Task 6 - Safety Review and Licensing On the Job Training ...

47
Task 6 - Safety Review and Licensing On the Job Training on Stress Analysis Pisa (Italy) June 15 – July 14, 2015 Static strength and High and Low-Cycle Fatigue at room temperature 1/2 Davide Mazzini – Ciro Santus

Transcript of Task 6 - Safety Review and Licensing On the Job Training ...

Page 1: Task 6 - Safety Review and Licensing On the Job Training ...

Task 6 - Safety Review and LicensingOn the Job Training on Stress Analysis

Pisa (Italy)June 15 – July 14, 2015

Static strength and High and Low-Cycle Fatigueat room temperature 1/2

Davide Mazzini – Ciro Santus

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Teaching

Fundamental of Machine Design (Bachelor, Mechanical Engineering)

Computer-Aided Engineering, FE (Master, Mechanical Engineering)

Research

Fatigue of Materials and Structures

Contact Mechanics

Dynamics

Pisa, June 15 – July 14, 2015

Prof. Ciro Santus

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3Pisa, June 15 – July 14, 2015

My latest paper – Eng. Fr. Mechanics, Elsevier

Flange leakage pressure deduced from a Weight Function application

Validations:- FE- Exper.

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4Pisa, June 15 – July 14, 2015

Other paper – Eng. Fr. Mechanics, Elsevier

Analytical/ Numerical procedure to calculate the Stress Intensity Factors for Rolling Contact Fatigue

FE validation

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Content

• Static strength of metals, Ductile/ Brittle

- Tensile test

- Plastic collapse vs. Brittle fracture notched components

• Fatigue of metals

- Stress/ Strain approaches

- Low/ High Cycle Fatigue

- Fatigue notch sensitivity

Table of content – Class VI.a.1

Pisa, June 15 – July 14, 2015

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Books on Material mechanical properties

W. D. Callister, D. G. Rethwisch. Fundamentals of Materials Science andEngineering An Integrated Approach. Wiley 2007.

N. E. Dowling. Mechanical Behavior of Materials. Prentice Hall 1999.

Books specifically on Fatigue

S. Suresh. Fatigue of Materials. Cambridge University Press 1998.

H. E. Boyer. Atlas of Fatigue Curves. ASM International 2003.

… and many many others

Books

Pisa, June 15 – July 14, 2015

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Metals

FCC – Face Centered Cubic BCC – Body Centered Cubic

Pisa, June 15 – July 14, 2015

Most usual metal crystal structures

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Dislocation mechanics

Metals

The dislocation mobility is the basic for

Metals ductility

Pisa, June 15 – July 14, 2015

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Dislocation interactions

Other dislocation previousy accumulated → work hardening

Other defect → alloy composition

Grain boundaries → heat treatment

Dislocation Mechanics

Pisa, June 15 – July 14, 2015

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Static, quasi-static, or monotonic tests

Tensile tests

Hardness tests

Fracture Toughness tests

Charpy tests

… and others

Mechanical tests on materials

Pisa, June 15 – July 14, 2015

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Specifications

Uniform section of the specimen

Imposed constant (low) Strain rate up to fracture

Measurements:

Load Cell and

Extensometer Displacement

Material properties tested

Bulk strength “without any gradient” (unnotched specimen)

Ductility up to fracture

Tensile test

Pisa, June 15 – July 14, 2015

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ASTM Standard E8/E8M – 11

Definition of the test, specimen sizes, recommendations, etc.

Tensile test

Pisa, June 15 – July 14, 2015

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ASTM Standard E8/E8M – 11

Specimen:

- Flat specimen

- Round specimen

Tensile test

Pisa, June 15 – July 14, 2015

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ASTM Standard E8/E8M – 11

Specimen:

- Flat specimen

- Round specimen

Tensile test

Most used

20 0

Initialsection and lenght:

,4

A D L G

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Tensile test

Linear elasticbehavior

Elastic-plastic,post yield

YS

0.2%

US

FS

NeckingPost necking

Final Fracture

0

LL

F

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0

FA

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Tensile Test – definitions

0

0

Y U F

F

Load as measured by the load cellElongation as measured by theextensometer

Engineeringstress

Engineeringstrain

(before yield) Young's modulus

, , Yield, Ultimate, Fracture strength valuesEl

FL

FAL

L

E

S S S

ongation at Fracture (usually in %)

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Tensile Test – definitions

Yield point

Low-carbon steel, C 0.05-0.15%Mild/ high-carbon steel, C≥0.2%And all the other metals

Yield point

Conventional Yield(at 0.2% offset)

0.2%

Line parallelto the elastic

Pisa, June 15 – July 14, 2015

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Tensile Test – True curve

Engineering/ True curve

0 0

, Engineering, True

Ais thecurrent area

d+...=

Before necking:(1 )ln(1 )

FAL L L

L L L L

Pisa, June 15 – July 14, 2015

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Tensile Test – True curve

After necking

is no more uniform,the test redportio

uces to aof thesp nn ecime

A

A

Pisa, June 15 – July 14, 2015

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Tensile Test – True curve

True curve Stress/ Strain at final fracture

f

0F F

F

0F

F

F

0 F

0

At least at fracture is known:

ln

Instead of ,Reduction of Area

% 100

AASA

AA

A ARAA

f

(measuredafter fracture)

A

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Example

0 5 10 150

200

400

600

800

1000

1200

Strain, %

Stre

ss, M

Pa

exp. data0.2% Yield line0.2% Yield StrengthUltimate Tensile StrengthFracture

AISI 4340, Engineering

E

F F,S

US

YS

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0 10 20 30 40 50 600

200

400

600

800

1000

1200

1400

Strain, %

Stre

ss, M

Pa

EngineeringTrue

Example

AISI 4340, True

F F,

Linear interpolationfrom Necking pointto Fracture point

Pisa, June 15 – July 14, 2015

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Homework

Write a MATLAB script to find both Engineering and True curve

and find the Stress and elongation parameters

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YouTube video

https://www.youtube.com/watch?v=NrIErdXvjRQ

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Why does the Necking happen?

SU is not a strength parameter, Necking is a point of instability onset

d d dd d d

At necking d / d 0 :d dd d

After necking d /predominant until fr

d is

thusact

d 0ure

d /

F AF AAt t t

F tAA

t tA t

F t

Positive Negative

Weakest linkIt goes into NeckingChain model of the

tensile specimen

The other links experience unloadingbefore reaching their necking condition, so necking does not extend to the stronger links

Pisa, June 15 – July 14, 2015

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Necking on the entire specimen

Other materials (not metal) may have necking distributed

on the entire specimenAt necking d / d 0 :d dd d

After necking d / d is predominantthus the load drops, but

db

predomin

efore fracture, becomesd

again so neckingextends to the entire speci

ante

m n

F tAA

t tA t

t

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Tempering after quenching at different temperatures (Es. AISI 4340)

Steel - Different mechanical properties

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Hardness tests

Resistance to the penetration / scratch

Different mechanical properties

Pisa, June 15 – July 14, 2015

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Different mechanical properties

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Hardness tests

Differences with respect to the Tensile test:

• Compressive rather than Tensile

• Plastic deformation and No fracture

• Multiaxial (stress) instead of Uniaxial

• Small surface portion of material instead of

bulk material

• Result dependent on the Standard definition

of load and indenter size

Different mechanical properties

U

Nevertheless alinear relationshipis remarkably accurate(only for steels):

3.45HBS

Pisa, June 15 – July 14, 2015

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Metals can be (broadly) distinguished into:

- Ductile, elongation at fracture > 5%

- Brittle, elongation at fracture < 5%

Usually brittle metals do not

reach the Necking

Ductile - Brittle

0 1 2 3 4 50

500

1000

1500

2000

2500

Strain, %

Stre

ss, M

Pa

Example: Quenched steel

F F,S

Pisa, June 15 – July 14, 2015

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Different criteria for Ductile/ Brittle metals

- Ductile:

- Plastic collapse

- Ductility exhaustion

- Brittle:

- Fracture

Ductile - Brittle

Pisa, June 15 – July 14, 2015

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Notched geometry

Stress Concentration – Force flux

Central hole in a plate

Stress concentrates at the notch apexeither a circle or any other concave shape

Pisa, June 15 – July 14, 2015

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Notched geometry

n 0

max

maxt

Nominalstress: , , (force/area)

Maximumstress: (peak value)

SCF:

K

Stress Concentration Factor

Central hole in a plate

Pisa, June 15 – July 14, 2015

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Notched geometry

maxtK

Stress Concentration Factor

Central hole in a plate

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Notched geometry

Stress Concentration Factor

Many tables and graph for several cases

Pisa, June 15 – July 14, 2015

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Ductile metal

Plastic collapse

Elastic perfectly plasticallyModel

Different stagesof the load

F

timePlasticity onset

Plastic collapse

ab

cd

Pisa, June 15 – July 14, 2015

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Ductile metal

Plastic collapse

YF ASAt plastic collapse the ultimate force does not depend on theStress Concentration Factor

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Ductile metal

Ductility exhaustion

The fracture could happen before the Plastic Collapse, if the strain reaches the (true) elongation at fracture

max

F

max F ?

How tocalculate ?

Plasticity zone spreading out

Fracture for ductility exhaustion

Pisa, June 15 – July 14, 2015

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Ductile metal

The Neuber’s rule (1946)

, el el

tt

2t( )

nominalstress

K SK SE

K SE

S

After imposing equal the (triangular) areas it follows:

Any kind of (radiused)notch

el el,

Pisa, June 15 – July 14, 2015

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Ductile metal

The Neuber’s rule (1946)

2t( )K SE

ElastAny ma

ic peterial mode

rfectly plla, suchsti

ascally

Neuber’shyperbola

YS

Pisa, June 15 – July 14, 2015

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Ductile metal

Plastic collapse/ Neuber’s rule example

Y

t

Steel Fe360-S235235MPa

205GPa% 50%

5.0(anyshape)

SERAK

Plas

Byin

tic

creasing

collapse

the load,what happ

Ductility e

ens first:or

xhaustion?

Pisa, June 15 – July 14, 2015

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Ductile metal

Plastic collapse/ Neuber’s rule example

Y

t

Steel Fe360-S235235MPa

205GPa% 50%

5.0(anyshape)

SERAK

F

Y

2t

max max

1ln 0.691 % /100

Assuming to have plastixccollapse first:

Neuber:

RA

S

KE

Pisa, June 15 – July 14, 2015

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Ductile metal

Plastic collapse/ Neuber’s rule example

Y

t

Steel Fe360-S235235MPa

205GPa% 50%

5.0(anyshape)

SERAK

max Y

max2t Y

max

max F

then,assuming elastic prefectlyplastic material model:

finally, can besolved:

0.029

beingplasticcollapse happens first

S

K SE

Pisa, June 15 – July 14, 2015

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Ductile metal

Plastic collapse/ Neuber’s rule example

Y

t

Steel Fe360-S235235MPa

205GPa% 50%

5.0(anyshape)

SERAK

Y F

t

Homework:1.What if a different steel is considered:

1700 MPa and 0.08

2.Which is the(minimum) to haveductilityexhaustion first?

S

K

Pisa, June 15 – July 14, 2015

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Brittle metal

The maximum stress just induces fracture

0 1 2 3 4 50

500

1000

1500

2000

2500

Strain, %

Stre

ss, M

Pa

F F,S

max t F

Fracture:K S

No more margindue to ductility

The SCF has a direct effect on fracture.Ductile metals are usually preferred than Brittle

Pisa, June 15 – July 14, 2015

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Ductile/ Brittle metal

Different levels of stress concentration severity

Ductile,blunt notchPlasticcollapse

Brittle,blunt notchFracture

Ductile,sharp notchPlasticCollapse orDuctility exhaustion

Brittle,sharp notchFracture

tK

tK

tK

tK

Ductile,Crack notchHow to predict the strength?

Brittle,Crack notchHow to predict the strength?

tK

tK

r r 0

Pisa, June 15 – July 14, 2015