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Structure Analysis I
Chapter 5
Structure Analysis I
Chapter 5
Cables & Arches
Cables
• Cables are often used in engineering structure to
support and or transmit loads from one member to
another
Structural Analysis IDr. Mohammed Arafa
Cables subjected to concentrated
loads
Example 1
Determine the tension in cables and what is the dimension h ?
   
kNT
TT
M
CD
CDCD
A
79.6
0)4(8)2(35.52
0
5
4
5
3



o
BC
BC
BCBCy
BCBCx
T
TF
TF
3.32
82.4
0sin8)(79.60
0cos)(79.60
5
4
5
3









o
BA
BA
BABA
o
y
BABA
o
x
T
TF
TF
8.53
90.6
0sin3)3.32(sin82.40
0cos)3.32(cos82.40









  mh 74.28.53tan2 
Cables subjected to a Uniform
Distributed Load
Cables subjected to a Uniform
Distributed Load
Analysis Procedure
   
   0
0
0 cos cos 0
0 sin sin 0
0 cos sin 0
2
Dividingeach eq. byΔx and taking thelimit as Δx 0
and hence y 0, 0 and T 0
x
y
o
F T T T
F T w x T T
x
M w x T y T x
  
  
 

       
         

       

     



Analysis Procedure
Structural Analysis IDr. Mohammed Arafa
 
 
0
cos
0 (1)
sin
(2)
tan (3)
d T
dx
d T
w
dx
dy
dx






Analysis Procedure
 
 
H
0
0
at x=0 T=F
Integrate eqs. 1 where T=F at x=0
cos (4)
Integrate eqs. 2 where Tsin =0 at x=0
sin (5)
dividing 4 by 5
tan =
H
H
H
T F
T w x
w xdy
dx F








Analysis Procedure
2
0 0
2
0
2
2
2
,
2
H H
H
w x w xdy
y
dx F F
w L
at x L y h F
h
h
y x
L
  
  
 
Analysis Procedure
 
max
2 2
max
0
2
22
max 0 0
cos
cos
is at where is maximum
( )
In our Case at x=L
1
2
H
H
H
H
T F
F
T
T
at x L
T F V
V w L
L
T F w L w L
h






 

 
     
 
Analysis Procedure
 
2
2
2
0
2 2
22 2 2
max max 0
2
cos
H
H
H
H H
h
y x
L
w L
F
h
F
T F V
T F V F w L



  
   
Summary
Suspension Bridge
Cable Stayed Bridge
Example 2
Determine the tension of the cable at points A, B, C
Assume the girder weight is 850 lb/ft
Structural Analysis IDr. Mohammed Arafa
2 2 2 2
max
500 30
7500 Ib=7.5k
2 2
7.031 7.5 10.280
A B
A B
WL
V V
T T T H V

   
      
Example 3
Determine the tension of the cable at points A, B
 
2
500 15
7031.25
2 8
HF  

2
0
2
H
w L
F
h


HF
AV BV
HF
Example 4
Problem 1: The cable AB is subjected to a uniform loading of
200kN/m. If the weight of the cable is neglected and the slope angles at
points A and B are 30 and 60, respectively, determine the curve that
defines the cable shape and the maximum tension developed in the
cable.
 
 
0 0 1
Integrate the equations
(1)
(2)
cos
0 cos
sin
sin
H
d T
T F
dx
d T
w T w x C
dx




  
   


1
0
Substitute at 0
sin30 tan3
30
cos cos30
eq.(2) willbe:
sin tan
0
(3)30
A
H H
H
A H
F F
T T
T
x
C T
F
F
w x






 





 
  
     
0
2
tan30
tan
1
0.2 tan30
60
1
tan 60 0.2 15 tan30
Divide
2.6
1 1
0.2 tan30 0.2 2.
(3) by (1)
Substitute
6 0.577
2.60
0
at 15
(Equation of thecablecurv.0385 0.577 e)
H
H
H
H
H
H
H
H
H
w x F
F
dy
x F
dx F
F
F
F kN
dy
x F x
dx F
x x
x
y




 

 



   
 
max
cos
2.6
cos cos
At 0 30
2.6
3.0
cos3
Substitute in (1)
0
At 15 60
2.6
5.2
cos60
H
H
A
B
T F
F
T
x
T kN
x
T kN T

 



 
 
 
 
  
Problem 2: Determine the maximum and minimum tension in the
parabolic cable and the force in each of the hangers. The girder is
subjected to the uniform load and is pin connected at B.
Draw the shear and moment diagrams for the pin connected girders
AB and BC.
HF
HF
HF
HF
0
5 5 2.5 0.5 0 (1)
0
20 20 10 8 0 (2)
Solve(1) and (2) 0 & 25
A
y H
C
y H
y H
M
B F
M
B F
B F kN

     

     
 


 
 
2
0
2
0
0
min
22
max 0
22
2
20
25
2 8
1 /
For the main Cabl
25
25 1 20 32.02
e
H
H
H
w L
F
h
w
w kN m
T F kN
T F w L
kN




 
 
   
0
Force in each ha
2.5 1 2.5 2
g
.5
n er
T w kN    
Problem ٣: The beams AB and BC are supported by the cable that
has a parabolic shape. Determine the tension in the cable at points
D, F, and E, and the force in each of the equally spaced hangers
Arches
Arches Types
Example of Fixed Arch
Three Hinge Arches
Example 5
Determine the internal forces at Section D
 
kNA
kNA
F
kNB
BM
kNB
BM
y
x
x
x
xRightC
y
yA
93
0F
86
0
86
0)20(67)8(60)6(0
67
0)28(60)10(100)40(0
y












86
93
86 cos20
93 sin20
86 sin20
93 cos20
242
242
112.6
58
Example 6
Determine the internal forces at Section D
 
y
0 25
F 0
25
0 25 (50) (25) 25 (25) 0
25
0
25
A y
y
B xRight
x
x
x
M C kips
A kips
M C
C kips
F
A kips
  


    







yF 0
0
0
25
y
x
x
B
F
B kips






 
 
2
2
2
1
2
25
25
50
25
2
50
25
tan 2 25 0.5
50
26.6
x
o
y x
dy
x
dx
dy
dx








    

25cos 12.5sin 27.95
25 12.5cos 0.0
25(6.25) 12.5(12.5) 0
D
D
D
N
V sin
M
 
 
  
  
   
26.6o
 
Example 7
Structural Analysis IDr. Mohammed Arafa
Problem 3
Determine the internal forces at B

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Chapter 5-cables and arches

  • 1. Structure Analysis I Chapter 5 Structure Analysis I Chapter 5
  • 3. Cables • Cables are often used in engineering structure to support and or transmit loads from one member to another Structural Analysis IDr. Mohammed Arafa
  • 4. Cables subjected to concentrated loads
  • 5. Example 1 Determine the tension in cables and what is the dimension h ?
  • 6.     kNT TT M CD CDCD A 79.6 0)4(8)2(35.52 0 5 4 5 3    o BC BC BCBCy BCBCx T TF TF 3.32 82.4 0sin8)(79.60 0cos)(79.60 5 4 5 3         
  • 8. Cables subjected to a Uniform Distributed Load
  • 9. Cables subjected to a Uniform Distributed Load
  • 11.        0 0 0 cos cos 0 0 sin sin 0 0 cos sin 0 2 Dividingeach eq. byΔx and taking thelimit as Δx 0 and hence y 0, 0 and T 0 x y o F T T T F T w x T T x M w x T y T x                                               Analysis Procedure Structural Analysis IDr. Mohammed Arafa
  • 12.     0 cos 0 (1) sin (2) tan (3) d T dx d T w dx dy dx       Analysis Procedure
  • 13.     H 0 0 at x=0 T=F Integrate eqs. 1 where T=F at x=0 cos (4) Integrate eqs. 2 where Tsin =0 at x=0 sin (5) dividing 4 by 5 tan = H H H T F T w x w xdy dx F         Analysis Procedure
  • 14. 2 0 0 2 0 2 2 2 , 2 H H H w x w xdy y dx F F w L at x L y h F h h y x L         Analysis Procedure
  • 15.   max 2 2 max 0 2 22 max 0 0 cos cos is at where is maximum ( ) In our Case at x=L 1 2 H H H H T F F T T at x L T F V V w L L T F w L w L h                    Analysis Procedure
  • 16.   2 2 2 0 2 2 22 2 2 max max 0 2 cos H H H H H h y x L w L F h F T F V T F V F w L           Summary
  • 19.
  • 20. Example 2 Determine the tension of the cable at points A, B, C Assume the girder weight is 850 lb/ft Structural Analysis IDr. Mohammed Arafa
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  • 25. 2 2 2 2 max 500 30 7500 Ib=7.5k 2 2 7.031 7.5 10.280 A B A B WL V V T T T H V             Example 3 Determine the tension of the cable at points A, B   2 500 15 7031.25 2 8 HF    2 0 2 H w L F h   HF AV BV HF
  • 27.
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  • 30. Problem 1: The cable AB is subjected to a uniform loading of 200kN/m. If the weight of the cable is neglected and the slope angles at points A and B are 30 and 60, respectively, determine the curve that defines the cable shape and the maximum tension developed in the cable.
  • 31.     0 0 1 Integrate the equations (1) (2) cos 0 cos sin sin H d T T F dx d T w T w x C dx              1 0 Substitute at 0 sin30 tan3 30 cos cos30 eq.(2) willbe: sin tan 0 (3)30 A H H H A H F F T T T x C T F F w x             
  • 32.            0 2 tan30 tan 1 0.2 tan30 60 1 tan 60 0.2 15 tan30 Divide 2.6 1 1 0.2 tan30 0.2 2. (3) by (1) Substitute 6 0.577 2.60 0 at 15 (Equation of thecablecurv.0385 0.577 e) H H H H H H H H H w x F F dy x F dx F F F F kN dy x F x dx F x x x y                  
  • 33. max cos 2.6 cos cos At 0 30 2.6 3.0 cos3 Substitute in (1) 0 At 15 60 2.6 5.2 cos60 H H A B T F F T x T kN x T kN T                 
  • 34. Problem 2: Determine the maximum and minimum tension in the parabolic cable and the force in each of the hangers. The girder is subjected to the uniform load and is pin connected at B. Draw the shear and moment diagrams for the pin connected girders AB and BC.
  • 35. HF HF HF HF 0 5 5 2.5 0.5 0 (1) 0 20 20 10 8 0 (2) Solve(1) and (2) 0 & 25 A y H C y H y H M B F M B F B F kN                  
  • 36.     2 0 2 0 0 min 22 max 0 22 2 20 25 2 8 1 / For the main Cabl 25 25 1 20 32.02 e H H H w L F h w w kN m T F kN T F w L kN             0 Force in each ha 2.5 1 2.5 2 g .5 n er T w kN    
  • 37.
  • 38. Problem ٣: The beams AB and BC are supported by the cable that has a parabolic shape. Determine the tension in the cable at points D, F, and E, and the force in each of the equally spaced hangers
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  • 46. Example 5 Determine the internal forces at Section D   kNA kNA F kNB BM kNB BM y x x x xRightC y yA 93 0F 86 0 86 0)20(67)8(60)6(0 67 0)28(60)10(100)40(0 y            
  • 47. 86 93 86 cos20 93 sin20 86 sin20 93 cos20 242 242 112.6 58
  • 48. Example 6 Determine the internal forces at Section D
  • 49.   y 0 25 F 0 25 0 25 (50) (25) 25 (25) 0 25 0 25 A y y B xRight x x x M C kips A kips M C C kips F A kips                 
  • 51.     2 2 2 1 2 25 25 50 25 2 50 25 tan 2 25 0.5 50 26.6 x o y x dy x dx dy dx               25cos 12.5sin 27.95 25 12.5cos 0.0 25(6.25) 12.5(12.5) 0 D D D N V sin M               26.6o  
  • 52. Example 7 Structural Analysis IDr. Mohammed Arafa
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  • 56. Problem 3 Determine the internal forces at B