stress analysis lecture 3 me 276 spring 2017-2018

38
Stress Analysis Lecture 3 ME 276 Spring 2017 - 2018 Dr./ Ahmed Mohamed Nagib Elmekawy

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Page 1: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress Analysis

Lecture 3

ME 276

Spring 2017-2018

Dr./ Ahmed Mohamed Nagib Elmekawy

Page 2: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Axial Stress

2

Page 3: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Beam under the action of two tensile forces

3

Page 4: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Beam under the action of two tensile forces

4

Page 5: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Shear Stress

Average Shear Stress

is the average shear stress at the section

V is internal resultant shear force at the section determined

from the equations of equilibrium

A is the area at the section

A

V

Page 6: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

A

F

A

P

Single Shear

A

F

2

Double Shear

Page 7: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

Example 1

Determine the average shear stress in the 20-mm-diameter pin at A and the 30-mm

diameter pin at B that support the beam in the attached figure.

kNAAF

kNAAF

kNFFM

yyy

xxx

BBA

200305

45.120

5.705

35.120

5.1202*3065

40

Page 8: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

The resultant force acting on pin A is

kNAAF yxA 36.21205.72222

MPa

A

F

A

AA 34

204

*2

1000*36.21

2 2

MPa

A

F

B

BB 7.17

304

1000*5.21

2

double shear

single shear

Page 9: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

Allowable Stress

• An engineer on charge of the design of a structural or mechanical

element must restrict the stress in the material to a level that will be

safe.

• So it becomes necessary to perform the calculations using a safe or

allowable stress.

• To ensure safety, it is necessary to choose an allowable stress that

restrict the applied load to one that is less than the load the member

can fully support.

• One method of specifying the allowable load for the design or

analysis of a member is to use a number called the factor of safety.

allow

failsf

..

allow

failsf

..

Page 10: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

Example 1

The control arm is subjected to the loading shown in the figure. Determine to the

nearest ¼ in. the required diameter of the steel pin at C if the allowable shear stress

for the steel is allow = 8 ksi.

Page 11: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

kipF

FM

AB

ABC

3

05*5

353*38*0

kipC

CF

x

xx

1

05

4530

kipC

CF

y

yy

6

05

3530

kipCCF yxC 082.6612222

Page 12: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Stress

in6956.0

in6956.03801.0*44

4

in3801.082

082.6

2

2

2

d

AddA

AAA

Fallow

CC

Use a pin having a diameter of

in75.04

3d

Page 13: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion Stress

13

Page 14: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion Stress

14

Page 15: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion Stress

15

Page 16: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion Stress

16

Page 17: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsional Deformation of a Circular Shaft

Page 18: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Angle of Twist

18

Page 19: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Torsion Formula

If the material is linear-elastic, then Hook’s law

applies, = G, and consequently a linear variation

in shear strain, leads to a linear variation in shear

stress along any radial line on the cross section.

J

Tcand

J

T max

Where

T the resultant internal torque acting at the cross section.

J the polar moment of inertia of the cross-sectional area.

c the outer radius of the shaft.

max the maximum shear stress in the shaft, which occurs at the outer surface.

the radius

Page 20: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Torsion Formula

4

4

32

2

d

cJ

44

44

32

2

io

io

dd

ccJ

Page 21: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Shearing Strain

21

Page 22: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torque stress summary

22

Shear Stress

𝜏 = 𝐺𝛾= 𝑇𝑟

𝐽=

16𝑇

𝜋 𝑑3

𝜏 : Shear Stress 𝑟 : shaft radius𝐺: Modulus of rigidity 𝑑 : Shaft diameter𝛾: Shear Strain𝐽 : Polar moment of inertiaFor a hollow circular shaft of inner radius c1 and outer radius c2,the polar moment of inertia is

𝐽 =𝜋

32𝑑𝑜4 − 𝑑𝑖

4

∅: Angle of Twist

Page 23: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion of a Shaft with Circular Cross-SectionFinite Element Analysis

23

Page 24: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion of a Shaft with Circular Cross-SectionFinite Element Analysis

24

Page 25: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion of a Beam with the Square Cross-SectionFinite Element Analysis

25

Page 26: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Torsion of a Beam with the Square Cross-SectionFinite Element Analysis

26

Page 27: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Torsion Formula

Example 1

The shaft shown in the attached figure is supported by two bearings and is

subjected to three torques. Determine the shear stress developed at points A and B

located at section a-a of the shaft. The shaft diameter is 75 mm.

4.25 kN.m

3 kN.m

1.25 kN.m

Torque diagram

Page 28: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Torsion Formula

MPa89.1

75032

2/750*1000*1000*25.1

4

J

TrA

MPa337.0

75032

2/150*1000*1000*25.1

4

J

TrB

Page 29: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Torsion Formula

Example 2

The pipe shown in the attached figure has an inner diameter of 80 mm and an outer

diameter of 100 mm. If its end is tightened against the support at A using a torque

wrench at B, determine the shear stress developed in the material at the inner and

outer walls along the central portion of the pipe when the 80-N forces are applied

to the wrench.

Page 30: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Torsion Formula

N.m40

02.0*803.0*80;0

T

TM y

MPa345.0

40502

50*00040

44

J

Tcoo

Page 31: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Power Transmission

MPa276.0

40502

40*00040

44

J

Tcii

The Power Transmission

Shafts and tubes having circular cross sections

are often used to transmit power developed by

a machine. When used for this purpose, they

are subjected to a torque that depends on the

power generated by the machine and the

angular speed of the shaft.

TP

Page 32: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Example 1

A solid steel shaft AB shown in the figure is to be used to transmit 3750 W from

the motor M to which it is attached. If the shaft rotates at = 175 rpm and the steel

has an allowable shear stress of allow = 100 MPa determine the required diameter

of the shaft to the nearest mm.

N.mm8.204627

60

175*2

1000*3750

T

TP

allowd

T

d

dT

J

Tc

3

4max

16

32

2

The Power Transmission

Page 33: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Angle of Twist

mm22mm843.211008.20462716

3 dd

dAngle of Twist

Occasionally the design of a shaft depends on restricting the amount of rotation or

twist that may occur when the shaft is subjected to a torque. Furthermore, being able

to compute the angle of twist for a shaft is important when analyzing the reactions on

statically indeterminate shafts.

Page 34: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Angle of Twist

J

Tand

Gdxd

;

L

dxGxJ

xTdx

GxJ

xTd

0

Constant Torque and Cross-Sectional Area

JG

TL

The similarities between the above equations

and those for an axially loaded members

should be noted.

Page 35: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Angle of Twist

The equation of angle of twist is often

used to determine the shear modulus of

elasticity G of a material. To do so, a

specimen of known length and diameter is

placed in a testing machine like shown in

the attached figure. The applied torque T

and angle of twist are then measured

along the length L.

Multiple Torques

JG

TL

Page 36: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Angle of Twist

Sign Convention

JG

L

JG

L

JG

L

JG

TL CDBCABDA

000100007000080/

Page 37: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

Example 1

The gears attached to the fixed-end steel shaft are subjected to the torques shown in

the figure. If the shear modulus of elasticity is 80 GPa and the shaft has a diameter

of 14 mm, determine the displacement of tooth P on gear A. The shaft turns freely

within the bearing at B.

The Angle of Twist

Page 38: Stress Analysis Lecture 3 ME 276 Spring 2017-2018

The Angle of Twist

rad2121.0

500*000170300*000130400*000150

0008072

1

4

JG

TLA

Since the answer is negative, by the right–

hand rule the thumb is directed toward the

end E of the shaft and therefore gear A will

rotate as shown in the attached figure.

The displacement of tooth P on gear A is

mm2.21100*2121.0 rs AP