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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