Title: PILE DRIVING BY WAVE MECHANICS
1PILE DRIVINGBYWAVE MECHANICS
- George Goble
- GOBLE PILE TEST
2A 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
3WAVE PROPAGATION
Based on the assumption of linear elastic material
- 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. - A stress wave propagates unchanged in magnitude
at a constant speed, c, in a uniform cross
section pile.
4SOME 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
5WAVE MECHANICS
- The Hammer Impact Generates a Stress Wave
- The Wave Transmits the Driving Force
6BASIC EXPRESSION GOVERNING ONE DIMENSIONAL WAVE
PROPAGATION
7WAVE TRAVEL SPEED
- E Modulus of Elasticity
- ? - Mass Density
8WAVE TRAVEL IN A PILE
9FORCE A FUNCTION OF X
F
at time t
at time t ?t
X
x ct
10FORCE A FUNCTION OF t
F
t
11FORCE-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
12STRESS 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
134. A stress wave is reflected from the free end
of a rod with the opposite sign. Compression
reflects tension.
E
v
c
145. A stress wave reflects from a fixed end with
the same sign. Compression reflects compression.
- 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.
15REFLECTIONS 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
167. If a rigid mass impacts a pile the stress is
proportional to the velocity. The stress decays
exponentially.
1
17ENERGY CALCULATION
?? F?d ?d v?t ? ?Fvdt
18- The Energy Passing a Point in a Pile During the
Passage of a Stress Wave Is
? ?Fvdt
19The 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
20R
L1
L
R 2
Force
R 2
EA c
v
R 2
F
Force
EA c
v
21FR 2
F - R 2
Force
EA c
v
R
EA c
v
Force,
R
EA c
t
v
Force,
22Soil Resistance Effects on Force and Velocity
23Force and Velocity Measurements for Various Soil
Conditions.
24Energy transfer in easy driving conditions
25Energy transfer in hard driving conditions
26Effects of diesel hammer pre-ignition on energy
transfer
27Effects of diesel hammer pre-ignition on energy
transfer cont.
28Force and Velocity Measurements Illustrating
Progressive Concrete Pile Damage