14
3.
Emergence of Unsaturated Soil Mechanics in Pavement
Engineering
As discussed
in the previous chapter, the unbound layers in pavement structures and
the upper part of the subgrade can experience considerable
variation in the moisture
content throughout the year. The moisture content of the unbound layers can fluctuate
seasonally from the natural equilibrium condition due to several reasons, i.e.
winter frost
action and spring-thaw in cold regions, infiltration during rain events and variation in
the groundwater table.
Even though the underlying materials in pavement structures are generally in partially
saturated conditions, the impact of an unsaturated state on the mechanical behaviour of
the unbound materials and subgrade soils is generally not taken into account. The
performance of the pavement structures can to a large
extent be affected by the
behaviour of the underlying unbound materials and more reliable performance
prediction of pavement systems require consideration for the unsaturated state.
The mechanical behaviour of the soil is generally governed by the stress variables that
control the equilibrium of the soil structure (Fredlund and Morgenstern, 1977). An
unsaturated soil element consists of four different phases: soil particles or solid phase,
water phase, air phase and the contractile skin. The total equilibrium equation of this
four-phase soil structure can be formulated using the force equilibrium equation for the
air phase, water phase, contractile skin phase and the total equilibrium equation for the
soil element (Fredlund et al., 2012).
From the equilibrium equation of the unsaturated soil structure, three independent sets
of normal stresses can be extracted to form the stress state variables. These three
normal stress state variables are (
a
u
), (
w
a
u
u
) and
a
u
, where
is the total normal
stress and
𝑢
𝑎
and
𝑢
𝑤
are pore-air and pore-water pressures, respectively. The difference
between the pore-air and pore-water pressures (
w
a
u
u
)
within the unsaturated soil
structure is known as the matric suction (
m
). Assuming that the soil particles are
incompressible, the stress variable
𝑢
𝑎
can be eliminated and therefore the stress
state
variables for the unsaturated soil structure can be defined as (
a
u
) and (
w
a
u
u
)
(Fredlund et al., 2012). As the moisture content of the soil increases and the soil
structure goes from an unsaturated state to a fully saturated state (
S
=
100%) the
pore-water pressure approaches the pore-air pressure and therefore the matric suction
of the soil structure (
w
a
m
u
u
) goes toward zero. Matric suction is therefore known
to be the state variable with the highest relevance to unsaturated soil mechanics. The
matric suction of the subgrade is highly dependent on the moisture content of the soil
structure, commonly defined by the soil-water characteristic curves.
15
Since matric suction of the soil structure is directly related to its moisture content, and
moisture is the main environmentally driven factor affecting the behaviour of unfrozen
unbound layers, matric suction can be incorporated
into the material response
characterization models (i.e. the stiffness) for capturing the seasonal moisture variation
effects. Accounting for suction effects in the mechanical behaviour of unbound
materials is particularly important in materials with a high fines content (i.e. in subgrade
soils) (Khogali et al, 1991; Zapata et al., 2009).
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