civl3310 structural analysis professor cc chang chapter 5: cables and arches

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Page 1: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

CIVL3310 STRUCTURAL ANALYSIS

Professor CC Chang

Chapter 5: Chapter 5: Cables and ArchesCables and Arches

Page 2: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cables: Assumptions

Cable is perfectly flexible & inextensible No resistance to shear/bending: same as

truss bar The force acting the cable is always

tangent to the cable at points along its length

Only axial force!

Page 3: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Example 5.1 Under Concentrated Forces

Determine the tension in each segment of the cable. Also, what is the dimension h?

4 unknown external reactions (Ax, Ay, Dx and Dy)

3 unknown cable tensions

1 geometrical unknown h

8 unknowns

8 equilibrium conditions

Page 4: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Solution

mmhFinally

kNT

o

BAo

BA

7428532

906 and 853

Bat mequilibriuJoint Similarly,

..tan)(,

..

BCBA

kNT

mkNmkNmTmT

M

CD

CDCD

A

796

048235554253

0

.

)()().)(/())(/(

kNT

TkNkN

TkN

BCo

BC

BCBC

BCBC

824 and 332

0854796

053796

Cat mequilibriuJoint

..

sin)/(.

cos)/(.

Page 5: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable subjected to a uniform distributed load

Consider this cable under distributed vertical load wo

The cable force is not a constant.

0sincos)2/)((

0

ve as clockwise-antiWith

0)sin()()(sin

0

0)cos()(cos

0

0

xTyTxxw

M

TTxwT

F

TTT

F

o

o

y

x

3eqn tandx

dy

2eqn wdx

)sinT(d

1eqn 0dx

)cosT(d

o

FH

wo

cos)cos(coscos TTT

Page 6: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable subjected to a uniform distributed load

From Eqn 1 and let T = FH at x = 0:

Integrating Eqn 2 realizing that Tsin = 0 at x = 0:

Eqn 5/Eqn 4:

4eqn HFttanconscosT

5eqn sin xwT o

3eqn tandx

dy

2eqn wdx

)sinT(d

1eqn 0dx

)cosT(d

o

FH

6eqn tanH

o

F

xw

dx

dy

FH

TTsin

Page 7: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable subjected to a uniform distributed load

Performing an integration with y = 0 at x = 0 yields

7eqn 2

2xF

wy

H

o

6eqn tanH

o

F

xw

dx

dy

FH

Cable profile:parabola

8eqn 2

2

h

LwF oH

y = h at x = L

9eqn 22x

L

hy

Page 8: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable subjected to a uniform distributed load

Where and what is the max tension?

T is max when x=L10eqn 22 )Lw(FT oHmax

11eqn 21 2)h/L(LwT omax

FH

4eqn cos HFT

5eqn sin xwT o

8eqn 2

2

h

LwF oH

Tmax

max

22 )( xwFT oH

Page 9: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable subjected to a uniform distributed load

FH

cos HFT

sin xwT o

tanH

o

F

xw

dx

dy

T

2

2

h

LwF oH

22x

L

hy

)2/(1 2max hLLwT o

Page 10: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable subjected to a uniform distributed load

Neglect the cable weight which is uniform along the length

A cable subjected to its own weight will take the form of a catenary curve

This curve ~ parabolic for small sag-to-span ratio

a

xcoshay

Hangers are close and uniformly spaced

If forces in the hangers are known then the structure can be analyzed

1 degree of indeterminacy

Determinate structure

hinge

Wiki catenary

Page 11: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Example 5.2The cable supports a girder which weighs 12kN/m. Determine the tension in the cable at points A, B & C.

12kN/m

Page 12: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Solution

The origin of the coordinate axes is established at point B, the lowest point on the cable where slope is zero,

Assuming point C is located x’ from B:

From B to A:

(1) 6

2

12kN/m

2222 x

Fx

Fx

F

wy

HHH

o

(2) '0.1'6

6 22 xFxF HH

FH

mxxx

xx

xFH

43.12'0900'60'

)]'30(['0.1

612

)]'30([6

12

2

22

2

FH

kN.4154

203890 x.

Page 13: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Solution

FH=154.4kN

203890 x.y

x.dx

dytan 07770

kN.cos

FT

.

.dx

dytan

A

HA

oA

.xA

4261

7953

36615717

12.43m17.57m

A

C

CT

AT

kN..cos

.

cos

FT

.

.dx

dytan

oC

HC

oC

.xC

6214044

4154

044

96604312

cos HFT

Page 14: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Example 5.3

Determine the max tension in the cable IH

Assume the cable is parabolic

(under uniformly distributed load)

75180 .AIM yyB

HyyC F.AIM 66700

kN.FH 1328

Page 15: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Example 5.3

kN.FH 1328

2

2

h

LwF oH

m/kN.wo 133

kN46.9 21 2 )h/L(LwT omax

Page 16: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Cable and Arch

flip

What if the load direction reverses?

FH

FH

Page 17: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Arches An arch acts as inverted cable so it receives

compression An arch must also resist bending and shear

depending upon how it is loaded & shaped

Page 18: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Arches Types of arches

indeterminate

indeterminate

indeterminatedeterminate

Page 19: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Three-Hinged Arch

Ax

AyBy

Bx

Page 20: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Problem 5-30

Determine reactions at A and C and the cable force

3 global Eqs1 hinge condition

Ay

Ax

Cy

Ay

Ax

By

Bx

T

Page 21: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Example 5.4

The three-hinged arch bridge has a parabolic shape and supports the uniform load. Assume the load is uniformly transmitted to the arch ribs.

Show that the parabolic arch is subjected only to axial compression at an intermediate point such as point D.

Page 22: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Solution

=160 kN=160 kN

=160 kN

=160 kN10 m

=160 kN

=160 kN

160 kN =

0 =

2

220

10xy

x

y

o

102

626

5020

20

.

.x)(dx

dytan

D

mxD

0

0

9178

D

D

D

M

V

kN.N

8 kN/m

Page 23: CIVL3310 STRUCTURAL ANALYSIS Professor CC Chang Chapter 5: Cables and Arches

Reflection: What Have You Learnt?