Civil Engineering Reference
In-Depth Information
X
n
w
e
T
¼
Dl
1
l
1
¼
1
A
1
Dl
i
;
1
l
1
A
i
;
1
:
ð
2
:
97g
Þ
i
¼
0
Introduced in (
2.97f
) the component of the longitudinal force of the wire i in the
strand axis direction—induced by the rope twisting—is
X
n
w
S
i
;
1
¼
A
i
;
1
A
1
Dl
i
;
1
l
1
A
i
;
1
E
Dl
i
;
1
l
1
A
i
;
1
E
:
i¼0
and the enforced extension of the wire i in strand axis direction is
X
n
w
e
i
¼
1
A
1
Dl
i
;
1
l
1
A
i
;
1
Dl
i
;
1
l
1
:
i¼0
With this equation and the relation for the parallel lay strands
tan a
i
¼
r
i
r
n
tan a
n
¼
r
i
r
n
tan a
the enforced extension of the wire i in the strand axis direction is
r
1
2
r
i
;
1
x
1
r
i
;
1
r
n
;
1
e
i
¼
X
n
w
A
i
;
1
A1
tan a
r
i
;
1
x
1
1
i¼0
r
1
2
r
i
;
1
x
1
r
i
;
1
r
n
;
1
tan a
r
i
;
1
x
1
þ
1
:
ð
2
:
97h
Þ
The longitudinal stress of a wire i according to (
2.20
)—neglecting the strand
contraction and left out the index 1 as there is only one strand layer—is
r
long
;
i
¼ e
i
E
:
In addition to that the tensile stress from an outer rope tensile force is according
to (
2.31
)
S
A
cos a
i
cos b
:
r
t
;
i
¼
The both stresses can be added to a resulting tensile stress
r
res
;
i
¼
r
long
;
i
þ
r
t
;
i
:
The calculation is only valid and the rope structure remains intact, if the
resulting longitudinal stresses of all wires are tensile (positive).
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