PILE DRIVING BY WAVE MECHANICS - PowerPoint PPT Presentation

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PILE DRIVING BY WAVE MECHANICS

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Title: PILE DRIVING BY WAVE MECHANICS


1
PILE DRIVINGBYWAVE MECHANICS
  • George Goble
  • GOBLE PILE TEST

2
A STUPID QUESTION
  • WHAT MAKES A PILE PENETRATE?
  • A FORCE
  • IF WE PUSH SLOWLY BUT HARD ENOUGH IT WLL MOVE
    DOWN AGAINST THE SOIL RESISTANCE
  • THE MAGNITUDE OF THE PUSH WILL BE THE PILE
    CAPACITY (BUT HOW DO WE DEFINE CAPACITY)
  • BUT WHAT IF WE USE A VERY BRIEF PUSH THAT WILL
    PENETRATE THE PILE? PERHAPS AN IMPACT
  • THAT FORCE WILL BE LARGER THAN THE CAPACITY?
  • THERE IS A DYNAMIC RESISTANCE
  • WE WANT TO UNDERSTAND THE EFFECT OF AN IMPACT ON
    THE PILE IN ORDER TO DEAL WITH PROBLEMS LIKE THE
    ABOVE

3
WAVE PROPAGATION
Based on the assumption of linear elastic material
  1. If a force is suddenly applied to the end of a
    pile a wave (disturbance) is generated that
    travels along the pile. When the wave passes a
    point on the pile the point displaces with some
    velocity and acceleration. A force is present in
    the pile. The disturbance can be expressed as a
    wave of any of these quantities.
  2. A stress wave propagates unchanged in magnitude
    at a constant speed, c, in a uniform cross
    section pile.

4
SOME WAVE SPEEDS
  • Steel 16,800 feet/sec.
  • Almost 12,000 miles/hour
  • Concrete 11,000 to 14,000 feet/sec
  • Both Modulus and Density Vary so Wave Speed
    Varies
  • Wave Speed Is a Material Property

5
WAVE MECHANICS
  • The Hammer Impact Generates a Stress Wave
  • The Wave Transmits the Driving Force

6
BASIC EXPRESSION GOVERNING ONE DIMENSIONAL WAVE
PROPAGATION
  • ?2u/?t2 c2 ?2u/?x2

7
WAVE TRAVEL SPEED
  • E Modulus of Elasticity
  • ? - Mass Density

8
WAVE TRAVEL IN A PILE
9
FORCE A FUNCTION OF X
F
at time t
at time t ?t
X
x ct
10
FORCE A FUNCTION OF t
F
t
11
FORCE-VELOCITY PROPORTIONALITY e (1/c) v s
(E/c) v F (EA/c) v SO IF THE PARTICLE VELOCITY
IS KNOWN THEN STRESS AND FORCE CAN BE
CALCULATED OR THE REVERSE SO, FOR GRAPHIC
REPRESENTATION THE F v PROPORTIONALITY CAN BE
USED COMPRESSION AND DOWN VELOCITY
POSITIVE TENSION AND UP VELOCITY NEGATIVE
12
STRESS IMPEDANCE
  • For Steel
  • E/c 30,000/16,800
  • E/c 1.80 ksi/ft/sec
  • So
  • If an Air Hammer Falls 3.0 feet with an
    Efficiency of 65
  • vi (?2gh)1/2 11.2 ft/sec
  • ? is the efficiency
  • s (E/c) v (1.8)(11.2) 20 ksi

13
4. A stress wave is reflected from the free end
of a rod with the opposite sign. Compression
reflects tension.
E
v
c
14
5. A stress wave reflects from a fixed end with
the same sign. Compression reflects compression.
  1. An increase in cross section will reflect a wave
    of the same sign. A decrease in cross section
    will reflect a wave of the opposite sign.

15
REFLECTIONS FROM PILE SECTION CHANGES
  • Section Increases Reflect Compression and Up
    Velocity
  • Section Decreases Reflect Tension and Down
    Velocity
  • The Larger the Section Change the Larger the
    Reflection

16
7. If a rigid mass impacts a pile the stress is
proportional to the velocity. The stress decays
exponentially.
1
17
ENERGY CALCULATION
?? F?d ?d v?t ? ?Fvdt
18
  1. The Energy Passing a Point in a Pile During the
    Passage of a Stress Wave Is

? ?Fvdt
19
The Energy Passing a Point in a Pile During the
Passage of a Stress Wave Is
? ?Fvdt If F EA/c (v) Then ? c/EA ?F2 dt
Assumes No Reflections Half Kinetic Half
Strain
20
R
L1
L
R 2
Force
R 2
EA c
v
R 2
F
Force
EA c
v
21
FR 2
F - R 2
Force
EA c
v
R
EA c
v
Force,
R
EA c
t
v
Force,
22
Soil Resistance Effects on Force and Velocity
23
Force and Velocity Measurements for Various Soil
Conditions.
24
Energy transfer in easy driving conditions
25
Energy transfer in hard driving conditions
26
Effects of diesel hammer pre-ignition on energy
transfer
27
Effects of diesel hammer pre-ignition on energy
transfer cont.
28
Force and Velocity Measurements Illustrating
Progressive Concrete Pile Damage
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