
P or W
LD
b
p =  
5.  Clearance ratio
D
C
 is selected. 
6.  Select suitable viscosity(Z) of oil corresponding to oil temperature .