Fundamentals of Dynamic Driven Pile Analysis

© 2013, Pile Dynamics, Inc. - Frank Rausche, Ph.D., P.E.

1 GRLWEAP Fundamentals CONTENT • Introduction • Why, when and where wave equation • Wave Equation Models: Hammer, Pile, • An Example • Summary

2 GRLWEAP Fundamentals GRLWEAP Application • WHEN? – Before pile driving begins, based on estimates – After initial pile tests using test results (refined WE) • WHY? – Formulate driving criterion (for required capacity) – Equipment (hammer and driving system) selection – Pile size/impedance selection – and blow count calculation (driveability) – Capacity determination

3 GRLWEAP Fundamentals GRLWEAP Application: During Design

Get Factored Loads

Qft = Σ(fi Qi) Do Borings Perform required initial tests Decide Pile Type Ru Verification No and Resistance Satisfactory? Factor, φ No

Dynamic Required R = n Analysis:Driveable (1/φ) Q Establish Driving Criterion ft Pile? Do Static Analysis Drive Production Piles to Find Pile Length Blow Count Test as many as required

4 GRLWEAP Fundamentals Wave Equation Application: Capacity Determination by Bearing Graph GRL Engineers, Inc. 08-Aug-2012 GRLWEAP Example GRLWEAP Version 2010

20 20 DELMAG D 30-32 Ram Weight 29.37 kN 16 16 Efficiency 0.800 Pressure 9645 (99%) kPa Helmet Weight 17.79 kN 12 12 Hammer Cushion 19259 kN/mm Pile Cushion 1009 kN/mm COR of P.C. 0.500 8 8

Skin Quake 2.500 mm TensionStress (MPa)

CompressiveStress (MPa) Toe Quake 10.160 mm 4 4 Skin Damping 0.650 sec/m Toe Damping 0.500 sec/m Pile Length 20.50 m 0 0 Pile Penetration 14.01 m Pile Top Area 3716.12 cm2 4000 5 Skin Pile Model Distribution 3200 4

2400 3 Stroke(m)

1600 2 UltimateCapacity (kN)

800 1

0 0 0 60 120 180 240 300 360 Res. Shaft = 71 % Blow Count (blows/.30m) (Proportional)

5 GRLWEAP Fundamentals GRLWEAP Application: Driveability Check

Blow Count < Acceptable

Stresses < Acceptable

6 GRLWEAP Fundamentals Dynamic Formulas

1893 Wellington (Engineering News) Now: Modified Gates

Energy Dissipated in Soil = Energy Provided by Hammer

(RUC)(Pile Set) = (Hammer Efficiency) (Wr h)

7 GRLWEAP Fundamentals ENR and Gates for D 19-42

Er = 42 kip-ft = 57 kN-m

4000

3500

3000

2500

2000

1500 Capacity in kN Capacityin 1000

500

0 0 25 50 75 100 125 150 175 200 Blows/0.25 m

Gates - w/ calculated Stroke ENR - Ru = Rd x 2

8 GRLWEAP Fundamentals Shortcomings of Formulas

• Rigid pile model • Poor hammer representation • Inherently inaccurate for both capacity and blow count predictions • No stress results • Unknown hammer energy • Relies on EOD Blow Counts

9 GRLWEAP Fundamentals The 1-D Wave Equation ρ(δ2u/ δt2) = E (δ2u/ δx2) E … elastic modulus f ρ … mass density

with c2 = E/ ρ ... Wave Speed Solution: u = f(x-ct) + g(x+ct)

g x x … length coordinate t ... time u … displacement

10 GRLWEAP Fundamentals THE WAVE EQUATION MODEL

• The Wave Equation Analysis calculates the displacement of any point of a slender elastic rod at any time using a difference method. • The calculation is based on rod – Length – Cross Sectional Area – Elastic Modulus – Mass density

11 GRLWEAP Fundamentals

GRLWEAP Fundamentals Hammer • For a pile driving analysis, the D.S. “slender, elastic rod” consists of Hammer+Driving System+Pile

• The soil is represented by resistance forces acting on the pile and Pile representing the forces in the pile-soil interface

12 GRLWEAP Fundamentals The Pile Model To solve the wave equation numerically:

• The hammer-pile system is divided into ∆L segments (masses and springs) – of length ∆L typically: ∆L ≤ 1 m (3.3 ft) – with mass m = ρ A ∆L – and stiffness k = E A / ∆L – there are N = L / ∆L pile segments

13 GRLWEAP Fundamentals We can model 3 hammer-pile systems

14 GRLWEAP Fundamentals External Combustion Hammer Modeling

Cylinder and upper frame = assembly top mass

Ram guides for assembly stiffness Drop height

Ram: A, L for stiffness, mass

Hammer base = assembly bottom mass

15 GRLWEAP Fundamentals External Combustion Hammers Ram Model

Ram segments ~1m long

Combined Ram- H.Cushion Helmet mass

16 GRLWEAP Fundamentals External Combustion Hammers Combined Ram Assembly Model

Ram segments

Assembly segments

Combined Ram- H.Cushion Helmet mass 17 GRLWEAP Fundamentals External Combustion Hammer Analysis Procedure • Static equilibrium analysis • Dynamic analysis starts when ram is within 1 ms of impact. • All ram segments then have velocity 1/2 VRAM = (2 g h η) – 0.001 g

g is the gravitational acceleration h is the equivalent hammer stroke and η is the hammer efficiency h = Hammer potential energy/ Ram weight

18 GRLWEAP Fundamentals External Combustion Hammer Analysis Procedure

• Dynamic analysis ends when

– Pile toe has rebounded to 80% of max dtoe – Pile has penetrated more than 4 inches

– Pile toe has rebounded to 98% of max dtoe and energy in pile is essentially dissipated

19 GRLWEAP Fundamentals

Diesel Hammers

Open Ended Open Closed Ended Closed

20 GRLWEAP Fundamentals Diesel Hammer Components

Piston = Ram

Cylinder

Fuel Port (closed by piston) pump Compressive stroke Combustion chamber

Impact block Hammer Cushion; Helmet

21 GRLWEAP Fundamentals Diesel Hammer Model

Ram segments ~1m long

Ram bottom/impact block Impact Block mass Hammer Cushion Helmet mass

22 GRLWEAP Fundamentals Diesel Hammer Combustion Pressure Model

• Compressive Stroke, hC

• Cylinder Area, ACH

• Final Chamber Volume, VCH

• Max. Pressure, pMAX Ports Precompression- h Combustion- C Expansion- Pressure

23 GRLWEAP Fundamentals DIESEL PRESSURE MODEL Liquid Injection Hammers

Liquid Injection Timing Parameters: Pressure Combustion Delay, ∆t

Combustion Duration, tD

Expansion:

1.25 Port p=pMAX(VCH/V) Open tD ∆t Compression:

1.35 p=patm(Vin/V) pMAX Time

24 GRLWEAP Fundamentals Energy, Efficiency and Measurements Potential (Rated)  Kinetic  Transferred

25 GRLWEAP Fundamentals WR Measured Transferred Energy

Max ET = ∫F(t) v(t) dt h (EMX, ENTHRU) WR

ηT = ENTHRU/ ER (transfer ratio or efficiency) Measure

ER = WR h Force, F(t) Manufacturer’s Rating Velocity, v(t)

26 GRLWEAP Fundamentals Measured Transfer Ratios for Diesels Steel Piles Concrete Piles

27 GRLWEAP Fundamentals SA Air Hammers – SA Hydraulic Hammers on Steel Piles

28 GRLWEAP Fundamentals GRLWEAP

Impact Hammer Efficiencies , ηh Diesel hammers: 0.80 Traditional air/steam hammers: 0.67 Hydraulic hammers: 0.80 Hammers with energy monitoring: 0.95

These efficiencies account for energy losses that we cannot calculate or otherwise assess!

29 GRLWEAP Fundamentals Vibratory Hammers

30 GRLWEAP Fundamentals Vibratory Hammer Model

• Line Force FL

• Bias Mass and m1

• Oscillator mass, m2

• Eccentric masses, me, m2 FV radii, re • Clamp Vibratory Force: 2 FV = me [ω resin ω t - a2(t)]

31 GRLWEAP Fundamentals Driving System Models

The Driving Systems Consists of 1. Helmet including inserts to align hammer and pile 2. Optionally: Hammer Cushion to protect hammer 3. For Concrete Piles: Softwood Cushion

32 GRLWEAP Fundamentals Driving System Model Example of a diesel hammer on a concrete pile

Hammer Cushion: Spring plus Dashpot Helmet + Inserts Pile Cushion + Pile Top: Spring + Dashpot

Pile Top Mass

33 GRLWEAP Fundamentals The Soil Model After Smith

Outer Soil: Interface Soil: Rigid Elasto-Plastic Springs and Viscous Dashpots

34 GRLWEAP Fundamentals Soil Resistance • Soil resistance slows pile movement and causes pile rebound • A very slowly moving pile only encounters static resistance • A rapidly moving pile also encounters dynamic resistance • The static resistance to driving differs from the soil resistance under static loads

35 GRLWEAP Fundamentals Smith’s Soil Model Total Soil Resistance

Rtotal = Rsi +Rdi

R function of u Segment si i function of v i Rdi i

Fixed Displacemt ui Velocity vi

37 GRLWEAP Fundamentals Static Shaft Resistance Pile Segment Model Parameters R , q ui i Elastic spring with max. Static Resistance compression q (quake) Rigid plastic slider Rui with Resistance Rui

ksi = Rui /qi Fixed reference

quake, qi Pile Displacement 38 GRLWEAP Fundamentals Shaft Resistance and Quake Static Resistance

-Rui Rui qi

Recommended

qi Shaft Quakes: 2.5 mm or 0.1 inches Pile Displacement

39 GRLWEAP Fundamentals The Static Toe Resistance and Quake Static Toe Resistance

Rui qi For impact hammers

For vibratory hammers qi

Toe Displacement

40 GRLWEAP Fundamentals Recommended Toe Quakes, qt Static Toe Res. Non-displacement Displacement piles R piles qt ut 0.1” or 2.5 mm D/120: very dense/hard 0.04” or 1 mm on hard rock D/60: softer/loose soils qt

Toe Displacement

D

41 GRLWEAP Fundamentals Smith’s Soil Damping Model (Shaft or Toe)

Rd = RsJs v Fixed Pile Smith damping factor, reference J [s/m or s/ft] Segment (soil around s pile) Rd = RuJsv v Smith-viscous damping

factor Jsv [s/m or s/ft] velocity v For RSA and Vibratory Ananlysis

dashpot

42 GRLWEAP Fundamentals Recommended Smith damping factors

Shaft : 0.65 s/m or 0.20 s/ft : 0.16 s/m or 0.05 s/ft : use an intermediate value Layered soils: use a weighted average for bearing graph Toe All soils: 0.50 s/m or 0.15 s/ft

43 GRLWEAP Fundamentals Resistance Distribution

1. Simplest I. Percentage Shaft resistance (from static soils analysis) II. Triangular or Rectangular or Trapezoidal Only reasonable for a simple

Bearing Graph where little is Penetration known about soil. End Bearing = Total Capacity x (100% - Percent Shaft Resistance)

44 GRLWEAP Fundamentals Resistance Distribution

2. Still Simple: ST Analysis based on some knowledge of Soil Types

Reasonable for a simple Bearing Graph; for Driveability possible, but more accurate analysis should be done. Penetration

End Bearing = From Soil Type, Pile Bottom Area

45 GRLWEAP Fundamentals Resistance Distribution 3. More Involved: I. SA Input: SPT Blow Count, Friction

Angle or Unconfined Compressive Strength II. API (offshore wave version) Input: Friction Angle or Undrained

III. CPT Penetration Input: Cone Record including Tip Resistance and Sleeve Friction vs Depth.

All are good for a Bearing Graph May be OK for Driveability Analysis Local experience may provide better values

46 GRLWEAP Fundamentals Numerical Treatment • Predict displacements:

uni = uoi + voi ∆t uni-1 Mass i-1 R • Calculate spring compression: i-1

ci = uni - uni-1 Fi, ci

• Calculate spring forces: uni Mass i Ri

Fi = ki ci

• Calculate resistance forces: uni+1 Mass i+1 Ri+1 Ri = Rsi + Rdi

47 GRLWEAP Fundamentals Force balance at a segment

Force from upper spring, Fi

Resistance force, Ri Mass i Weight, Wi

Force from lower spring, Fi+1

Acceleration: ai = (Fi + Wi – Ri – Fi+1) / mi

Velocity, vi, and Displacement, ui, from Integration

48 GRLWEAP Fundamentals Set or Blow Count Calculation (a) Simplified: extrapolated toe displacement Static soil Resistance

Max. Displacement

Calculated

Extrapolated Ru

Pile Displacement

Final Set Quake

49 GRLWEAP Fundamentals (b) Blow Count Calculation by RSA

• Residual Stress Analysis is also called Multiple Blow Analysis • Analyzes several blows consecutively with initial stresses, displacements from static state at end of previous blow • Yields residual stresses in pile at end of blow; generally lower blow counts

50 GRLWEAP Fundamentals Blow Count Calculation (b) Residual Stress Analysis (RSA)

Set for 2 Blows

Convergence: Consecutive Blows have same pile compression/sets

51 GRLWEAP Fundamentals RSA: When and How • RSA is the preferable method of analysis for long slender piles (e.g., steel piles with Lp/D > 100 or Monotube/Taper Tube piles) • RSA calculates somewhat higher blow counts than standard analysis (non- conservative) • RSA calculates somewhat higher stresses than standard analysis (conservative)

52 GRLWEAP Fundamentals Program Flow – Bearing Graph

Input Distribute Ru Increase Ru Set Soil Constants

Model hammer, Static Equilibrium

driving system Ram velocity

and pile Dynamic analysis Y Increase

Ru? • Pile stresses • Energy transfer Choose first Ru • Pile velocities N

Calculate Blow Count Output

53 GRLWEAP Fundamentals Bearing Graph: Variable Capacity, One depth SI-Units; Clay and Sand Example; D19-42; HP 12x53;

54 GRLWEAP Fundamentals The Inspectors’ Chart: One Capacity and One Depth – Stroke Variable GRL Engineers, Inc. 21-Aug-2011 Demo 3-Inspector's Chart - D16-32 GRLWEAP Version 2010

250 250 DELMAG D 16-32 Capacity 1600.0 kN Ram Weight 15.66 kN 200 200 Efficiency 0.800 Pressure 9825 (99%) kPa Helmet Weight 8.45 kN 150 150 Hammer Cushion 10535 kN/mm COR of H.C. 0.800 Skin Quake 2.500 mm Toe Quake 2.500 mm 100 100 TensionStress (MPa) Skin Damping 0.259 sec/m

CompressiveStress (MPa) Toe Damping 0.500 sec/m Pile Length 18.28 m 50 50 Pile Penetration 16.76 m Pile Top Area 140.64 cm2

Skin Friction 0 0 Pile Model Distribution

3.50

3.10

2.70 Stroke(m)

2.30

1.90

1.50 40 80 120 160 200 240 280 Res. Shaft = 30 % Blow Count (blows/.25m) (Proportional)

55 GRLWEAP Fundamentals Formulas and Wave Equation D19-42; HP 12x53; Clay and Sand

4000

3500

3000

2500

2000

1500 Capacity in Capacity kN 1000

500

0 0 25 50 75 100 125 150 175 200 Blow s/0.25 m

Gates ENR GRLWEAP-Clay GRLWEAP-Sand

56 GRLWEAP Fundamentals Driveability Analysis

Basically: • Perform a static soil analysis – do it as accurately as possible • Perform wave equation analyses for

different depths with Ru from static soil analysis

• Plot calculated Ru, blow count, maximum stresses vs. depth

57 GRLWEAP Fundamentals Driveability Analysis

• Analyze a series of Bearing Graphs for different depths for SRD and/or LTSR • Put the results in sequence so that we get predicted blow count and stresses vs pile toe penetration • Note that, in many or most cases, shaft resistance is lower during driving (soil setup) and end bearing is about the same as long term • In the few cases of relaxation, the toe resistance is actually higher during driving than long term

58 GRLWEAP Fundamentals Program Flow – Driveability

Input Calculate Ru for first gain/loss Model Hammer & Next G/L Driving System Analysis

Choose first Depth to analyze Increase Y G/L?

Pile Length and N

Model Y Increase Output Depth? Increase Depth N

59 GRLWEAP Fundamentals Driveability Result

60 GRLWEAP Fundamentals Remarks About SRD

• WHAT IS RU DURING DRIVING? We call it SRD, because we lose static shaft resistance during driving. • In general, we will regain static resistance by Soil Setup - primarily along shaft (maybe up to 10x in clay) • During analysis we may want to analyze with full loss of setup or with partial loss of setup or with no loss of setup at all.

61 GRLWEAP Fundamentals For Driveability with variable setup time

• Setup time Setup Time Defines after how Ru much waiting time setup is gained Ru/SF

Time Ru Limit • Limit Distance Distance Defines after how Ru/SF much driving distance soil setup is lost Pile Penetration

62 GRLWEAP Fundamentals Summary • The wave equation helps for equipment selection, setting preliminary driving criteria and capacity determination, if testing is not feasible. • For capacity determination without measurements the factor of safety has to be greater than when doing measurements (GIGO).

63 GRLWEAP Fundamentals Summary • The wave equation analysis simulates what happens in the pile due to a hammer impact. • It calculates a relationship between capacity and blow count, or blow count vs. depth. • The analysis model represents hammer (3 types), driving system (cushions, helmet), pile (concrete, steel, timber) and soil (at the pile-soil interface) • GRLWEAP provides a variety of input help features (hammer and driving system data, static formulas among others).

64 GRLWEAP Fundamentals Summary

• Good hammer performance is essential for both good productivity and a meaningful construction control by blow count. • Wave Equation analysis results are only as good as the accuracy of the hammer efficiency and soil resistance input.

65 GRLWEAP Fundamentals Thank you for your attention For further information see: www.pile.com

QUESTIONS?

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66 GRLWEAP Fundamentals