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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

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Page 1: Dynamic Earth pressure - Myths, Realities and Practical … ·  · 2017-08-05Dynamic Earth pressure - Myths, Realities and Practical Ways for Design ... seismic lateral active earth

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

Page 2: Dynamic Earth pressure - Myths, Realities and Practical … ·  · 2017-08-05Dynamic Earth pressure - Myths, Realities and Practical Ways for Design ... seismic lateral active earth

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

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Introduction and Background

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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

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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

Page 6: Dynamic Earth pressure - Myths, Realities and Practical … ·  · 2017-08-05Dynamic Earth pressure - Myths, Realities and Practical Ways for Design ... seismic lateral active earth

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

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Standard Practice for Partially or FullyBuried Liquid-containing Structures

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Total Base Shear and Wall Pressures

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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.

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Sliding or wall rotation must occur for K < K0

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Hydrodynamic Pressures (ACI 350)

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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

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Dynamic Soil Pressures ASCE 4-98 (Wood 1973)

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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

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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.

Page 16: Dynamic Earth pressure - Myths, Realities and Practical … ·  · 2017-08-05Dynamic Earth pressure - Myths, Realities and Practical Ways for Design ... seismic lateral active earth

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

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Experimental Results

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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)

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Representative Experimental Results

L. Atik and N. Sitar (2007)

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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)

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Detailed Seismic Fluid Soil Structure Interaction

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Fluid Structure Interaction

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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

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Case Study: Intake Pump Station

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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

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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.

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Finite Element Model, Showing Critical Panels

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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

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Comparison of Acceleration Transfer Functions

EQz

EQy

EQx

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

SSI Model

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Sample Results

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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.

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Dynamic Earth pressures - Myths, Realities and Practical Ways for Design : October 2012

Design of Walls and Slabs

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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.

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Thank You!