International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1830
A Discussion of Liquefaction Mitigation Methods
Maithili K L
1
1
Assistant Professor, Department of Civil Engineering, AMC EC, Bangalore, India
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Abstract - Loose sandy deposits sometimes change to liquid
state during rapid vibrations. This is called LIQUEFACTION
and poses a serious problem. When the sandy soils liquefy,
structures built on them are seriously affected; for example,
heavy structures settle and light buried structures heave.
Reliable remediation with respect to liquefaction is necessary
in geotechnical engineering practice. The various
methodologies for the assessment of liquefaction potential and
remedial measures to mitigate liquefaction are based on
continuous research and decades of experience in design and
construction of structures. This paper reviews the different
methods available for soil improvement and aspects of
liquefaction resistant structures.
Key Words: Liquefaction, Mitigation, Sandy soils, Soil
Improvement, Grouting
1. INTRODUCTION
When subjected to strong vibrations, saturated sandy soils
may suddenly change into muddy water and start flowing.
This phenomenon is called Dzliquefactiondz. )t is a process
where the strength and stiffness of soil are reduced, which
changes the soil to liquid state due to rapid loading like an
earthquake shaking, blasting etc.
When liquefaction occurs the strength of the soil reduces and
the ability of the soil deposit to support foundations for
structures like buildings and bridges decreases. Liquefied
soil also applies higher pressure on retaining walls that
cause them to tilt or slide. This movement can cause damage
to structures on the ground surface. During liquefaction the
water pressure in the soil increases and this may cause
landslides and also collapse of dams.
2. LIQUEFACTION PHENOMENON
It is important to understand the conditions that exist in a soil
deposit before the application of rapid loading to understand
liquefaction phenomenon. A soil deposit comprises of an
assembly of individual soil particles, each particle being in
contact with the neighboring particles. The overlying soil
weight causes contact forces between the particles. Thus, the
weight of the overlying soils is transmitted through these
contacts. These contact forces hold the individual particles in
place and allow the shear resistance of soil to support a
structure on the ground surface.
The strong vibrations produced during rapid loading like
those produced during an earthquake, blasting etc. cause
shear stresses, and the soil structure deforms resulting in
decrease of contacts between the particles. As the soil
arrangement changes, the loosely packed soil particles try to
move into a denser configuration. But, during this rapid
loading, there is not sufficient time for the water in the pores
to be squeezed out. )nstead, the water is Dztrappeddz and
inhibits the soil particles from moving closer together. Thus,
the pore water pressure rises, contact forces between the
individual soil particles decreases. Then the weight of the
overlying structures which was originally supported in a
vertical direction through the contact points is instead
transmitted through pore water. The decrease of contact
between the soil particles results in reduction of shear
resistance of the soil, thereby softening and weakening the
soil deposit.
If the pore water pressure becomes too high, the soil particles
lose connection with each other. The soil will then have very
little strength, and will behave similar to a liquid with the unit
weight of the saturated soil – hence the name Dzliquefactiondz.
3. LIQUEFACTION OF SANDS
Taking the cohesion intercept as zero, the shear strength of
sandy soils as given by Mohr – Coulomb equation is,
S = tan’ ȋͳȌ
Where, S = shear strength
= effective stress
’ = Angle of shearing resistance in terms of effective stress.
Consider a sand deposit at a depth z from the ground surface
with the water table at the ground surface, the effective stress
is given as = satx z- wx z
= ’x z
Where, sat = saturated unit weight of the sand deposit
w = unit weight of water
’= submerged unit weight of the sand deposit
Thus (1) becomes, S = ’x z x tan’
If the sand deposit is shaken due to an earthquake or other
oscillatory loads, extra pore water pressure ȋu’Ȍ builds up and
the shear strength equation becomes
S = (’x z – u’Ȍ x tan’
As the excess pore water pressure increases, the shear
strength decreases. In extreme case, when the pore water
pressure increases so high that the soil looses all its shear
strength, then