PSI - Issue 64
Francesco Focacci et al. / Procedia Structural Integrity 64 (2024) 1557–1564 Author name / Structural Integrity Procedia 00 (2019) 000–000
1559
3
where u f ( z ) and u c ( z ) are the longitudinal displacements of the fibers and matrix at the interface, respectively.
a
b
c
d
q ( z ) = λ q 0 ( z )
d G
M t +d M t
M 1 +d M 1
M 1 +d M 1
M t
M 1
M 1
H
N t +d N t
N 1 +d N 1
N +d N
N t
N 1
N
V t +d V t
V 1 +d V 1
V t +d V t
V t
V 1
V t
z
d z
τ ( s )
τ ( s )
d z
N 2 +d N 2
N 2
N +d N
N
d z
d z
Fig. 1. (a) Composite beam; (b) internal forces in the composite beam; (c) internal forces in the layers; (d) internal forces in the layers with N t =0.
Un-cracked cross-sections In the un-cracked portions of the beam, the displacement u c ( z ) is continuous and differentiable, whereas u f ( z ) is continuous and differentiable at any z . The introduction of the curvature χ = χ( z ) and the axial force N = N (z) in the derivative of Eq. (2) yields:
d
N
( )
(
)
(3)
s z
−χ − n H d
=
d
z
E A
f
f
where A f and E f are the cross-sectional area and the elastic modulus of fibers, respectively, H is the height of the concrete beam, and d n is the neutral axis depth (Fig. 2a). Eq. (3) implies that fibers are linear elastic and the concrete beam cross-sections remain plane during the loading process.
d z
a
b
d c
w
|σ cw |
d G
d n d G
M 1
M 1
H
H
χ
∆ϕ
x
x
G
G
N
N
G
ε
|σ c |
G
G
b ( ζ )
b ( ξ )
ξ
ζ
y
y
ζ
ζ
ξ
ξ
| s r |
| s l |
∆ϕ ( H - d c )
Fig. 2. (a) Un-cracked cross-section of the concrete layer; (b) cracked cross-section.
The equilibrium of an infinitesimal segment of fibers of length d z (Fig. 1c and d) yields:
d
( ) = τ f N z p z ( )
(4)
d
z
where ( ) ( ) ( ) τ = τ z s z is the shear stress at the coordinate z , where the slip is s (z), p f is the width of the fiber-matrix interfacial surface, and ( ) s τ is the interfacial cohesive material law (CML). Eqs. (3) and (4), together with the definition of the curvature, constitute the following system of differential equations:
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