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Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC DAN BROW N ASSOCIATES AND 43 rd Annual Midwest Geotechnical Conference October 1 – October 3, 2014 Bloomington, Minnesota
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Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Dec 16, 2015

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Page 1: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Designing Piles for Drag Force

Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC

DANBROWNASSOCIATESAND

43rd Annual Midwest Geotechnical ConferenceOctober 1 – October 3, 2014Bloomington, Minnesota

Page 2: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Aspects of Axial Resistance of Piles

Neutral Plane Concepts

Example of Drag Force on Vertical Pile

Downdrag on Batter

Page 3: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Aspects of Axial Resistance of Piles

Page 4: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

AXIAL RESISTANCE OF PILES

The axial resistance of deep foundations may be divided into two components:

Qnominal compression

Rtip

1. Side resistance (unit value is fside )

2. Tip resistance

@ nominal compression (i.e., FOS = 1) the entire side resistance is positive/upward

Negative skin friction doesn’t exist at the geotechnical strength limit state.

It is unrealistic to represent drag force as a top load for strength limit analysis.

S Area x fside = Rside

Page 5: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

FUNDAMENTALS OF SIDE RESISTANCE

1. The shear is confined to a thin zone around the pile and drainage can take place. Therefore, the side resistance is frictional.

Burland, J.B. (1973) “Shaft friction in Piles in Clay – A Simple Fundamental Approach” Ground Engineering, 6(3), 30-42.

Meyerhoff, G.G. (1976) “Bearing Capacity and Settlement of Pile Foundations” Journal of the Geotechnical Engineering Division, American Society of Civil Engineers, 102, 195-228.

Page 6: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

FUNDAMENTALS OF SIDE RESISTANCE

2. The direction of the (frictional) side resistance is always to resist the tendency for movement.

Friction Friction

Block Block

Page 7: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

FUNDAMENTALS OF SIDE RESISTANCE

3. The side resistance is fully mobilized at very small relative movements between the pile and soil.

Hanna, T.H. and Tan, R.H.S. (1973) “The behavior of long piles under compressive loads in sand” Canadian Geotechnical Journal, 10(3), 311-340.

less than 1 mm

Page 8: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Neutral Plane Concepts

Fellenius, B.H. (1989) “Unified design of piles and pile groups”, Transportation Research Board, Washington, TRB Record, 1169, 75-82.

Fellenius, B.H. (1998) “Recent advances in the design of piles for axial loads, drag loads, downdrag, and settlement” Proceedings, Seminar by ASCE and Ports of New York and New Jersey, 19p.

Page 9: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEGATIVE SKIN FRICTION

…..is side resistance mobilized as the ground moves downward relative to the pile.

The magnitude of ground settlement is irrelevant to the development of drag force. Essentially all piles will move relative to the soil as a result of differences in compressibility.*

* Fellenius, B.H. Brusey, W.G., and Pepe, F. (2000) “Soil setup, variable concrete modulus and residual load”, ASCE Proceedings, Specialty Conference on Performance Confirmation of Constructed Facilities, 16 p.

Page 10: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

DRAG FORCE

…..is the axial compressive force induced in a pile due to accumulated negative skin friction.

Qpermanent

Page 11: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE

…..is the location along the pile where there is no relative movement between the pile and adjacent soil.

The side resistance is negative above the neutral plane.

The side resistance is positive below the neutral plane.

It is the location of the maximum axial compressive stress.

Page 12: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

DOWNDRAG

….. is the downward movement of the pile (Spile) resulting from ground settlement.

Page 13: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

PERMANENT (OR SUSTAINED) LOADS

….. are constant over time (weight).

Page 14: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

TRANSIENT LOADS

….. act only a short time (e.g., wind, seismic, traffic).

Page 15: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE MODEL

Profile of Ground Settlement

Qpermanent

Arr

ow

s in

dic

ate

dir

ect

ion o

f si

de r

esi

stance

Rtip

NeutralPlane

0 Smax

Spile

Pile moves downward relative to soil

Soil moves downward relative to pile

Page 16: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE MODEL

Profile of Ground Settlement

0 Smax

Qpermanent Axial Compressive Load in Pile

0 Rtip

Qpermanent

Drag Force Neutral

PlaneA

rrow

s in

dic

ate

dir

ect

ion o

f si

de r

esi

stance

Spile

Rtip

Posit

ive

Side

Resis

tanc

e

Negative Skin

Friction

Page 17: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE METHOD IN DESIGNImportant -

Ideally, the neutral plane should be determined using the actual, unfactored permanent load.

Page 18: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE METHOD IN DESIGNImportant -

Ideally, the neutral plane should be determined using the actual, unfactored permanent load.

The neutral plane should be determined using unfactored side/mobilized tip resistances.

Page 19: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE METHOD IN DESIGNImportant -

Ideally, the neutral plane should be determined using the actual, unfactored permanent load.

The neutral plane should be determined using unfactored side/mobilized tip resistances.

The mobilized tip resistance is unknown and must be assumed. Tip resistance versus displacement curves (or t-z curves) may be used in a more refined iterative approach.

Page 20: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

NEUTRAL PLANE METHOD IN DESIGN

Important -

Drag force is not considered when evaluating the geotechnical strength limit state. It is considered in settlement at the geotechnical service limit state and in the structural limit state.

Page 21: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

EXAMPLE

New approach fill

Compressible soil

Piles are sleeved through fill

We want to know the effect of the new approach fill on the existing piles.

Page 22: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

EXAMPLE

This diagram shows that the sustained load, drag force and mobilized resistances are in equilibrium.

Qpermanent

Page 23: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Pile top movement

Ground Settlement

Pile Movement = Ground Movement at Neutral Plane + Elastic Shortening

Penetration of Pile Tip

Neutral PlaneDepth

alo

ng p

ile

EXAMPLE

This diagram shows the ground settlement and pile movement….

and the fact that they are the same at the neutral plane.

Qpermanent

Page 24: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

What about the transient load?

Page 25: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Sustained LoadTransientLoad

Dep

th a

lon

g p

ile

Cumulative Positive Side Resistance Plus Mobilized Tip Resistance

Max. Force

Mobilized Tip Resistance

Sustained Load Plus Cumulative Negative Skin Friction

Neutral Plane

Resistance

Load

EXAMPLE

This diagram shows that for the case where the transient load is less than the drag force……….

the transient load temporarily “replaces” part of the drag force in the pile.

Qpermanent + Qtransient

Page 26: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Downdrag on Batter Piles

Takahashi, K. (1985) “Bending of A Batter Pile Due to Ground Settlement”, Soils and Foundations, Japanese Society of Soil Mechanics and Foundation Engineering, Vol.25, No.4, 75-91.

Sawaguchi, M. (1989) “Prediction of Bending Moment of a Batter Pile in Subsiding Ground”, Soils and Foundations, Japanese Society of Soil Mechanics and Foundation Engineering, Vol.29, No.4, 120-126.

Narasimha Rao, S., Murthy, T.V.B.S.S. and Veeresh, C. (1994) “Induced Bending Moments in Batter Piles in Settling Soils”, Soils and Foundations, Japanese Society of Soil Mechanics and Foundation Engineering, Vol.34, No.1, 127-133.

McGuire, M. and Filz (2012) Interim Guidance, Revised LPILE Method to Calculate Bending Moments in Batter Piles for T-Walls Subject to Downdrag, Contract Report W912P8-07-D-0062 for the Army Corps of Engineers.

Page 27: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

DOWNDRAG ON BATTER PILES

Batter pile

q

Ground surface

Profile of Ground Settlement

0 Smax

Ground movement perpendicular to pileS to pile = S*sin(q)

T

0 S to pile

T

Page 28: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

DOWNDRAG ON BATTER PILES

Input profile of ground movement perpendicular to pile into LPILE or GROUP

The curvature of the profile of ground movement ( ┴ to pile ) determines the moment distribution in the pile .

Page 29: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

Review of Main Points

Page 30: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The “Neutral Plane Method” is accepted by AASHTO; however, the details of its implementation are unclear.

Page 31: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The “Neutral Plane Method” is accepted by AASHTO; however, the details of its implementation are unclear.

• The neutral plane method provides a rational framework to consider negative skin friction, drag force, and downdrag (settlement).

Page 32: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The “Neutral Plane Method” is accepted by AASHTO; however, the details of its implementation are unclear.

• The neutral plane method provides a rational framework to consider negative skin friction, drag force, and downdrag (settlement).

• Negative skin friction does not exist at the geotechnical strength limit state – so it is not realistic to add drag force when determining the required nominal geotechnical resistance.

Page 33: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The “Neutral Plane Method” is accepted by AASHTO; however, the details of its implementation are unclear.

• The neutral plane method provides a rational framework to consider negative skin friction, drag force, and downdrag (settlement).

• Negative skin friction does not exist at the geotechnical strength limit state – so it is not realistic to add drag force when determining the required nominal geotechnical resistance.

• The location of the neutral plane may be where the maximum axial force and is appropriately used to determine the required nominal structural resistance of the deep foundation.

Page 34: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The “Neutral Plane Method” is accepted by AASHTO; however, the details of its implementation are unclear.

• The neutral plane method provides a rational framework to consider negative skin friction, drag force, and downdrag (settlement).

• Negative skin friction does not exist at the geotechnical strength limit state – so it is not realistic to add drag force when determining the required nominal geotechnical resistance.

• The location of the neutral plane may be where the maximum axial force and is appropriately used to determine the required nominal structural resistance of the deep foundation.

• The location of the neutral plane is where the ground and pile move together – and so settlement of the ground at the neutral plane is equal to the settlement of the pile.

Page 35: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The curvature of the profile of ground movement ( ┴ to pile ) determines the moment distribution in the pile.

Page 36: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

REVIEW

• The curvature of the profile of ground movement ( ┴ to pile ) determines the moment distribution in the pile.

• The resulting moment distribution usually will not control the pile design. A more critical situation occurs when the curvature of the settlement profile is very large.

Page 37: Designing Piles for Drag Force Timothy C. Siegel, P.E., G.E., D.GE with Dan Brown and Associates PC 43 rd Annual Midwest Geotechnical Conference October.

THANK YOU FOR YOUR ATTENTION

DANBROWNASSOCIATESAND

43rd Annual Midwest Geotechnical ConferenceOctober 1 – October 3, 2014Bloomington, Minnesota