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TRANSCRIPT
Behavior of Plain Elastomeric
Pads
John Stanton & Scott Tetzlaff
University of Washington
AASHTO SCOBS T-2 Meeting
9 July 2012, Austin, TX.
Acknowledgments
• AASHTO
• MN DOT
Plain Elastomeric Pads – the
Problem.
• Plain pads are made from unreinforced
sheets of elastomer (Natural Rubber or
Neoprene.)
• MN DOT found plain pads bulging out
from the plates that they support.
• Was something wrong with the rubber?
• Are the AASHTO design values at fault?
MNDOT bearing
Girder
Steel
rocker
Elastomeric
pad
Welded
studs
Concrete
pier cap
MNDOT bearing
MNDOT bearing
Plain Pad in Compression
Plain Pad in Compression
Plain Pad in Compression
Slip No slip Slip
Comparison with Steel-Laminated
Bearing
Comparison with Steel-Laminated
Bearing
No lateral expansion –
bonded to internal plates
Plain Pad in Compression
Slip No slip Slip
Rubber volume stays constant.
Lateral expansion implies vertical deflection.
Expansion resisted by friction (m) and rubber stiffness, G.
Compression Stiffness.
Reinforced (bonded) Bearing
t
AEK cc
Kc = stiffness
A = plan area
t = rubber thickness
Ec = Effective modulus
S = Shape Factor
W
L
ti
WLt
LWS
i
224GSEc
Compression Stiffness. Plain pad
LRBcKPEPc EfE ,,
fK ≈ 0.75m (Nasty math. Depends on slip/no slip boundary).
Assumes: Incompressible material.
W = infinite (strip bearing).
Constant m (independent of contact pressure).
Plain pads:
Compression Stiffness Factor
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.2 0.4 0.6 0.8 1
m
f K
S = 2
S = 3
S = 4
S = 6
S = 8
approx
t
AEK cc
Test Plan
Compression test variables:
Elastomer material
Contact surface (may affect friction)
Shape factor
Aspect ratio
Loading type and level
Friction test variables
Contact pressure
Compression Test Matrix
Test Rubber Contact Length Width S AR Loading
Name Material Surface (inch) (inch)
1.GG.24.12 Lot 1 GG 24 12 8 2 Cyc
2.GG.24.12 Lot 2 GG 24 12 8 2 Cyc
1.CC.24.12 Lot1 CC 24 12 8 2 Cyc
1.SS.24.12 Lot1 SS 24 12 8 2 Cyc
1.CS.24.12 Lot1 CS 24 12 8 2 Cyc
1.GG.12.06 Lot1 GG 12 6 4 2 Cyc
1.GG.06.03 Lot1 GG 6 3 2 2 Cyc
1.GG.24.05 Lot1 GG 24 4.8 4 5 Cyc
1.GG.24.02 Lot1 GG 24 2.18 2 11 Cyc
1.GG.24.12 Creep Lot1 GG 24 12 8 2 Creep
1.GG.24.12.Alt Lot1 GG 24 12 8 2 Alt cyc
1.GG.24.12.Offset Lot1 GG 24 12 8 2 Offset
Test set up
Loading
beam
Galvanized
plate
Rubber pad
Concrete block on
steel plate
CROSS-SECTION
Instrumentation.
Horizontal
potentiometer
PLAN
Vertical
potentiometer
Loading Protocol.
Loading Protocols
0
100
200
300
400
500
600
700
800
900
1000
0 200 400 600 800 1000 1200
Time (sec)
Stre
ss, p
si
Normal loading
Alt loading
Test Results – Vertical Strain.
Plain Pad Compression Test: 1.GG.24.12
0
100
200
300
400
500
600
700
800
900
1000
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5
Axial Strain, in/in
Stre
ss, p
si
"200"
"400"
"600"
"800"
• Zero for strain difficult to define: “bedding in”.
• eel ≈ 12% at 800 psi
• Large “creep” strains
Test Results - Lateral Strain.
• Lateral strain = average slip on long sides/short dimension.
• Strain zero does not need adjustment.
• Lateral strain ≈ vertical strain (constant volume).
Plain Pad Compression Test: 1.GG.24.12
0
100
200
300
400
500
600
700
800
900
1000
0 0.05 0.1 0.15 0.2 0.25 0.3Lateral Strain, in/in
Stre
ss, p
si
Test Results - Lateral Strain.
Compression Test Results.
Marks on rubber showing slip region.
No cracks or other damage.
Compression Test Results.
Cyclic loading & creep cause additional deflection.
Total strain comparable to galvanized (1.GG.24.12).
Plain Pad Compression Test: 1.CC.24.12
0
100
200
300
400
500
600
700
800
0 0.05 0.1 0.15 0.2
Lateral Strain, in/in
Stre
ss, p
si
Test Results.
High Aspect Ratio (11.0), Low S ( 2.0).
High elastic strains, lower creep strains.
Plain Pad Compression Test: 1.GG.24.02
0
100
200
300
400
500
600
700
800
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4
Lateral Strain, in/in
Stre
ss, p
si
Test Results - Creep.
Creep increases significantly above 400 psi (= 0.5GS)
Compression Tests: 2.GG.24.12.Creep
0
100
200
300
400
500
600
700
800
900
1000
0 0.05 0.1 0.15 0.2 0.25 0.3
Lateral Strain, in/in
Stre
ss, p
si
Test Results – Creep Rate.
Compression Tests:
2.GG.24.12.Creep
0
100
200
300
400
500
600
700
800
900
0 1000 2000 3000 4000 5000 6000 7000
Time (sec)
Late
ral S
trai
n R
ate
( me
/se
c)
Compression Tests:
2.GG.24.12.Creep
0
0.05
0.1
0.15
0.2
0.25
0.3
0 1000 2000 3000 4000 5000 6000 7000
Time (sec)
Late
ral S
trai
n (
in/i
n)
Compression Test Results -
Summary.
• Elastomer: Negligible effect.
• Contact Surface: Little effect.
• Shape Factor: High S higher elastic stiffness.
• Aspect Ratio: Little effect. (High AR less stiff).
• Loading: Large effect. Creep and cyclic load:
large increase in deflections.
Friction tests
3 steel plates (24” x 12”). (2 galvanized, 1 as-rolled).
2 rubber pads (6” x 3”).
Contact pressures: 200, 400, 600 psi.
Friction tests
Friction tests
FrictionTest: 600psi
0
0.1
0.2
0.3
0.4
0.5
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6
Deflection (in)
F/N
Elastic shear
deformation Sliding
Friction tests
Coefficient of friction:
Rubber vs. bare steel
0
0.1
0.2
0.3
0.4
0.5
0.6
0 100 200 300 400 500 600 700
Compressive stress (psi)
m
mu
Previous studies have also found that rubber friction
varies with contact pressure. Similar to PTFE.
Data Analysis
• Quantify the effects of the various parameters on
compression stiffness.
• Use the measured friction coefficients in the analytical
model to compare predicted and measured
compression stiffnesses.
Data Analysis Contact Surface (Concrete, Steel, Galvanized)
Laterals strain shown includes creep.
Bare steel has lowest friction, highest lateral strain.
Differences are small.
Data Analysis Shape Factor, S.
Effect of Shape Factor
0
0.5
1
1.5
2
2.5
3
3.5
0 5 10 15 20 25 30 35
Lateral Strain, %
Max
Str
ess/
GS
S= 8 AR= 2
S= 4 AR= 2
S= 2 AR= 2
For 24” x 12” pad, rubber squeezed out from plates.
For smaller pads, rubber remained between plates.
Data Analysis Aspect ratio (for same S)
Effect of Aspect Ratio
0
0.5
1
1.5
2
2.5
3
3.5
0 5 10 15 20 25 30 35 40
Lateral Strain, %
Max
. Str
ess/
GS
S= 4 AR= 2
S= 4 AR= 5
S= 2 AR= 2
S= 2 AR= 11
Larger AR gives slightly higher strains.
Difference is quite small
Comparison with Theory. Plain pad
W
L
t
LRBcKPEPc EfE ,,
fK ≈ 0.75m Use mave = 0.44. Then fK ≈ 0.33 Stiffness of a plain pad should be expected to be about 1/3
of that of a reinforced bearing with the same S. However,
this does not include creep deflections.
Plain pads:
Compression Stiffness Factor
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.2 0.4 0.6 0.8 1
m
f K
S = 2
S = 3
S = 4
S = 6
S = 8
approx
Tentative Design Criteria.
• Design plain pads using criteria similar to
those for steel-reinforced bearings, but
with lower values.
• No long-term damage to pads occurred,
so difficult to link design criteria to
potential damage.
• Consider a limiting compression strain,
and generate a stress criterion from it.
Tentative Design Criteria. Example:
• If strain limited to 10%, s < 0.6GS
Effect of Shape Factor
0
0.5
1
1.5
2
2.5
3
3.5
0 5 10 15 20 25 30 35
Lateral Strain, %
Max
Str
ess/
GS
S= 8 AR= 2
S= 4 AR= 2
S= 2 AR= 2
Governed here by bearings with S = 8.
Outcomes for Users.
• Plain pad strips under rectangular box
beams: make pad wider.
• Leveling pad (e.g. MNDOT): present pads
are at ≈ 800 psi (would need S = 16, thus
¼” thick pad). Potential problems unless
stiffer material used (70 durometer?).
• Use under prestressed girders. Problems
similar to leveling pads.
• Others?
Preliminary Conclusions
• Additional strain due to creep and cyclic
load is significant, controls behavior.
• Present AASHTO LRFD stress of 800 psi
is much too high.
• Stress limit should be related to S.
• Before recommending changes to
AASHTO LRFD Spec, need to check other
conditions (e.g. higher durometer pads).