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VECTOR MECHANICS FOR ENGINEERS: STATICS Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University CHAPTER © 2007 The McGraw-Hill Companies, Inc. All rights reserved. 7 Forces in Beams and Cables

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VECTOR MECHANICS FOR ENGINEERS:

STATICS

Eighth Edition

Ferdinand P. Beer

E. Russell Johnston, Jr.

Lecture Notes:

J. Walt Oler

Texas Tech University

CHAPTER

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

7 Forces in Beams

and Cables

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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Contents

Introduction

Internal Forces in Members

Sample Problem 7.1

Various Types of Beam Loading

and Support

Shear and Bending Moment in a

Beam

Sample Problem 7.2

Sample Problem 7.3

Relations Among Load, Shear,

and Bending Moment

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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Contents

Sample Problem 7.4

Sample Problem 7.6

Cables With

Concentrated Loads

Cables With

Distributed Loads

Parabolic Cable

Sample Problem 7.8

Catenary

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Introduction

•Preceding chapters dealt with:

a) determining external forces acting on

a structure and

b)determining forces which hold together

the various members of a structure.

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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Introduction

•The current chapter is concerned with

determining the internal forces (i.e.,

tension/compression, shear, and

bending) which hold together the

various parts of a given member.

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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•Focus is on two important types of

engineering structures:

a)Beams - usually long, straight,

prismatic members designed to

support loads applied at various points

along the member.

b)Cables - flexible members capable of

withstanding only tension, designed to

support concentrated or distributed

loads.

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Internal Forces in Members

•Straight two-force

member AB is in

equilibrium under

application of F and

-F. •Internal forces

equivalent to F and -F

are required for

equilibrium of free-

bodies AC and CB.

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Internal Forces in Members

•Multiforce member

ABCD is in equili-

brium under

application of cable

and member contact

forces.

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Internal Forces in Members

•Internal forces

equivalent to a

force-couple

system are

necessary for

equili-brium of

free-bodies JD

and ABCJ.

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Internal Forces in Members

•An internal force-couple system is

required for equilibrium of two-

force members which are not

straight.

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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Beams

7- 11

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Pure Bending

Pure Bending: Prismatic members subjected

to equal and opposite couples acting in the

same longitudinal plane

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7- 14

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Post and Lintel

7- 16

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Parthenon, Athens

7- 17

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Corbelled domes and vaults

7- 18

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Various Types of Beam Loading and Support

•Beam - structural member

designed to support loads

applied at various points

along its length.

•Beam can be subjected

to concentrated loads or

distributed loads or

combination of both.

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Various Types of Beam Loading and Support

• Beam design is two-step

process:

1)determine shearing forces

and bending moments

produced by applied loads

2)select cross-section best

suited to resist shearing

forces and bending

moments

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Various Types of Beam Loading and Support

•Beams are classified according to way in

which they are supported.

•Reactions at beam supports are

determinate if they involve only three

unknowns. Otherwise, they are statically

indeterminate.

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Various Types of Beam Loading and Support

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Shear and Bending Moment in a Beam

• Wish to determine bending moment and

shearing force at any point in a beam

subjected to concentrated and distributed

loads.

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Shear and Bending Moment in a Beam

• Determine reactions at supports by

treating whole beam as free-body.

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Shear and Bending Moment in a Beam

• From equilibrium considerations,

determine M and V or M’ and V’.

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Shear and Bending Moment in a Beam

• Cut beam at C and draw free-body diagrams for AC

and CB. By definition, positive sense for internal

force-couple systems are as shown. This way we

don’t have to specify from which section ( AC or BC)

we are calculating V and M.

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Shear and Bending Moment Diagrams

• Variation of shear and bending moment along

beam may be plotted. • Determine reactions at supports.

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22 PxMPV

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22 xLPMPV

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Shear and Bending Moment Diagrams

• Cut beam at E and consider member EB, 22 xLPMPV

• Cut beam at C and consider member AC,

22 PxMPV

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Shear and Bending Moment Diagrams

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Shear and Bending Moment Diagrams

• For a beam subjected to concentrated loads,

shear is constant between loading points and

moment varies linearly.

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Sample Problem 7.2

Draw the shear and bending moment

diagrams for the beam and loading shown.

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• Taking entire beam as a free-body, calculate

reactions at B and D.

• Find equivalent internal force-couple systems for

free-bodies formed by cutting beam on either side

of load application points.

• Plot results.

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:0yF

0kN20 1V kN201V

:01M

0m0kN20 1M 01M

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Sample Problem 7.2

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Sample Problem 7.2

7- 42

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0kN14

mkN28kN14

mkN28kN26

mkN50kN26

66

55

44

33

MV

MV

MV

MV

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Sample Problem 7.2

•Plot results.

Note that shear is

of constant value

between

concentrated

loads and bending

moment varies

linearly.

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UDL (Uniformly distributed load)

7- 45

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7- 50

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Sample Problem 7.3

7- 53

Draw the shear and bending moment

diagrams for the beam AB. The

distributed load of 7200 N/m extends over

0.3 m of the beam, from A to C, and the

1800-N load is applied at E.

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Sample Problem 7.3

7- 54

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Sample Problem 7.3

7- 55

SOLUTION:

•Taking entire beam as free-body,

calculate reactions at A and B.

•Determine equivalent internal force-

couple systems at sections cut within

segments AC, CD, and DB.

•Plot results.

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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Sample Problem 7.3

7- 56

SOLUTION:

• Taking entire beam as a free-body, calculate

reactions at A and B.

:0AM

0m550N1800m150N2160m80 ...By

N51642 .By

:0BM

0m8.0N25.0N1800m65.0N2160 A

N52317.A

:0xF 0xB

• Note: The 1800-N load at E may be replaced by

a 1800-N force and 180-N . m couple at D.

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Sample Problem 7.3

7- 57

• Evaluate equivalent internal force-

couple systems at sections cut

within segments AC, CD, and DB.

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:01M 072005231721 Mxxx.

m.N )360052317( 2xx.M

From A to C:

:0yF 0720052317 Vx.

N)720052317( x.V

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Sample Problem 7.3

7- 61

:02M 0150216052317 M.xx.

mN 5157324 x.M

From C to D:

:0yF 0216052317 V.

N 5157.V

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Sample Problem 7.3

7- 63

:03M

04501800

180150216052317

M.x

.xx.

mN 516421314 x.M

From D to B:

:0yF

01800216052317 V.

N 51642.V

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Sample Problem 7.3

7- 64

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Sample Problem 7.3

7- 65

• Plot results.

From A to C:

From C to D:

From D to B:

N)720052317( x.V

m.N )360052317( 2xx.M

N 5157.V

mN 5157324 x.M

N 51642.V

mN 516421314 x.M

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Relations Among Load, Shear, and Bending Moment

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Relation between load and shear

wx

V

dx

dV

xwVVV

x 0lim

0

curve loadunder areaD

C

x

xCD dxwVV

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Relation between Shear, and Bending Moment

VxwVx

M

dx

dM

xxwxVMMM

xx 21

00limlim

02

curveshear under areaD

C

x

xCD dxVMM

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Relations Among Load, Shear, and Bending Moment

•Reactions at supports,

2

wLRR BA

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Relations Among Load, Shear, and Bending Moment

•Reactions at supports,

2

wLRR BA

•Shear curve,

xL

wwxwL

wxVV

wxdxwVV

A

x

A

22

0

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•Moment curve,

0at 8

22

2

max

2

0

0

Vdx

dMM

wLM

xxLw

dxxL

wM

VdxMM

x

x

A

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Sample Problem 7.4

Draw the shear and bending-

moment diagrams for the beam

and loading shown.

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Sample Problem 7.4

SOLUTION:

•Taking entire beam as a

free-body, determine

reactions at supports.

•Between concentrated load

application points,

and shear is constant.

0wdxdV

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Sample Problem 7.4

•With uniform loading

between D and E, the

shear variation is

linear.

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Sample Problem 7.4

•Between concentrated load application

points, The

change in moment between load

application points is equal to area under

shear curve between points.

const.VdxdM

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Sample Problem 7.4

•With a linear shear variation

between D and E, the bending

moment diagram is a

parabola.

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SOLUTION:

Taking entire beam as a free-body,

determine reactions at supports.

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Sample Problem 7.4

:0AM

0m .48kN 12

m .24kN 12m .81kN 20m .27D

kN 26D

:0yF

0kN 12kN 26kN 12kN 20yA

kN 18yA

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Sample Problem 7.4

•Between concentrated

load application points,

and shear is constant.

0wdxdV

•With uniform loading

between D and E, the

shear variation is linear.

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Sample Problem 7.4

•Between concentrated load application

points,

•The change in moment between load

application points is equal to area under

the shear curve between points.

.constVdxdM

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048

mkN 48140

mkN 9216

mkN 108108

EDE

DCD

CBC

BAB

MMM

MMM

MMM

MMM

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Sample Problem 7.4

•With a linear shear variation between D

and E, the bending moment diagram is a

parabola.

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Sample Problem 7.4

•With a linear shear variation between

D and E, the bending moment diagram

is a parabola.

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Sample Problem 7.6

Sketch the shear

and bending-

moment

diagrams for the

cantilever beam

and loading

shown.

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Sample Problem 7.6

SOLUTION:

The change in shear

between A and B is equal

to the negative of area

under load curve between

points. The linear load

curve results in a

parabolic shear curve.

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Sample Problem 7.6

•With zero load, change

in shear between B

and C is zero.

•The change in moment between A and B

is equal to area under shear curve

between points. The parabolic shear

curve results in a cubic moment curve.

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Sample Problem 7.6

•The change in moment

between B and C is

equal to area under

shear curve between

points. The constant

shear curve results in a

linear moment curve.

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Sample Problem 7.6

SOLUTION:

•The change in shear

between A and B is equal

to negative of area under

load curve between

points. The linear load

curve results in a

parabolic shear curve.

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Sample Problem 7.6

•With zero load, change in shear between

B and C is zero.

awVV AB 021 awVB 02

1

0,at wdx

dVB

0,0,at wwdx

dVVA A

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

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Sample Problem 7.6

•The change in moment

between A and B is

equal to area under

shear curve between

the points. The

parabolic shear curve

results in a cubic

moment curve.

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Sample Problem 7.6

aLawMaLawMM

awMawMM

CBC

BAB

3061

021

203

1203

1

0,0,at Vdx

dMMA A

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Sample Problem 7.6

•The change in moment

between B and C is

equal to area under

shear curve between

points. The constant

shear curve results in a

linear moment curve.