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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Dynamic Earth pressure - Myths, Realities and Practical Ways for Design
Carlos Coronado and Javeed Munshi
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Presentation Outline
Introduction and Background
Standard Practice
Simplified Determination of Lateral Earth Pressures
Hydrodynamic Fluid Pressures
Review of Lateral Soil Pressure Theories
Recent Experimental Results
Detailed Seismic Fluid Soil Structure Interaction
Detailed fluid-structure interaction
Simplified fluid modeling
Seismic soil structure interaction
Case Study Intake Pump Station
Introduction and Background
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Force Diagram of Subsurface Walls - Static Conditions
ground surface
groundwater
Applicable loads
at-rest earth pressure
surcharge stress from surface loading
compaction stresses from Duncan's method (1991 and 1993)
U = buoyancy due to water table
N = normal stress along basemat
N = W - U
STATIC
Building Weight, W
at-restat-rest
surchargesurcharge
compaction compaction
surcharge, w
waterwater Hydrostatic
Uplift, U
K0g'HK0w
gwHw
HHw
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Force Diagram of Subsurface Walls – Seismic Without Movement
ground surface
groundwater
Base Friction = m N , where N = W - U - V
+ Base adhesion
Applicable loads
at-rest earth pressure
surcharge stress from surface loading
compaction stresses from Duncan's method (1991 and 1993)
U = buoyancy due to water table
V = vertical seismic force
N = normal stress along basemat
base friction using interface coefficient, m
traction = friction along building sides = at-rest pressure x msides
msides = friction coefficient along sidewalls of structure
seismic increment = horizontal base forces from SASSI output include all driving forces,
composed of those from seismic, at-rest, and building inertia
Sliding check Compare SASSI basemat horizontal forces (Demand = D)
against basemat frictional/adhesional resistance (Capacity = C).
If FS = C/D 1.1, then building is stable against sliding
SEISMIC - NO MOVEMENT
Building Weight, W
at-restat-rest
surchargesurcharge
compaction compaction
surcharge, w
waterwater
Hydrostatic
Uplift, U
seismic increment
traction
(front and
back walls)
K0g'HK0w
gwHw
H
Hw
Building inertia
Vertical
Seismic, V
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Force Diagram of Subsurface Walls – Seismic With Movement
ground surface
groundwater
Base Friction = m N (m reduced 25%)
where N = W - U - V
+ Base adhesion
Applicable loads
resisting earth pressure is dependent on amount of movement
surcharge stress from surface loading
U = buoyancy due to water table
V = vertical seismic force
N = normal stress along basematreduced base friction using interface coefficient, mred
reduced traction = friction along building sides = at-rest pressure x msides_red
msides_red = reduced friction coefficient along sidewalls of structure
seismic increment = horizontal base forces from SASSI output include all driving forces,
composed of those from seismic, at-rest, and building inertia
Sliding check Compare SASSI basemat horizontal driving forces (Demand = D)
against basemat friction/adhesion + side friction + passive resistance (Capacity = C)
using reduced resistance coefficients for frictional/adhesional components
If FS = C/D 1.1, then building is stable against further sliding
SEISMIC - WITH MOVEMENT
Building Weight, W
active
surcharge, w
Building inertia
K = at-rest
increasing to
passive with
movement
seismic
increment
Hydrostatic
Uplift, U
Kag'H
H
Hw
Kg'H
traction
(front and
back walls)
Vertical
Seismic, V
Standard Practice for Partially or FullyBuried Liquid-containing Structures
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Total Base Shear and Wall Pressures
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Practical Earth Pressure Analysis
Select all potential critical interface combinations at the base and sides of the structure on which to determine the minimum base frictional resistance.
Compare base and side frictional resistance to seismic at-rest demand. If C/D > 1.0, then use seismic at-rest demand to design walls.
If the C/D < FS, then sliding will occur. Then reduce base and side friction coefficients by 25%. loading side of the structure will be subject to the active earth pressure, the seismic lateral active earth pressure increment, and the building inertia. Increase resisting load on the passive side, until C/D ≥ 1.0.
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Sliding or wall rotation must occur for K < K0
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Hydrodynamic Pressures (ACI 350)
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Seismic Active and At-Rest Lateral Earth Pressure
𝐾𝐴𝐸 =𝑐𝑜𝑠2(𝜙 − 𝜃 − 𝛽)
cos𝜃 cos2𝜷cos(𝛽 + 𝜃 + 𝛿) 1 +sin 𝜙 + 𝛿 sin(𝜙 − 𝜃 − 𝑖)cos(𝛽 + 𝜃 + 𝛿) ∗ cos(𝑖 − 𝛽)
𝟐 𝜽 = tan−1𝑘ℎ
1 − 𝑘𝑣
PAE = 0.5gH2(KA+DKAE) pAD = DKAE·g·(H-z) p0D = 2DKAE·g·(H-z)
NCHRP 611
DKAE~0.75kh
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Dynamic Soil Pressures ASCE 4-98 (Wood 1973)
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Soil Pressures Sample Calculation
EL 0’
EL -5’
EL -20’
= 320
g = 120 pcf
Kh = 0.25
249 (498) psf
147 (294) psf
0 psf
0 psf
186 (300) psf
454 (732) psf 936 psf 1390 (1668) psf
249 (498) psf
333 (594) psf
0’
-5’
-20’
Static Earth Pressure Seismic Earth Pressure Hydrostatic Pressure Total Pressure
H = 20 ft.
q = tan-1(0.25) = 14o
KAE = = 0.48
KA = 0.31
DKAE = 0.48-0.31 = 0.17
DKAE ~ 3/4·0.25 = 0.1875, use 0.17
gmoist = 120 pcf
gsub = 120-62.4 = 57.6 pcf
K0S = 1-sin(32o) = 0.47, use K0S = 0.5
DK0E = 2DKAE = 2·0.17 = 0.34
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Ground Water Considerations
if the backfill is well drained, seismic ground water pressures need not be considered. In this case, only hydrostatic pressures are taken into consideration:
pW = gWz
Whitman, RV (1990) suggests that the seismic ground water thrust exceeds 35% of the hydrostatic thrust for kh>0.3g.
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Influence of Wall Movement on Intensity of Earth Pressures in Cohesionless Materials
ground surface
groundwater
Base Friction = m N (m reduced 25%)
where N = W - U - V
+ Base adhesion
Applicable loads
resisting earth pressure is dependent on amount of movement
surcharge stress from surface loading
U = buoyancy due to water table
V = vertical seismic force
N = normal stress along basematreduced base friction using interface coefficient, mred
reduced traction = friction along building sides = at-rest pressure x msides_red
msides_red = reduced friction coefficient along sidewalls of structure
seismic increment = horizontal base forces from SASSI output include all driving forces,
composed of those from seismic, at-rest, and building inertia
Sliding check Compare SASSI basemat horizontal driving forces (Demand = D)
against basemat friction/adhesion + side friction + passive resistance (Capacity = C)
using reduced resistance coefficients for frictional/adhesional components
If FS = C/D 1.1, then building is stable against further sliding
SEISMIC - WITH MOVEMENT
Building Weight, W
active
surcharge, w
Building inertia
K = at-rest
increasing to
passive with
movement
seismic
increment
Hydrostatic
Uplift, U
Kag'H
H
Hw
Kg'H
traction
(front and
back walls)
Vertical
Seismic, V
ground surface
groundwater
Base Friction = m N , where N = W - U - V
+ Base adhesion
Applicable loads
at-rest earth pressure
surcharge stress from surface loading
compaction stresses from Duncan's method (1991 and 1993)
U = buoyancy due to water table
V = vertical seismic force
N = normal stress along basemat
base friction using interface coefficient, m
traction = friction along building sides = at-rest pressure x msides
msides = friction coefficient along sidewalls of structure
seismic increment = horizontal base forces from SASSI output include all driving forces,
composed of those from seismic, at-rest, and building inertia
Sliding check Compare SASSI basemat horizontal forces (Demand = D)
against basemat frictional/adhesional resistance (Capacity = C).
If FS = C/D 1.1, then building is stable against sliding
SEISMIC - NO MOVEMENT
Building Weight, W
at-restat-rest
surchargesurcharge
compaction compaction
surcharge, w
waterwater
Hydrostatic
Uplift, U
seismic increment
traction
(front and
back walls)
K0g'HK0w
gwHw
H
Hw
Building inertia
Vertical
Seismic, V
Experimental Results
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Recent Experimental Studies (PEER 2007/06)
Stiff and flexible model structures configuration
Centrifuge model configuration
L. Atik and N. Sitar (2007)
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Representative Experimental Results
L. Atik and N. Sitar (2007)
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Maximum total dynamic pressure distributions measured and estimated
L. Atik and N. Sitar (2007)
Detailed Seismic Fluid Soil Structure Interaction
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Fluid Structure Interaction
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Seismic Soil Structure Interaction
(SASSI2010 Theory Manual)
Substructuring in the Flexible Volume Method Substructuring in the Substructure Subtraction Method
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Case Study: Intake Pump Station
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Structure Geometry
EL. +0'-0" (Maximum
Operating Level in Forebay)
EL. (-) 22'-6"
EL. + 26'-6"EL. + 11'-6"
(Operating Deck)
EL. + 11'-6"
(Operating Deck)EL. + 10'-0" EL. + 10'-6"
EL. (-) 5'-6"
Circulating Water
Intake StructureForebay Structure
UHS Intake Structure
UHS Electrical
Building
EL. (-) 10'-0" EL. (-) 10'-0"EL. (-) 11'-0" EL. (-) 8'-0"
EL. + 3'-0" (GWT)
Pump house Enclosure
3'-0" 3'-0"
5'-0"
Baffle Wall
Slanting/
Skimmer Wall
Slanting/
Skimmer Wall
Baffle
Wall
5'-0"
2'-0"
Bar Screens
Y
X
2'-0"
Expansion
Joint
EL. + 20'-6"
Traveling Screen
Enclosure
Pump Room
Staircase
Enclosure
80
'-0
" (c
lea
r
dim
en
sio
n)
100'-0" (clear
dimension) 59'-0" 33'-0"
36
'-6
"
60
'-0
"
74
'-0
"
CWS Makeup Water
Intake Structure Forebay Structure UHS Makeup Water
Intake Structure
UHS Electrical
Building
CCNPP
Unit 3
NORTH
18
'-6
"
105'-11" (including
slab on grade portion)
26'-6"
Pump House
Enclosure
Electrical
Room Slab
Pump House Enclosure
Slab on grade
X
Z
Expansion
Joint
7'-0"
60" dia.
Intake Pipe (TYP)
Debris Basin
Slab
Debris Basin
Slab
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Overall Analysis/Design Approach
The finite element model of the structures is developed using GT STRUDL Version 29.1.
Lumped Mass is used to model the Hydrodynamic Load.
The SSI analysis is performed using Site-Specific Input Ground Motion and three soil cases (UB, BE and LB).
The FE model used for the SSI analysis is modified to obtain the static response of the structure, using GT STRUDL.
Only critical panels are designed. Microsoft Excel Workbook is used to combine element forces and moments from static and SSI analyses, for these critical panels.
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Finite Element Model, Showing Critical Panels
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Hydrodynamic loads
(a) Actual distribution (b) Idealized distribution
CCNPP Unit 3 NORTH
20
8,
14
54
20
8, 1
45
4
20
8,
14
54
20
8, 1
45
4
207, 1449
207, 1449
Equivalent weights of accelerating liquid
Wi.ew
tanh 0.866
Lew
HL
0.866
Lew
HL
WL
Impulsive Weight Distributions
Wiy.ew y( )
Wi.ew
2
4HL 6 hi.ew 6 HL 12 hi.ew y
HL
HL2
Height to centers of gravity EBP
hi.ew 0.5 0.09375
Lew
HL
HL
Lew
HL
1.333if
0.375( ) HL otherwise
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Comparison of Acceleration Transfer Functions
EQz
EQy
EQx
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
SSI Model
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Sample Results
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Design of Walls and Slabs
a. Design for In-plane shear using full section cuts.
b. Design vertical and horizontal sections for out-of-plane moments and axial forces using a P-M interaction analysis.
c. Conservatively add the reinforcement from steps a and b
d. Check out-of-plane shear for the whole wall, or whole segments on either side of openings, based on average shear.
e. Check for punching shear where required.
Forces and moments computed after combination of seismic and static results are used for the design of each critical panel, using a Microsoft Excel Workbook, as outlined next and described in detail later.
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Design of Walls and Slabs
Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012
Conclusions
Simplified and detailed approached for the dynamic analysis of embedded liquid containing structures where presented. Conclusions and recommendations are as follows:
Additional guidelines are required for the calculations of dynamic earth pressures. In particular regarding the use of active or at rest dynamic soil pressures.
Detailed soil structure interaction analyses can provide additional inside regarding the behavior of embedded liquid containing structures. However they are only warranted for critical structures.
Thank You!