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A Reprint from Machinery Lubrication magazine
March - April 2008
Klüber Lubrication
32 Industrial Drive
Londonderry, NH 03053
(800) 447-2238
www.kluber.com
2 March - April 2008 machinerylubrication.com Machinery Lubrication
BY DENNIS A. LAUER, KLUBER LUBRICATION
I
n the past, the lubrication requirements for a specific appli-
cation could be satisfied by using general-purpose lubricants.
Lubricantselectionwastypicallybasedonexperienceandknowl-
edge. Today, this approach is no longer viable due to the
requirements of the current demanding environments to run
faster, longer and hotter. Today’s lubricants must satisfy extreme
requirements that are specific to each application.
Tribology - the study of friction, lubrication and wear - has
become the basis for selecting lubricants. The lubrication
requirements for a given application can be identified by
examining the effects of tribological system parameters on
lubricant chemistry.
Tribological System
Before the proper lubricant can be selected, the tribological
systemmustbeidentified.Thissystemincludesthetypeofmotion,
speed, temperatures, load and the operating environment.
Once these system parameters are identified, the lubrica-
tion engineer (or tribo-engineer) can utilize different
lubricant chemistries to select a lubricant that will optimize
the performance of the application. Because each chemistry
has advantages and disadvantages, it is important to choose
the appropriate one to address each of the tribological
system parameters.
In addition, the lubrication engineer must analyze the
application based on the identified tribological system. This
analysis includes elements such as speed factors, elastohy-
drodynamic (EHD) lubrication, bearing-life calculations,
extreme-pressure lubrication, emergency lubrication and
various special application requirements.
Type of Motion
The first parameter of the tribological system involves the
type of motion. The motion may be sliding, which would
require the hydrodynamic lubrication theory for its analysis, or
rolling, in which case EHD lubrication theory would be applied.
Combined sliding and rolling is also a possible form of
motion in certain rolling-element bearings including the
tapered roller bearing. Sliding in the rib area can occur in this
bearing, but the rolling elements roll on the raceway surfaces.
Lubricant protection of these types of motion can be opti-
mized with specific chemistries. Some lubricant chemistries
are effective in sliding contacts but do not perform as well in
rolling contacts.
Speed
Speed is the second parameter on the tribological system.
Speed of roller element bearings can be broken into the
Tribology: The Key to Proper
Lubricant Selection
LUBRICANT SELECTION
Figure 1. Minimum Allowable Viscosity for Lubrication of
Rolling-element Bearings at Operating Temperature
Minimumkinematicviscosity(V1),mm2
/s
Mean bearing diameter (dm), mm
3
5
10
20
50
100
200
500
1,000
0 20 50 100 200 500 1000
2
5
10
20
50
100
200
500
1,0001,5002,0003,000
10,00020,000
50,000100,000
Operatingspeed(n),rpm
general ranges: fast, moderate and slow. Specific ranges for
each of these speed categories can be set by using the speed
factor, as defined in Equation 1:
The Stribeck curve is a graph showing the relationship
between coefficient of friction and the dimensionless number
ηn/P, where η is dynamic viscosity, n is speed, and P is the
load per unit of projected area. According to this curve, there
is an optimum speed for the lubricated contact. Knowing the
speed of the contact, a lubricant can be selected with the
optimum physical attributes to minimize friction.
Temperature
The third tribological parameter is temperature. All lubri-
cants have specific temperature ranges for optimal
performance. Many lubricants have a broad operational
temperature range; however, some lubricants are more suited
for lower temperatures. For example, there are some greases
with synthetic hydrocarbon base oil and barium-complex
thickener that can operate at temperatures as low as -60°C.
Other lubricants are designed for high-temperature applica-
tions,suchasgreaseswithperfluorinatedaliphaticetherbaseoil
thickenedwithpolytetrafluoroethylene(PTFE)thatcanlubricate
an oven chain bearing at 220°C for more than 15,000 hours.
Knowing the temperature of the tribological system enables the
engineer to select a lubricant that will provide optimum oper-
ating life and performance at the application temperature.
Load
Load, the fourth parameter, is an important factor
affecting the lubricant requirement. A light load may indicate
the application is sensitive to frictional torque, and therefore
a lubricant would have to be selected to minimize the fluid
friction while still providing protection from metal-to-metal
friction. On the opposite end is a heavily loaded application,
which could require specific additives to help protect from
pitting, galling and extreme wear.
Operating Environment
The last parameter of the tribological system is the appli-
cation’s operating environment. If the environment includes
moisture or water, the lubricant must provide good anticor-
rosion properties as well as resistance to water washout or
contamination. If the application operates in a vacuum or
partial vacuum, the atmospheric pressure of the application
must be within the operational limits of the lubricant and
above its vapor pressure at the operating temperature.
If the application requires the presence of certain chemical
liquids or vapors, the selected lubricant must be resistant to
these chemicals. Even an ideal environment, such as a
computer room or clean-room processing facility, could have
specific requirements for noise-reducing lubricants in rolling-
element or instrument bearings.
Equation 1
OD = outside diameter, mm2
D = inside diameter, mm
= (ID +OD)/2
dm = mean bearing diameter, mm
n = operating speed, rpm
Speed factor = n•dm
Machinery Lubrication machinerylubrication.com March - April 2008 3
Figure 2. κκ Values
Lifeadjustmentfactorsrelatngto
operatingconditionsandbearingmaterial
0.05
0.1
0.2
0.5
1
2
5
0.05 0.1 0.2 0.5 1 2 5 10
Viscosity at operating temperature
Required viscosity for the bearing
K =
Kappa of 1 - 2.5 is desired
These circumstances often call for the
need of EP additives:
• Prevent problems with scoring at
rib and roller end interface
• High load conditions
• Shock loading
• Very low speeds
• Low Kappa
Minimum viscosity at operating
temperature:
• Ball bearing = 13.2 cSt
• Cylindrical and needle roller = 13.2 cSt
• Spherical (self-aligning) roller = 20 cSt
• Tapered roller = 20 cSt
• Spherical (self-aligning) roller
thrust= 33 cSt
Risks of too much viscosity:
• Skidding
• Viscous drag
• Heat/friction/energy consumption
• Retarded oil flow
A23
K = v/v1
Possible need of
EP oils when Kappa
is less than 1
Maximum bearing
life at Kappa of 4
Figure 3. Pressure-viscosity Coefficients for Five Oils Over the
Pressure Range 0 to 2,000 bar
Pressure-viscosity
coefficient(α)108
m2/N
1
2
3
4
5 10 100 1,000
Viscosity (V), mm2/s
Perfluorinated
aliphatic ether
Diester
Mineral
Polyglycol
Synthetic hydrocarbon
LUBRICANT SELECTION
4 March - April 2008 machinerylubrication.com Machinery Lubrication
Tribological Analysis Theories
The five parameters of the tribological system must be
taken into consideration and analyzed for the best lubricant
to be selected for the application. However, the information
obtained by defining the tribological system parameters also
provides data for further in-depth technical analysis.
EHD Lubrication Theory
An important type of analysis involves the lubrication
theory for rolling-element bearings. Elastohydrodynamic
(EHD) lubrication theory, sometimes referred to as EHL, is
used to identify a lubricant’s film thickness in a rolling
contact. A roller and a raceway can illustrate the factors
affecting the minimum film thickness, h0, in the area of
rolling contact. Assuming that both surfaces are perfectly
smooth, we can define the minimum film thickness, h0 in a
rolling contact situation according to Equation 2 which
forms the basis for EHD lubrication theory:
where
Lubrication engineers use the EHD lubrication theory to
select the proper viscosity of the lubricant. Each of the vari-
ables in Equation 2 has a specific impact on the ultimate film
thickness. Most of these variables are under the control of the
designer of the application, but several may also be under the
control of the lubrication engineer. One of the lubrication
engineer’s primary interests is how a change in a specific vari-
able will affect the magnitude of the film thickness.
From Equation 2, it can be determined that if the pressure-
viscosity coefficient (α) is doubled, there is an increase in the
film thickness by 51 percent. Knowing the pressure-viscosity
coefficient of the different lubricant chemistries, the lubrica-
tion engineer can alter the film thickness by changing the
lubricant chemistry. The remaining physical characteristics of
the lubricant are not changed.
Another lubricant-related variable in Equation 2 is the
dynamic viscosity, η. The dynamic viscosity can be directly
related to the kinematic viscosity, and if it is doubled, will
increase film thickness by 62 percent. By doubling the
velocity of the roller bearing, the film thickness of the lubri-
cant can again be increased by 62 percent. The lubrication
engineer has no control over the speed of the application, but
knowing how the speed affects the film thickness is impor-
tant to the selection of a lubricant when the application has
variable-speed capability. Additional variables have a lesser
impact on the film thickness of the lubricant.
WhiletheinformationinEquation2isimportanttothelubri-
cantselectioncriteria,theEHDfilmthicknessisnotuseddirectly
because in reality, surfaces are not perfectly smooth. Instead of
minimum film thickness, the lubrication engineer works with the
specific film thickness, λ, defined as the ratio between the
average or mean EHD film thickness, a, and the composite
surface roughness of the rolling contacts σ (equation 3).
where
= ( σ1
2 + σ2
2)½
σ = composite roughness of the two contact surfaces
λ = specific film thickness
λ = h0/σ
Equation 2
1/m = Poisson’s ration
= 2.08 x 105 for steel
E = modulus of elasticity, N/mm2
L = roller length, mm
Q = roller load, N
r2 = inner ring raceway radius, mm
r1 = roller radium, mm
v2 = raceway velocity, m/s
v1 = roller velocity, m/s
v = (v1 + v2)/2, m/s
η = dynamic viscosity, mPa•s
α = pressure-viscosity coefficient, mm2/N
h0 = minimum lubricating film thickness in area of
rolling contact, μm
{E/[1-(1/m2)]}0.03
/{[(1/r1) +(1/r2)0.43(Q/l)0.13})
h0 =([0.1 x α0.6 x (ηv)0.07])
From Equation 3, it is clear that if the specific film
thickness is close to zero, there will be a dramatic increase
in the metal-to-metal contact at the friction point. This
increased metal contact produces unacceptable wear.
When λ=1, the bearing will have only partially separated the
metal asperities and some metal-to-metal contact will still
be occurring.
It is at this point that the transition from boundary lubri-
cation into the mixed lubrication occurs. As the specific film
thickness increases above 1 and approaches values greater
than 3, there will be a decrease in metal-to-metal contact
with an associated decrease in wear. When λ = 3 to 4 or
greater, there is full metal separation between the peaks, indi-
cating full fluid film lubrication and an absence of wear.
Lambda values greater than 4 are possible and sometimes
desirable, particularly where variable speeds and or shock
loading is present. However as λ increases beyond 4, the
internal fluid friction may increase and generate excessive
heating and energy consumption depending upon the relative
bearing speed and oil viscosity.
Required Viscosity
Research sponsored by the bearing manufacturers has
made it possible to calculate the minimum required viscosity
of the lubricant V1 to obtain separation of the moving
surfaces. The nomograph in Figure 1 can be used to deter-
mine the value of V1 from the mean bearing diameter, dm,
and the operating speed, n.
For example, enter the bottom of the chart with the
average diameter of the rolling-element bearing (100 mm),
then proceed vertically to the speed of the bearing (2,000
rpm). Drawing a line horizontally to the left then provides
the required viscosity (10mm2/s) to obtain λ = 1 in this
specific application at the given operating temperature.
Knowing the required minimum viscosity, V1, at operating
temperature, the lubrication engineer can then select the
appropriate lubricant based on the specific viscosity, κ,
which is defined as the ratio of the actual viscosity, V, of the
selected lubricant to the required minimum viscosity, V1.
Given this information, the engineer will attempt to select a
lubricant to meet the full fluid film lubrication regime for the
application. If this is not possible, then the next available
option is to select a lubricant that provides the best protec-
tion to the application.
Figure 2 shows how κ relates to both lubricant selection
and expected bearing life. At κ values below 1, it is generally
accepted that EP additives will be required to mitigate the
effects of boundary lubrication conditions. As κ approaches
1, the life expectancy approaches the rated life expectancy L
of the bearing according to DIN ISO 281. At κ values above
1, it is in fact possible to exceed the L value of the bearings,
perhaps by as much as 2.5 times.
As κ approaches 4, the bearing life approaches a
maximum (all else being equal) while κ values above 4
may cause increase fluid friction, viscous drag, ball skidding
and other undesirable effects. It is generally accepted
that ê values in the 1 to 2.5 range are optimal for most
bearing applications.
If the application must be operated in the boundary lubri-
cation regime, then specific additives must be provided to
protect the metal contact points. If the application is oper-
ating in a lubrication regime that approaches full fluid film
lubrication, these extreme-pressure additives can be elimi-
nated from the lubricant.
Points of Consideration
The EHD theory is a valuable tool in guiding the lubrica-
tion engineer toward selecting the proper lubricant. If the
lubrication engineer uses the specific viscosity as part of the
selection criteria, the assumptions used in the analysis must
be taken into consideration, along with the controllable vari-
ables. Two specific points should be considered:
1. Calculation of film thickness (h0), specific film thickness
(λ), and the chart used to determine required viscosity
(V1) are all based on the pressure-viscosity coefficient (α)
of mineral oil. Figure 3 shows the pressure-viscosity coef-
ficient for mineral oil and four other oils over the pressure
range zero to 2,000 bar.
2. The oil is considered to be the only lubricating component
of the lubricant. In a grease, it is believed that the thick-
ener system does not contribute to the lubricating film
thickness. However, the thickener system can have a
significant effect on film thickness.
Figure 4 documents research identifying the effect of a
grease thickener system on the actual film thickness. The
upper chart shows that a clay-thickened grease will reduce
Equation 3
σ2 = rms roughness of roller, μm
σ1 = rms roughness of raceway, μm
Machinery Lubrication machinerylubrication.com March - April 2008 5
LUBRICANT SELECTION
6 March - April 2008 machinerylubrication.com Machinery Lubrication
the film thickness of the application to almost 50 percent of
the film thickness provided by the base oil alone. A grease
thickened with a barium-complex soap has the opposite
effect of almost doubling the film thickness relative to the
base oil alone.
However, as shown in the lower chart in Figure 4, the
advantage of increased load-carrying film thickness comes
with the disadvantage of frictional torque. While a clay-thick-
ened grease reduces the film thickness, it does have the
benefit of reducing frictional torque in the bearing. The
opposite effect is observed for grease thickened with a
barium-complex soap.
Speed Factor and
Bearing Design
Speed is another parameter of the tribological system that
requires further detailed analysis. The calculated speed factor
for a rolling-element bearing, which is defined as the product
of bearing speed (n) and mean bearing diameter (dm), is not
consistent for all bearings with the same dimensions and
speed. The lubrication engineer must apply a correction to
the calculated speed factor, depending on the bearing design.
Lubricant Selection Criteria
Tribological System
Analysis of the tribological system for a given application
is essential to the selection of the appropriate lubricant.
• Service temperature range
• Speed factor (n•dm)
• Hydrodynamic lubrication
• Elastohydrodynamic lubrication
• Extreme pressure
• Emergency lubrication
• Fretting
Special Requirements
Many applications have special requirements that go
beyond the tribological system that must be taken into
consideration. Some applications are limited to oils, while
others require a grease. Applications that involve the use of
sintered bearings or special sealing arrangements will require
additional analysis. Material compatibility is another impor-
tant issue.
Other Requirements
Lubricant selection can also be affected by a variety of other
specialized requirements:
• Design life
• Lubrication equipment
• Acceptable relubrication intervals
• Cost
• Special certifications such as NSF registration
• Biodegradability
Summary
Multipurpose lubricants cannot provide satisfactory
service in current demanding environments. Lubricant
performance must be optimized to meet the increasing
demands of modern industry.
The first step in selecting the best lubricant for a given
application is to define the tribological system. With a fully
defined tribological system in place, the next step is theo-
retical analysis. Selection of a lubricant based on EHD
lubrication analysis or analysis of any other discrete param-
eter is inappropriate, because such analyses focus only on a
subset of the tribological system.
About the Author
Dennis Lauer is vice president-engineering for Kluber Lubrication North
America LP.
Figure 4. Film Thickness and Frictional Torque for Base Oil
and Five Greases as Functions of Bearing Speed
FrictionalTorque,N•mm
Speed, rpm
0
1,000
2,000
3,000
3,000
5,000
6,000
2
0 40 80 120 160
Filmthickness
µm
0
1
0 40 80 120 160
E
C
B
D
A
E
C
B
D
A
Base oil
Base oil
A Clay
B Lithium soap
C Sodium soap
D Calcium-complex soap
E Barium-complex soap

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Cara Menggugurkan Sperma Yang Masuk Rahim Biyar Tidak Hamil
 

Tribology proper lubricant_selection Mr Tùng - 0987 988 407 | www.khodaumo.com

  • 1. A Reprint from Machinery Lubrication magazine March - April 2008 Klüber Lubrication 32 Industrial Drive Londonderry, NH 03053 (800) 447-2238 www.kluber.com
  • 2. 2 March - April 2008 machinerylubrication.com Machinery Lubrication BY DENNIS A. LAUER, KLUBER LUBRICATION I n the past, the lubrication requirements for a specific appli- cation could be satisfied by using general-purpose lubricants. Lubricantselectionwastypicallybasedonexperienceandknowl- edge. Today, this approach is no longer viable due to the requirements of the current demanding environments to run faster, longer and hotter. Today’s lubricants must satisfy extreme requirements that are specific to each application. Tribology - the study of friction, lubrication and wear - has become the basis for selecting lubricants. The lubrication requirements for a given application can be identified by examining the effects of tribological system parameters on lubricant chemistry. Tribological System Before the proper lubricant can be selected, the tribological systemmustbeidentified.Thissystemincludesthetypeofmotion, speed, temperatures, load and the operating environment. Once these system parameters are identified, the lubrica- tion engineer (or tribo-engineer) can utilize different lubricant chemistries to select a lubricant that will optimize the performance of the application. Because each chemistry has advantages and disadvantages, it is important to choose the appropriate one to address each of the tribological system parameters. In addition, the lubrication engineer must analyze the application based on the identified tribological system. This analysis includes elements such as speed factors, elastohy- drodynamic (EHD) lubrication, bearing-life calculations, extreme-pressure lubrication, emergency lubrication and various special application requirements. Type of Motion The first parameter of the tribological system involves the type of motion. The motion may be sliding, which would require the hydrodynamic lubrication theory for its analysis, or rolling, in which case EHD lubrication theory would be applied. Combined sliding and rolling is also a possible form of motion in certain rolling-element bearings including the tapered roller bearing. Sliding in the rib area can occur in this bearing, but the rolling elements roll on the raceway surfaces. Lubricant protection of these types of motion can be opti- mized with specific chemistries. Some lubricant chemistries are effective in sliding contacts but do not perform as well in rolling contacts. Speed Speed is the second parameter on the tribological system. Speed of roller element bearings can be broken into the Tribology: The Key to Proper Lubricant Selection LUBRICANT SELECTION Figure 1. Minimum Allowable Viscosity for Lubrication of Rolling-element Bearings at Operating Temperature Minimumkinematicviscosity(V1),mm2 /s Mean bearing diameter (dm), mm 3 5 10 20 50 100 200 500 1,000 0 20 50 100 200 500 1000 2 5 10 20 50 100 200 500 1,0001,5002,0003,000 10,00020,000 50,000100,000 Operatingspeed(n),rpm
  • 3. general ranges: fast, moderate and slow. Specific ranges for each of these speed categories can be set by using the speed factor, as defined in Equation 1: The Stribeck curve is a graph showing the relationship between coefficient of friction and the dimensionless number ηn/P, where η is dynamic viscosity, n is speed, and P is the load per unit of projected area. According to this curve, there is an optimum speed for the lubricated contact. Knowing the speed of the contact, a lubricant can be selected with the optimum physical attributes to minimize friction. Temperature The third tribological parameter is temperature. All lubri- cants have specific temperature ranges for optimal performance. Many lubricants have a broad operational temperature range; however, some lubricants are more suited for lower temperatures. For example, there are some greases with synthetic hydrocarbon base oil and barium-complex thickener that can operate at temperatures as low as -60°C. Other lubricants are designed for high-temperature applica- tions,suchasgreaseswithperfluorinatedaliphaticetherbaseoil thickenedwithpolytetrafluoroethylene(PTFE)thatcanlubricate an oven chain bearing at 220°C for more than 15,000 hours. Knowing the temperature of the tribological system enables the engineer to select a lubricant that will provide optimum oper- ating life and performance at the application temperature. Load Load, the fourth parameter, is an important factor affecting the lubricant requirement. A light load may indicate the application is sensitive to frictional torque, and therefore a lubricant would have to be selected to minimize the fluid friction while still providing protection from metal-to-metal friction. On the opposite end is a heavily loaded application, which could require specific additives to help protect from pitting, galling and extreme wear. Operating Environment The last parameter of the tribological system is the appli- cation’s operating environment. If the environment includes moisture or water, the lubricant must provide good anticor- rosion properties as well as resistance to water washout or contamination. If the application operates in a vacuum or partial vacuum, the atmospheric pressure of the application must be within the operational limits of the lubricant and above its vapor pressure at the operating temperature. If the application requires the presence of certain chemical liquids or vapors, the selected lubricant must be resistant to these chemicals. Even an ideal environment, such as a computer room or clean-room processing facility, could have specific requirements for noise-reducing lubricants in rolling- element or instrument bearings. Equation 1 OD = outside diameter, mm2 D = inside diameter, mm = (ID +OD)/2 dm = mean bearing diameter, mm n = operating speed, rpm Speed factor = n•dm Machinery Lubrication machinerylubrication.com March - April 2008 3 Figure 2. κκ Values Lifeadjustmentfactorsrelatngto operatingconditionsandbearingmaterial 0.05 0.1 0.2 0.5 1 2 5 0.05 0.1 0.2 0.5 1 2 5 10 Viscosity at operating temperature Required viscosity for the bearing K = Kappa of 1 - 2.5 is desired These circumstances often call for the need of EP additives: • Prevent problems with scoring at rib and roller end interface • High load conditions • Shock loading • Very low speeds • Low Kappa Minimum viscosity at operating temperature: • Ball bearing = 13.2 cSt • Cylindrical and needle roller = 13.2 cSt • Spherical (self-aligning) roller = 20 cSt • Tapered roller = 20 cSt • Spherical (self-aligning) roller thrust= 33 cSt Risks of too much viscosity: • Skidding • Viscous drag • Heat/friction/energy consumption • Retarded oil flow A23 K = v/v1 Possible need of EP oils when Kappa is less than 1 Maximum bearing life at Kappa of 4 Figure 3. Pressure-viscosity Coefficients for Five Oils Over the Pressure Range 0 to 2,000 bar Pressure-viscosity coefficient(α)108 m2/N 1 2 3 4 5 10 100 1,000 Viscosity (V), mm2/s Perfluorinated aliphatic ether Diester Mineral Polyglycol Synthetic hydrocarbon
  • 4. LUBRICANT SELECTION 4 March - April 2008 machinerylubrication.com Machinery Lubrication Tribological Analysis Theories The five parameters of the tribological system must be taken into consideration and analyzed for the best lubricant to be selected for the application. However, the information obtained by defining the tribological system parameters also provides data for further in-depth technical analysis. EHD Lubrication Theory An important type of analysis involves the lubrication theory for rolling-element bearings. Elastohydrodynamic (EHD) lubrication theory, sometimes referred to as EHL, is used to identify a lubricant’s film thickness in a rolling contact. A roller and a raceway can illustrate the factors affecting the minimum film thickness, h0, in the area of rolling contact. Assuming that both surfaces are perfectly smooth, we can define the minimum film thickness, h0 in a rolling contact situation according to Equation 2 which forms the basis for EHD lubrication theory: where Lubrication engineers use the EHD lubrication theory to select the proper viscosity of the lubricant. Each of the vari- ables in Equation 2 has a specific impact on the ultimate film thickness. Most of these variables are under the control of the designer of the application, but several may also be under the control of the lubrication engineer. One of the lubrication engineer’s primary interests is how a change in a specific vari- able will affect the magnitude of the film thickness. From Equation 2, it can be determined that if the pressure- viscosity coefficient (α) is doubled, there is an increase in the film thickness by 51 percent. Knowing the pressure-viscosity coefficient of the different lubricant chemistries, the lubrica- tion engineer can alter the film thickness by changing the lubricant chemistry. The remaining physical characteristics of the lubricant are not changed. Another lubricant-related variable in Equation 2 is the dynamic viscosity, η. The dynamic viscosity can be directly related to the kinematic viscosity, and if it is doubled, will increase film thickness by 62 percent. By doubling the velocity of the roller bearing, the film thickness of the lubri- cant can again be increased by 62 percent. The lubrication engineer has no control over the speed of the application, but knowing how the speed affects the film thickness is impor- tant to the selection of a lubricant when the application has variable-speed capability. Additional variables have a lesser impact on the film thickness of the lubricant. WhiletheinformationinEquation2isimportanttothelubri- cantselectioncriteria,theEHDfilmthicknessisnotuseddirectly because in reality, surfaces are not perfectly smooth. Instead of minimum film thickness, the lubrication engineer works with the specific film thickness, λ, defined as the ratio between the average or mean EHD film thickness, a, and the composite surface roughness of the rolling contacts σ (equation 3). where = ( σ1 2 + σ2 2)½ σ = composite roughness of the two contact surfaces λ = specific film thickness λ = h0/σ Equation 2 1/m = Poisson’s ration = 2.08 x 105 for steel E = modulus of elasticity, N/mm2 L = roller length, mm Q = roller load, N r2 = inner ring raceway radius, mm r1 = roller radium, mm v2 = raceway velocity, m/s v1 = roller velocity, m/s v = (v1 + v2)/2, m/s η = dynamic viscosity, mPa•s α = pressure-viscosity coefficient, mm2/N h0 = minimum lubricating film thickness in area of rolling contact, μm {E/[1-(1/m2)]}0.03 /{[(1/r1) +(1/r2)0.43(Q/l)0.13}) h0 =([0.1 x α0.6 x (ηv)0.07])
  • 5. From Equation 3, it is clear that if the specific film thickness is close to zero, there will be a dramatic increase in the metal-to-metal contact at the friction point. This increased metal contact produces unacceptable wear. When λ=1, the bearing will have only partially separated the metal asperities and some metal-to-metal contact will still be occurring. It is at this point that the transition from boundary lubri- cation into the mixed lubrication occurs. As the specific film thickness increases above 1 and approaches values greater than 3, there will be a decrease in metal-to-metal contact with an associated decrease in wear. When λ = 3 to 4 or greater, there is full metal separation between the peaks, indi- cating full fluid film lubrication and an absence of wear. Lambda values greater than 4 are possible and sometimes desirable, particularly where variable speeds and or shock loading is present. However as λ increases beyond 4, the internal fluid friction may increase and generate excessive heating and energy consumption depending upon the relative bearing speed and oil viscosity. Required Viscosity Research sponsored by the bearing manufacturers has made it possible to calculate the minimum required viscosity of the lubricant V1 to obtain separation of the moving surfaces. The nomograph in Figure 1 can be used to deter- mine the value of V1 from the mean bearing diameter, dm, and the operating speed, n. For example, enter the bottom of the chart with the average diameter of the rolling-element bearing (100 mm), then proceed vertically to the speed of the bearing (2,000 rpm). Drawing a line horizontally to the left then provides the required viscosity (10mm2/s) to obtain λ = 1 in this specific application at the given operating temperature. Knowing the required minimum viscosity, V1, at operating temperature, the lubrication engineer can then select the appropriate lubricant based on the specific viscosity, κ, which is defined as the ratio of the actual viscosity, V, of the selected lubricant to the required minimum viscosity, V1. Given this information, the engineer will attempt to select a lubricant to meet the full fluid film lubrication regime for the application. If this is not possible, then the next available option is to select a lubricant that provides the best protec- tion to the application. Figure 2 shows how κ relates to both lubricant selection and expected bearing life. At κ values below 1, it is generally accepted that EP additives will be required to mitigate the effects of boundary lubrication conditions. As κ approaches 1, the life expectancy approaches the rated life expectancy L of the bearing according to DIN ISO 281. At κ values above 1, it is in fact possible to exceed the L value of the bearings, perhaps by as much as 2.5 times. As κ approaches 4, the bearing life approaches a maximum (all else being equal) while κ values above 4 may cause increase fluid friction, viscous drag, ball skidding and other undesirable effects. It is generally accepted that ê values in the 1 to 2.5 range are optimal for most bearing applications. If the application must be operated in the boundary lubri- cation regime, then specific additives must be provided to protect the metal contact points. If the application is oper- ating in a lubrication regime that approaches full fluid film lubrication, these extreme-pressure additives can be elimi- nated from the lubricant. Points of Consideration The EHD theory is a valuable tool in guiding the lubrica- tion engineer toward selecting the proper lubricant. If the lubrication engineer uses the specific viscosity as part of the selection criteria, the assumptions used in the analysis must be taken into consideration, along with the controllable vari- ables. Two specific points should be considered: 1. Calculation of film thickness (h0), specific film thickness (λ), and the chart used to determine required viscosity (V1) are all based on the pressure-viscosity coefficient (α) of mineral oil. Figure 3 shows the pressure-viscosity coef- ficient for mineral oil and four other oils over the pressure range zero to 2,000 bar. 2. The oil is considered to be the only lubricating component of the lubricant. In a grease, it is believed that the thick- ener system does not contribute to the lubricating film thickness. However, the thickener system can have a significant effect on film thickness. Figure 4 documents research identifying the effect of a grease thickener system on the actual film thickness. The upper chart shows that a clay-thickened grease will reduce Equation 3 σ2 = rms roughness of roller, μm σ1 = rms roughness of raceway, μm Machinery Lubrication machinerylubrication.com March - April 2008 5
  • 6. LUBRICANT SELECTION 6 March - April 2008 machinerylubrication.com Machinery Lubrication the film thickness of the application to almost 50 percent of the film thickness provided by the base oil alone. A grease thickened with a barium-complex soap has the opposite effect of almost doubling the film thickness relative to the base oil alone. However, as shown in the lower chart in Figure 4, the advantage of increased load-carrying film thickness comes with the disadvantage of frictional torque. While a clay-thick- ened grease reduces the film thickness, it does have the benefit of reducing frictional torque in the bearing. The opposite effect is observed for grease thickened with a barium-complex soap. Speed Factor and Bearing Design Speed is another parameter of the tribological system that requires further detailed analysis. The calculated speed factor for a rolling-element bearing, which is defined as the product of bearing speed (n) and mean bearing diameter (dm), is not consistent for all bearings with the same dimensions and speed. The lubrication engineer must apply a correction to the calculated speed factor, depending on the bearing design. Lubricant Selection Criteria Tribological System Analysis of the tribological system for a given application is essential to the selection of the appropriate lubricant. • Service temperature range • Speed factor (n•dm) • Hydrodynamic lubrication • Elastohydrodynamic lubrication • Extreme pressure • Emergency lubrication • Fretting Special Requirements Many applications have special requirements that go beyond the tribological system that must be taken into consideration. Some applications are limited to oils, while others require a grease. Applications that involve the use of sintered bearings or special sealing arrangements will require additional analysis. Material compatibility is another impor- tant issue. Other Requirements Lubricant selection can also be affected by a variety of other specialized requirements: • Design life • Lubrication equipment • Acceptable relubrication intervals • Cost • Special certifications such as NSF registration • Biodegradability Summary Multipurpose lubricants cannot provide satisfactory service in current demanding environments. Lubricant performance must be optimized to meet the increasing demands of modern industry. The first step in selecting the best lubricant for a given application is to define the tribological system. With a fully defined tribological system in place, the next step is theo- retical analysis. Selection of a lubricant based on EHD lubrication analysis or analysis of any other discrete param- eter is inappropriate, because such analyses focus only on a subset of the tribological system. About the Author Dennis Lauer is vice president-engineering for Kluber Lubrication North America LP. Figure 4. Film Thickness and Frictional Torque for Base Oil and Five Greases as Functions of Bearing Speed FrictionalTorque,N•mm Speed, rpm 0 1,000 2,000 3,000 3,000 5,000 6,000 2 0 40 80 120 160 Filmthickness µm 0 1 0 40 80 120 160 E C B D A E C B D A Base oil Base oil A Clay B Lithium soap C Sodium soap D Calcium-complex soap E Barium-complex soap