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Wave-Induced Liquefaction. General Lecture B. Mutlu Sumer Technical University of Denmark, MEK, Coastal and River Engineering (formerly ISVA) 2800-Lyngby, Denmark – PowerPoint PPT presentation

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Title: Wave-Induced Liquefaction. General Lecture B. Mutlu Sumer


1
Wave-Induced Liquefaction. General Lecture
  • B. Mutlu Sumer
  • Technical University of Denmark, MEK, Coastal and
    River Engineering (formerly ISVA)
  • 2800-Lyngby, Denmark

2
Definition
  • Soft marine soils under high waves may undergo a
    process
  • in which the soil grains become completely free,
    and
  • the water-sediment mixture, as a whole, acts like
    a fluid!
  • This process is called liquefaction.
  • Under the liquefaction condition, obviously the
    soil fails!

3
Consequences. With the soil liquefied,
  • Buried pipelines may float to the surface of the
    seabed
  • Pipelines laid on the seabed may sink in the
    soil
  • Large individual blocks (like those used for
    scour protection) may penetrate into the seabed
  • Sea mines may enter into the seabed and
    eventually disappear
  • Or, an indirect effect As a result of the wave
    motion, structures may execute cyclic motions,
    resulting in local liquefaction around them,
    which may enhance scour, thus leading to the
    instability of the structures
  • Sometimes, we use wave-induced liquefaction to
    our end, to compact sand (as was done by
    LICengineering (Denmark), a member of LIMAS, in
    combination with soil replacement in an
    engineering exercise!)

4
Waves (for those who are not terribly familiar
with waves)?
  • In coastal areas, Wave height O(1-2 m)
  • In offshore areas, with water depth of 60-70 m,
    for example, wave height for 50-100 years return
    period O(10-20 m) are not unusual!
  • Wave period O(5-15 s)!

5
Two kinds of wave liquefaction
  • Liquefaction induced by the buildup of pore
    pressure, called the Residual Liquefaction
  • Liquefaction induced by the upward-directed
    pressure gradient, called the Momentary
    Liquefaction

6
Residual Liquefaction
7
Residual Liquefaction
  • The result of a lab experiment with a silt
    bottom Two time series
  • (1) Surface elevation and (2) Pressure time
    series
  • Water depth 42 cm
  • Wave height 10 cm
  • Wave period 1.6 s
  • Pressure measured at depth 16.5 cm in the soil

8
Residual Liquefaction
  • In this progressive buildup of the pore pressure,
    if the waves are high, the pressure may reach
    such levels that it will exceed the submerged
    weight of the soil above!
  • In this case, the soil grains will become unbound
    and completely free, and the soil will begin to
    act like a liquid!
  • This process is called the residual liquefaction!

9
Watch out The conditions for Residual
Liquefaction
  • Soil must be soft, like backfill in a trench
    hole, so that there is room for the grains to
    rearrange
  • (A soil with a long history of wave loading is
    unlikely to liquefy because there is not much
    room for the grains to rearrange this is due to
    compaction!)
  • Soil must be fine (silt, fine sand) so that all
    pore pressures accumulated during the wave cycle
    would not dissipate as rapidly as they develop
  • Waves must be sufficiently high

10
Residual Liquefaction. A video film
  • The video camera views the soil through the
    glass-side wall of the wave flume.
  • On the screen, in the upper left-hand corner, two
    signals in a window One is the surface
    elevation, and the other the pore pressure
    recorded at the depth 12 cm.
  • The signals recorded simultaneously with the
    videotaping.
  • Soil, Silt d50 0.045 mm Water depth 40 cm
    Wave height 17 cm, Wave period 1.6 s
  • Will see a horizontal band in the middle of the
    screen. Do not take any account of this! It is
    silicon used to fill the gap between the side
    wall of the flume and the side wall of the silt
    box.
  • Dr. Figen Hatipoglu (She is a Post-Doct at ISVA,
    Tech. Univ. Denmark) made the film.

11
Momentary Liquefaction
12
Momentary Liquefaction
  • Pressure distributions in the soil across the
    depth under the trough!
  • For two situations
  • (a) The case of a saturated soil (there is no
    gas/air in the soil)!
  • (b) The case of an unsaturated soil (there is
    gas/air in the soil)!

13
Momentary Liquefaction
  • This upward-directed pressure gradient induces a
    lift force on the soil under the wave trough
  • If the lift force exceeds the submerged weight,
    the soil will be liquefied!
  • This process is called the momentary
    liquefaction!
  • (Although there is also an upward-directed
    pressure-gradient force in the saturated case,
    this is apparently too small to cause
    liquefaction even under the highest waves!!)

14
Watch out The conditions for Momentary
Liquefaction
  • The soil must be an unsaturated soil (the soil
    may be liquefied even with Sr only slightly
    different from 1!)
  • Only a shallow, top layer of the soil is
    liquefied because of the large pressure gradient
    experienced (however, under extreme conditions,
    the liquefaction can penetrate to depths as far
    as O(0.5?Wave height))
  • Liquefaction occurs during the passage of the
    wave trough
  • Waves must be sufficiently high

15
Engineering practice
  • Be it the residual liquefaction or the momentary
    liquefaction, the question in engineering
    practice boils down to the following
  • Given the soil
  • Given the waves (50 year, 100 year,..)
  • Will there be any liquefaction risk for the soil
    supporting any structure (a pipeline, a gravity
    structure, a breakwater, a pier, a pile, a scour
    protection structure, etc.)?

16
To assess liquefaction
  • This has stimulated research on the topic in the
    area of coastal engineering over the past 20
    years
  • Three approaches have been adopted
  • Physical modelling (The ordinary physical
    modelling, and most recently the physical
    modelling involving centrifuge facilities)
  • Mathematical modelling
  • Deductions from field measurements

17
Physical modelling
  • The main objective of the physical modelling is
    to get a good understanding of the processes,
    simulated in the lab, under controlled conditions
  • It also enables systematic parametric studies
  • Furthermore, it provides data for the validation
    of mathematical models, a valuable by-product!
  • The down side, however, is that the soil response
    may not be properly extrapolated to the field
    conditions such a lab model may be treated as an
    individual prototype itself!
  • To get around the problem (of extrapolating the
    results to the prototype), centrifuge wave
    testing on a soil bed has been tried recently
    (1999, 2001)!

18
Mathematical modelling
  • The soil is assumed to be a poro-elastic medium
  • The model, which governs (1) the soil
    deformation, and (2) the movement of pore water
    (including the pore pressure), is basically the
    Biot equations
  • The latter are solved under the boundary
    condition at the seabed

19
(No Transcript)
20
Mathematical modelling
  • The Biot equations good enough to study the
    momentary liquefaction!
  • For the buildup of pore pressure and eventual
    residual liquefaction, however, we need some
    additional information
  • One such piece of information may be an empirical
    expression for the pressure generated by the
    cyclic shear (the source term!) such as

21
Mathematical modelling
  • Although this approach does a good job in
    engineering applications, it does not accommodate
    the continuous change of the soil properties, and
    particularly
  • it breaks down near liquefaction conditions!
  • Recently, sophisticated sand models have been
    developed
  • One such model which accounts for the
    contractive/dilative behavior of sand and can
    handle the long-term pore pressure buildup, has
    been adopted by HR!
  • HR will present early results of this approach,
    as applied to the wave-induced liquefaction!

22
Commercial!
  • Great many works have been devoted to the
    physical and mathematical modelling of
    wave-induced liquefaction.
  • A detailed account of these works (and its impact
    on scour-related problems) (with over 80
    references) is given in Chapter 10 in the book by
  • Sumer, B.M. and Fredsøe, J. (2002). The Mechanics
    of Scour in the Marine Environment. World
    Scientific, xiv536 p.

23
Deductions from field measurements
  • Field measurements not terribly easy to
    interpret. This is largely because we have no
    control over the test conditions!
  • Yet, we can make useful deductions from field
    data! (We have one wave-induced-liquefaction
    field study in LIMAS, Université de Pau and had
    one in SCARCOST, the predecessor of LIMAS,
    under EU MAST-III programme)
  • In this conjunction, another sensible approach
    would be to simulate the field conditions in the
    lab in a large-scale wave facility (We have one
    such study in LIMAS, Technische Universitat
    Braunschweig)

24
http//www.ce.washington.edu/liquefaction/html/wh
at/what1.html
25
Centrifuge facilities
  • Two types
  • (1) Beam type (Sassa Sekiguchi, 1999) and
  • (2) Drum type (pretty much the same as a washing
    machine!) (Mark Randolph Liang Cheng, Univ. of
    Western Australia)

26
Issues in engineering practice
  • Marine pipelines may be buried against heavy
    traffic, or fishing gear. (Dredge a trench Place
    the pipe in it Backfill the trench with the
    excavated material)).
  • Question Is the backfill material liquefaction
    resistant? (Otherwise the pipeline will float to
    the surface!) Or should it be replaced with a
    coarser material?

27
Issues in engineering practice
  • Marine pipelines may also be laid on the seabed.
  • Question Will the seabed be liquefied under
    extreme storm events (100 year storm) if it is a
    soft soil?
  • (Although there will be very little room for the
    rearrangement of grains, and therefore for the
    residual liquefaction, due to a long exposure of
    waves. However, remember the momentary
    liquefaction!)
  • If the bed is liquefied, that will jeopardize the
    pipelines stability!

28
Issues in engineering practice
  • Marine structures are protected against scour by
    scour protection (rock, armour blocks,..).
  • Question Can the supporting soil be liquefied
    under extreme storm events? If yes, to what
    depths do the elements of scour protection sink
    in the liquefied soil?

29
Issues in engineering practice
  • Marine structures (such as caisson breakwaters,
    gravity structures, piles) execute rocking motion
    under waves.
  • This may cause liquefaction around the structure,
    inducing enhancement in scour, and therefore
    endangering the stability of the structure
  • Question What is the extent of liquefaction
    around the structure?

30
Residual Liquefaction
31
Large-time behavior
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