Crack Paths 2009
Therefore, the multiscale design method is employed to reliably prepare the
cementitious cover layer toughened by the liquid latex. The primary mechanical
properties and failure behaviour of the designed cementitious cover layer are predicted
by a revised lattice model based on the real meso-structure image of the designed
composite. In order to determine an optimized mix proportion for the designed
cementitious cover layer, the prediction results of the numerical simulation are
compared with the laboratory mechanical test results.
2. M U L T I S C A LMEA T E R I ADLESIGN
2.1 Theoretical Background
The designed cementitious composites are composed of mortar matrix and coarse
aggregate. The mortar matrix also includes two elements, i.e. hardened cement paste,
fine aggregate. Therefore, the relations between the volume fractions of each
component are expressed in Eq. (1) and Eq. (2).
Macro-scale
(1)
1 = + ca m v v
Meso-scale
1 = + fa c v v
(2)
where m v , c a v , f a v ,cv is the volume fractions of mortar matrix, coarse aggregate, fine
aggregate and hardened cement paste, respectively. For a composite material, the
stress-strain relationships of the cementitious composite and the components are as
follows [6]:
{ } ] { [ } ε σ = q
Composite element
(3)
(4)
{ } ] { [ } m m m q ε σ =
Mortar matrix element
(5)
{ }]{[}caca ca σ = q ε
Coarse aggregate element
} ] { [ } f a f a fa q ε
{
(6)
Fine aggregate element
σ =
{ } ] { [ } c c c q ε σ =
(7)
Hardened cement paste element
Based on the assumption of plane stress, the equivalent stiffness is expressed as
(8)
q
E
υ υ
υ
=
0
] [
− 1 0 0 1 0 1
υ
2
(9)
E
E
=
2 1 υ −
υ
where }{σ ,}{εand ][q are the stress, the strain and the stiffness matrix, respectively.
is the Poisson’s ratio.
Further, E is the elastic modulus,
υ
The meanvolume stress and strain of the multiscale elements are defined as [6]:
Macro-scale element
} { } { } { ca ca m m v v σ σ σ + = (10)
(11)
}{}{}{cacammvvεεε+=
Meso-scale element
} { } { } { fa fa c c m v v σ σ σ + = (12)
(13)
}{}{}{fafaccmvvεεε+=
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