Civil Engineering Reference
In-Depth Information
cos
2
a
k
E
k
A
k
P
n
W
F
k
¼
S
:
ð
2
:
22a
Þ
i¼0
Z
i
cos
3
a
i
E
i
A
i
By neglecting the contraction, the tensile force of the stranded rope is
!
X
X
n
Wj
n
S
S ¼
DL
L
z
j
cos
3
b
j
z
ij
cos
3
a
ij
E
ij
A
ij
ð
2
:
28a
Þ
j¼0
i¼0
and the tensile force in the wire k of the strand l is
cos
2
b
l
cos
2
a
kl
E
kl
A
kl
S
:
F
kl
¼
P
n
S
P
n
wj
ð
2
:
29a
Þ
j¼0
z
j
cos
3
b
j
i¼0
z
ij
cos
3
a
ij
E
ij
A
ij
The wire tensile stresses in the spiral rope and in the stranded rope are
r
tk
¼
F
k
A
k
r
tkl
¼
F
kl
and
A
kl
:
All wires have nearly the same tensile stress if a wire rope has a fibre core and
the same lay angle for all wire layers (except, of course, the centre wires in the
strands which have a higher stress than the other wires). This common tensile
stress is
S
A
cos a
cos b
:
r
t
¼
ð
2
:
31
Þ
This equation was previously given by Wiek (
1980
). In the outer wires, the
tensile stress is a little smaller than as calculated in (
2.31
).
Example 2.1: Wire tensile stress in spiral wire ropes
Calculation of the tensile stress in the wires of the open spiral wire rope 1 9 37
according to Fig.
2.4
with the global wire rope tensile stress r
z
= 300 N/mm
2
.
The tensile force of the spiral rope, is
S ¼ A
m
r
z
¼ 1
:
431
þ
6
þ
12
þ
18
ð
ð
Þ
1
:
227
Þ
r
z
¼ 45
:
61
300 ¼ 13,680 N
:
Using (
2.23
), the tensile stress in the centre wire is
45
:
61
r
z
¼
45
:
61
r
t0
¼
41
:
09
r
z
0
:
9703
3
1
þ
0
:
3
0
:
2419
2
1
:
431
þ
ð
6
þ
12
þ
18
Þ
1
:
227
r
t0
¼ 1
:
110
r
z
¼ 333 N/mm
2
:
With the same Eq. (
2.23
), the tensile stress in the wires of the layers 1, 2 and 3
with the same lay angle a = 14 is
Search WWH ::
Custom Search