24
Mix design approaches
ܸ
ୣ୮
=
ܸ
ୡ୮
െ
ܸ
(
1
െ ߙ
ߙ
)
(3.23)
where
V
cp
and
V
agg
are volumes of cement paste and aggregate respectively and
Į
agg
is the
packing density of the aggregate which can be determined experimentally. Once
the volume
of excess paste is known, the thickness of paste layer t
ep
can be calculated by dividing the
volume of excess paste to the specific surface area of the particles. It should be mentioned that
there are no universally accepted and accurate method for measuring
the specific surface area
of particle and available methods involve high cost and complex devices. However, it is
possible to mathematically calculate the thickness of the surrounding layer based on the
following assumptions (Midorikawa, et al., 2009):
1. Particles in each size group are assumed to be spherical
2. The thickness of the excess paste layer is constant for different sizes of
particles.
Based on the above conditions, the volume of excess paste for
spherical particles can be
calculated by utilizing the size distribution curve of the material.
ܸ
ୣ୮
=
[
1
6
ߨ
{(
݀
+ 2
ݐ
)
ଷ
ୀଵ
െ ݀
ଷ
}
ܸ
1
6
ߨ݀
ଷ
]
(3.24)
where t
ep
is the paste layer thickness, d
i
is the diameter of particles in fraction
i
and V
i
is the
volume share of fraction
i
.
In case that the packing density of the total particle structure (including cement) was used as
value for
Ș
agg
in Eq. (3.23) instead of the packing density of the aggregate
structure, the
flowability arises from the excess amount of water present in the particle mixture as in the
excess water layer theory (Fennis, 2011) see Figure 3.7.
Figure 3.7. Volume of water, divided into excess water and void filling water, within a concrete
mixture in a unit volume (Midorikawa et al, 2009).
25
Mix design approaches
In a sense,
excess water layer theory
and
excess paste layer theory
follow a similar principal.
Based on excess water layer theory, the water is partly used to fill the voids in the particle
structure and the rest of the water form a layer with thickness of
t
ew
. The thickness of the
water film can be calculated by: (Krell et al, 1985).
ݐ
ୣ୵
=
ܸ
௪
ܣ
݉
=
ܸ
௪
െ ܸ
(
1
െ ߙ
௧
ߙ
௧
)
ܣ
݉
(3.25)
where:
V
ew
is
the volume of excess water,
A
p
is surface area of particles,
m
p
is the mass of the
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