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MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt Oler Texas Tech University CHAPTER © 2009 The McGraw-Hill Companies, Inc. All rights reserved. 6 Shearing Stresses in Beams and Thin- Walled Members

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Page 1: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF

MATERIALS

Fifth SI Edition

Ferdinand P. Beer

E. Russell Johnston, Jr.

John T. DeWolf

David F. Mazurek

Lecture Notes:

J. Walt Oler

Texas Tech University

CHAPTER

© 2009 The McGraw-Hill Companies, Inc. All rights reserved.

6Shearing Stresses in

Beams and Thin-

Walled Members

Page 2: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

Fifth

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6- 2

Shear on the Horizontal Face of a Beam Element

• Consider prismatic beam

• For equilibrium of beam element

A

CD

ACDx

dAyI

MMH

dAHF

0

xVxdx

dMMM

dAyQ

CD

A

• Note,

flowshearI

VQ

x

Hq

xI

VQH

• Substituting,

Page 3: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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Shear on the Horizontal Face of a Beam Element

• where

section cross full ofmoment second

above area ofmoment first

'

2

1

AA

A

dAyI

y

dAyQ

• Same result found for lower area

HH

QQ

qI

QV

x

Hq

axis neutral to

respect h moment witfirst

0

flowshearI

VQ

x

Hq

• Shear flow,

Page 4: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Concept Application 6.1

A beam is made of three planks,

nailed together. Knowing that the

spacing between nails is 25 mm and

that the vertical shear in the beam is

V = 500 N, determine the shear force

in each nail.

SOLUTION:

• Determine the horizontal force per

unit length or shear flow q on the

lower surface of the upper plank.

• Calculate the corresponding shear

force in each nail.

Page 5: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

Fifth

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6- 5

Concept Application 6.1

Page 6: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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6- 6

Determination of the Shearing Stress in a Beam

• The average shearing stress on the horizontal

face of the element is obtained by dividing the

shearing force on the element by the area of

the face.

It

VQ

xt

x

I

VQ

A

xq

A

Have

• b<=h/4,C1及C2點之剪應力值

不會超過沿中性軸之應力

平均值0.8% (p377)

• On the upper and lower surfaces of the beam,

yx= 0. It follows that xy= 0 on the upper and

lower edges of the transverse sections.

Page 7: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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Shearing Stresses xy in Common Types of Beams

• For a narrow rectangular beam,

A

V

c

y

A

V

Ib

VQxy

2

3

12

3

max

2

2

• For American Standard (S-beam)

and wide-flange (W-beam) beams

web

ave

A

V

It

VQ

max

Page 8: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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6- 8

Concept Application 6.2

τall=1.75MPa, Check that the design is acceptable

from the point of view of the shear stresses

Page 9: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

Fifth

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Sample Problem 6.1

6- 9

Page 10: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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Sample Problem 6.2

A timber beam is to support the three

concentrated loads shown. Knowing

that for the grade of timber used,

MPa8.0MPa12 allall

determine the minimum required depth

d of the beam.

SOLUTION:

• Develop shear and bending moment

diagrams. Identify the maximums.

• Determine the beam depth based on

allowable normal stress.

• Determine the beam depth based on

allowable shear stress.

• Required beam depth is equal to the

larger of the two depths found.

Page 11: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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Sample Problem 6.2

SOLUTION:

Develop shear and bending moment

diagrams. Identify the maximums.

kNm95.10

kN5.14

max

max

M

V

Page 12: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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Sample Problem 6.2

2

261

261

3121

m015.0

m09.0

d

d

dbc

IS

dbI

Page 13: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Shearing Stresses in Thin-Walled Members

• Consider a segment of a wide-flange

beam subjected to the vertical shear V.

• The longitudinal shear force on the

element is

xI

VQH

It

VQ

xt

Hxzzx

• The corresponding shear stress is

• NOTE: 0xy

0xz

in the flanges

in the web

• Previously found a similar expression

for the shearing stress in the web

It

VQxy

Page 14: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Shearing Stresses in Thin-Walled Members

• The variation of shear flow across the

section depends only on the variation of

the first moment.

I

VQtq

• For a box beam, q grows smoothly from

zero at A to a maximum at C and C’ and

then decreases back to zero at E.

• The sense of q in the horizontal portions

of the section may be deduced from the

sense in the vertical portions or the

sense of the shear V.

Page 15: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Shearing Stresses in Thin-Walled Members

• For a wide-flange beam, the shear flow

increases symmetrically from zero at A

and A’, reaches a maximum at C and

then decreases to zero at E and E’.

• The continuity of the variation in q and

the merging of q from section branches

suggests an analogy to fluid flow.

Page 16: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Sample Problem 6.3

Knowing that the vertical shear is 200

kN in a W250x101 rolled-steel beam,

determine the horizontal shearing

stress in the top flange at the point a.

Page 17: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Sample Problem 6.5 (自行練習)

6- 17

Page 18: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

Fifth

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Problems 6.37

• Knowing that a given vertical shear V causes a

maximum shearing stress of 75 MPa in an

extruded beam having the cross section shown,

determine the shearing stress at the three points

indicated.

6- 18

Page 19: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

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Problems 6.37

6- 19

Page 20: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

MECHANICS OF MATERIALS

Fifth

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Problems 6.38

6- 20

Page 21: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Problems 6.39

6- 21

Page 22: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Problems 6.39

6- 22

Page 23: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Unsymmetric Loading of Thin-Walled Members

• Beam loaded in a vertical plane

of symmetry deforms in the

symmetry plane without

twisting.

It

VQ

I

Myavex

• Beam without a vertical plane

of symmetry bends and twists

under loading.

It

VQ

I

Myavex

Page 24: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Unsymmetric Loading of Thin-Walled Members

• The point O is referred to as the shear center of

the beam section.

• If the shear load is applied such that the beam

does not twist, then the shear stress distribution

satisfies

FdsqdsqFdsqVIt

VQ E

D

B

A

D

Bave

• F and F’ indicate a couple Fh and the need for

the application of a torque as well as the shear

load. VehF

• When the force P is applied at a distance e to the

left of the web centerline, the member bends in a

vertical plane without twisting.

Page 25: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Concept Application 6.5

hbth

hbtbtthIII flangeweb

6

212

12

12

12

2121

233

• Combining,

mm1003

mm1502

mm100

32

b

h

be mm40e

• Determine the location for the shear center of the

channel section with b = 100 mm, h = 150 mm, and t = 4

mm

I

bth

V

h

I

Vthb

V

hFe

44

222

• where

I

Vthb

dsh

stI

Vds

I

VQdsqF

b bb

4

2

2

0 00

Page 26: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Concept Application 6.6

• Determine the shear stress distribution for

V = 10 kN

It

VQ

t

q

• Shearing stress in the web,

MPa3.18m15.0m1.06m15.0m004.02

m15.0m1.04N100003

62

43

6

42

121

81

max

hbth

hbV

thbth

hbhtV

It

VQ

• Shearing stresses in the flanges,

MPa3.13

m15.0m1.06m15.0m004.0

m1.0N100006

6

6

62

22

2121

hbth

Vb

hbth

Vhb

sI

Vhhst

It

V

It

VQ

B

Page 27: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Concept Application 6.7

6- 27

Page 28: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Problems 6.65

6- 28

Page 29: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Problems 6.66

6- 29

Page 30: Fifth SI Edition MECHANICS OF MATERIALS · MECHANICS OF MATERIALS Fifth SI Edition Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf David F. Mazurek Lecture Notes: J. Walt

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Problems 6.66

6- 30