Tribology Lecture I - PowerPoint PPT Presentation

1 / 23
About This Presentation
Title:

Tribology Lecture I

Description:

Tribology Lecture I From: = rubbing Friction Wear Lubrication Friction Loss of energy due to rubbing. Energy is converted to heat Extra energy and ... – PowerPoint PPT presentation

Number of Views:513
Avg rating:3.0/5.0
Slides: 24
Provided by: PeterR71
Category:

less

Transcript and Presenter's Notes

Title: Tribology Lecture I


1
TribologyLecture I
2
From ?????? rubbing
Tribology
Tribology deals with all aspects of
interacting surfaces in relative motion
  • Friction
  • Wear
  • Lubrication

- bearings
3
Friction
  • Loss of energy due to rubbing. Energy is
    converted to heat
  • Extra energy and force required to overcome
    friction
  • Causes wear and failure

4
Friction Amontons Law
W
Ffriction
A
V
5
Origin of Friction
  • Surface Roughness
  • Solid to solid contact
  • Adhesion
  • Deformation

6
Lubrication
Replace Solid to solid contact
Fluid Layer
with a fluid layer - i.e. a lubricant
7
Lubrication
Solid rubbing replaced by
Fluid Layer
viscous shearing
8
To be useful must support some load
W
Fluid Layer
9
To be useful must support some load
W
10
To be useful must support some load
W
Fluid Layer
p
Need pressure in the fluid to support the load
11
Hydrodynamic Lubrication
W
Fluid Layer
p
Pressure is generated by motion and geometry of
the the bearing in concert with the viscosity of
the lubricant
12
1-D Reynolds Equation
W
z
h(x)
ho
x
U
13
z
h
h0
p
t
Infinitesimal element
U
p
x
B
0
14
Force balance
Viscosity equation
Combine
15
Integrate wrt z
Apply BCs
No-slip ux U at z 0, ux 0 at z h
yields
Volumetric flow rate (per unit width)
Incompressible flow, q const. Evaluate at dp/dx
0
Solve for dp/dx
16
1-D Reynolds Equation
wn
z
h(x)
ho
x
U
Reynolds Equation
  • Integrate over x to get p(x)
  • Integrate over x again to get Wn
  • Result gives ho in terms of U, ?, Wn

17
Example Exponential h
B
wn
z
h(x)
ho
x
integrate wrt x apply BCs p 0 at x 0 and
at x -B
solve for p(x), integrate to get Wn/L, then solve
for h0
18
2-D Reynolds Equation
w
Sphere
R
z
Fluid Layer
hc
x
For sphere
Exact solution
19
Hydrodynamic LubricationPoint Contact
W
Sphere
R
Fluid Layer
hc
20
Hydrodynamic Lubrication(Refinement Both
surfaces moving)
W
Sphere
R
U1
Fluid Layer
hc
U2
Entrainment or Rolling Velocity
21
Hydrodynamic Lubrication(Refinement two spheres)
W
R1
U1
hc
U2
Where R is now reduced radius
R2
1
22
Hydrodynamic Lubrication
W
R1
U1
Nice theory but as a rule it greatly under
estimates hc
hc
U2
  • Pressure is very high near contact
  • P gtgt1000atm ( 108 Pa)
  • Pressure Dependence of ?
  • Elastic Deformation of Sphere

R2
23
Hydrodynamic Lubrication
Elasto-Hydrodynamic Lubrication
Write a Comment
User Comments (0)
About PowerShow.com