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Lecture Strength of Materials I: Chapter 4 - PhD. Tran Minh Tu

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• Shear Stress: positive: the direction associated with its subscripts are plus-plus or minus-minus; negative: the directions are plus-minus or minus-plus. 4.2[r]

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STRENGTH OF MATERIALS

TRAN MINH TU -University of Civil Engineering, Giai Phong Str 55, Hai Ba Trung Dist Hanoi, Vietnam

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4

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Contents

4.1 State of stress at a point 4.2 Plane Stress

4.3 Mohr’s Circle

4.4 Special cases of plane stress 4.5 Stress – Strain relations

4.6 Strength Hypotheses

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4.1 State of stress at a point K x y z n  

• External loads applied to the body => The body is deformed =>The stress is occurred

• At a point K on the arbitrary section, there are types of stress: normal stress s and shearing stress t

• The state of stress at a point K is a set of all stresses components acting on all sections, which go through this point

• The most general state of stress at a point may be represented by components,

, , , , , , ) normal stresses shearing stresses (Note:

x y z xy yz zx

xy yx yz zy zx xz

s s s t t t

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Principal planes: no shear stress acts on

4.1 State of stress at a point

Principal directions: the direction of the principal planes

Principal stresses: the normal stress act on the principal plane

• There are three principal planes , which are perpendicular to each other and go through a point

• Three principal stresses: s1, s2, s3 with: s1 ≥ s2 ≥ s3

• Types of state of stress:

- Simple state of stress: of principal stresses equal to zeros

- Plane state of stress: of principal stresses equal to zeros

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Plane Stress – the state of stress in which two

faces of the cubic element are free of stress For the illustrated example, the state of stress is defined by

. 0 ,

, y xy and zzxzy

x s t s t t s

• State of plane stress occurs in a thin plate subjected to the forces acting in the mid-plane of the plate

4.2 Plane Stress

sx

txy

sy

y

tyx x

y

sx

txy

sy

O

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Sign Convention

Normal Stress: positive: tension; negative: compression

Shear Stress: positive: the direction associated with its subscripts are plus-plus or minus-minus; negative: the directions are plus-minus or minus-plus

4.2 Plane Stress

y

4.2.1 Complementary shear stresses

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0

u

F  

2

2

cos cos sin sin sin cos

u x xy

y yx

A A A

A A

s s  t  

s  t  

 

  

 su >0 pull out

 t uv - clockwise

2

uv xy x

τ A - τ Acos α - σ Acosαsinα

v

F  0

x y sx txy sy O u

styyx sxv

u

A

A sin

su tuv

txy

4.2 Plane Stress

4.2.2 Stresses on Inclined Planes

Sign Convention

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1/10/2013 4.2 Plane Stress

tyx

sy

su

tuv

sy sx

txy

4.2.2 Stresses on Inclined Planes

x y

v u

-  > 0: counterclockwise from the x axis to u axis

x y x y

u cos xy sin s s s s

s     2 t 2

2 2

x y

uv sin 2 xy cos 2

2 s s

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4.2 Plane Stress

4.2.3 Principal stresses are maximum and minimum stresses

By taking the derivative of su to  and setting it equal to zero:

xy u p x y 2 d

0 => tg2 =-d

t

s 

  s s

2

2 1,2(3)

2 2 xy

x y x y

max, min

s s s s

s  s       t

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