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Pressure gradient in a translating and squeezing finite gap
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Fluid mechanics
Viscous fluid flow
Lubrication theory
Couette-Poiseuille flow in a thin gap
Moving-boundary lubrication flux
Reynolds lubrication equation
Created
2026-09-24
Updated
2026-10-05
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For lower
speed
U
, stationary upper
tangential speed
, upper normal
speed
−
V
, and equal endpoint
pressures
,
define
⟨
f
⟩
=
L
−
1
∫
0
L
f
(
x
)
d
x
. Then
p
x
=
h
2
6
μU
−
h
3
12
μ
(
V
x
+
C
)
,
(1)
where
C
=
2
U
⟨
h
−
3
⟩
⟨
h
−
2
⟩
−
V
⟨
h
−
3
⟩
⟨
x
h
−
3
⟩
.
(2)
Table of contents
Zero-shear lower wall in a translating and squeezing finite gap
Pressure gradient in a translating and squeezing finite gap
Zero-shear lower wall in a translating and squeezing finite gap
0
0
0
Pressure gradient in a translating and squeezing finite gap
The horizontal
force
on the lower wall vanishes when
U
=
6
V
4
⟨
h
−
1
⟩
−
3
⟨
h
−
2
⟩
2
/
⟨
h
−
3
⟩
⟨
x
h
−
2
⟩
−
⟨
h
−
2
⟩
⟨
x
h
−
3
⟩
/
⟨
h
−
3
⟩
.
(1)
Ancestors
(9)
Reynolds lubrication equation
Moving-boundary lubrication flux
Couette-Poiseuille flow in a thin gap
Lubrication theory
Viscous fluid flow
Fluid mechanics
Branch of physics
Physics
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Incoming links
(1)
Past exam of the mathematics course of the University of Cambridge
/
2023
/
ii
/
Paper 3
/
38C
/
c
/
Solution
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