WS2012/13 | BSc – Introduction in Materials Science | Prof. Dr.-Ing. Frank Mücklich 1 Chair of...

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WS2012/13 | BSc – Introduction in Materials Science | Prof. Dr.- Ing. Frank Mücklich 1 Chair of Functional Materials 6. Mechanical Properties Forms of Mechanical Loading tension compression shear torsion

Transcript of WS2012/13 | BSc – Introduction in Materials Science | Prof. Dr.-Ing. Frank Mücklich 1 Chair of...

Page 1: WS2012/13 | BSc – Introduction in Materials Science | Prof. Dr.-Ing. Frank Mücklich 1 Chair of Functional Materials 6. Mechanical Properties Forms of Mechanical.

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Chair of Functional Materials

6. Mechanical Properties

Forms of Mechanical Loading

tension compression

shear torsion

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Chair of Functional Materials

6. Mechanical Properties

Stress-Strain BehaviourLinearelastic Deformation

ERobert Hooke:

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Chair of Functional Materials

6. Mechanical Properties

Stress-Strain BehaviourNonlinearelastic Deformation

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Chair of Functional Materials

6. Mechanical Properties

Force-Separation-Curve

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Potentielle Energie

Anziehungskräfte

Abstoßungskräfte

Kraft

Kernabstand

Abs-k.

Anz-k.

K

K-abst.

6. Mechanical Properties

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Chair of Functional Materials

6. Mechanical Properties

Influence of Temperature

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Chair of Functional Materials

6. Mechanical Properties

Tensile Properties of Metals(1)

vbcV cV - Konz. gleitfähiger Versetzgb – BurgersvektorV - Abgleitgschwindigkeit

Lüders-DehnungStreck-grenzen-effekt

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Chair of Functional Materials

6. Mechanical Properties

Deformation Mechanisms for MetalsBasic Concepts of Dislocations(3)

Video Versetzungsbewegung (Blasenmodell)

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Chair of Functional Materials

6. Mechanical Properties

Deformation Mechanisms for MetalsCharacteristics of Dislocations(1)

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Chair of Functional Materials

6. Mechanical Properties

Tensile Properties of Metals(3)

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Chair of Functional Materials

6. Mechanical Properties

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Chair of Functional Materials

6. Mechanical Properties

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Chair of Functional Materials

6. Mechanical Properties

Deformation Mechanisms for MetalsBasic Concepts of Dislocations(1)

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Chair of Functional Materials

6. Mechanical Properties

Deformation Mechanisms for MetalsBasic Concepts of Dislocations(2)

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Chair of Functional Materials

6. Mechanical Properties

Deformation Mechanisms for MetalsBasic Concepts of Dislocations(3)

Video Versetzungsbewegung (Blasenmodell)

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Chair of Functional Materials

6. Mechanical Properties

Effect of Temperature

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Chair of Functional Materials

6. Mechanical Properties

Tensile Properties of Metals(2)

Zugversuch CuPK.mov

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6. Mechanical Properties

True Stress-Strain-Curve

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6. Mechanical Properties

Mechanical Behaviour of Ceramics(1)

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Chair of Functional Materials

6. Mechanical Properties

Mechanical Behaviour of Ceramics(2)

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Chair of Functional Materials

6. Mechanical Properties

Mechanical Behaviour of Polymers(1)

spröde

plastisch

hoch elastischC-CH-BrückenVan der Waals

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6. Mechanical Properties

Mechanical Behaviour of Polymers(2)

PolymethylmetacrylatePMMA(Plexiglas)

E-Modul sinkt mit steigender TDuktilität steigt mit steigender T

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Chair of Functional Materials

6. Mechanical Properties

Tensile Properties of Metals(2)

Zugversuch CuPK.mov

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6. Mechanical Properties

Slip in Single CrystalsGeometrical Relationships

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Chair of Functional Materials

6. Mechanical Properties

Slip in Single CrystalsGeometrical Relationships

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Chair of Functional Materials

6. Mechanical Properties

Example

Video Gleitlinienbildung

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6. Mechanical Properties

Slip Systems in the fcc-Lattice

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6. Mechanical Properties

Slip Systems in the bcc-Lattice(1)

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6. Mechanical Properties

Slip Systems in the bcc-Lattice(2)

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6. Mechanical Properties

Slip Systems in the bcc-Lattice(3)

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6. Mechanical Properties

Slip Systems in the hcp-Lattice(3)

{1000}-[1120] →1 plane, 3 directions

{1010}-[1120] →3 planes, 1 direction

{1011}-[1120] →6 planes, 1 direction

Only few possible

slip systems!

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Slip Systems

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6. Mechanical Properties

Deformation twinning

Twin

Matrix

Anwendung in TWIP-Stählen=> Hohe Verformung + Festigkeit

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Streckgrenze [MPa]

Ver

form

bark

eit

Hochleistungswerkstoff Stahl – eine faszinierende Vielfalt

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6. Mechanical Properties

Slip Twinning

Atomic movement Lattice orientation Atoms move fractional atomic spacing.

Microscopic appearance

Thin lines Wide bands or broad lines

Lattice orientation

No change in lattice orientation. The steps are only visible on the surface of the crystal and can be removed by polishing. After polishing there is no evidence of slip.

Lattice orientation changes. Surface polishing will not destroy the evidence of twinning.

Deformation: Slip vs. Twinning

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6. Mechanical Properties

What is the maximum shear-stress ?

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6. Mechanical Properties

The shear-stress-law of Schmid

kristallographische Gleitebenedefiniert AKristallographische Gleitrichtungdefiniert Fg

Schmid-Faktor

Winkel zwischen Zug- und Gleitrichtung

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2

bGR

Dislocation Sources - The Frank-Read Source

Critical radius: R=lo/2

lo: dislocation length

0l

bGo

·b

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6. Mechanical Properties

Plastic Deformation of Polycrystalline Materials (Cu)

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6. Mechanical Properties

Plastic Deformation of Polycrystalline Materials

Requirement of five independent slip systems to realize any plastic deformation in polycrystals (Compatibility of deformation)

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6. Mechanical Properties

Plastic deformation: Single vs. polycrystal

Why such an increase of strength?

Increase due to:• Manifold of grain

orientations in polycrystals• Grain Boundaries!!!

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6. Mechanical Properties

Plastic deformationCharacteristics of Dislocations

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6. Mechanical Properties

Plastic deformation Characteristics of Dislocations

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Plastic Deformation of Polycrystalline Materials• Grains with the highest Schmid-factor deform first.• yield stress (= Streckgrenze) is reached when deformation of all grains occurs• any plastic deformation of polycrystalline materials needs activation of • 5 independent slip systems (Compatibility of deformation)

The role of Grain size

6. Mechanical Properties

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The Relation of Hall-Petch

6. Mechanical Properties

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Solid solution hardeningAlloying causes hardening effects due to three types of interactions between the dislocations and the alloyed atoms:

• Parelastic interaction distortion of the lattice; change in the lattice parameter a

• Dielastic interaction different shear modulus G of alloyed atoms compared to that of the matrix atoms

• chemical interaction

atomalloyedPar c

aGbF

_

2 ln

atomalloyedDiel c

GGbF

_

2 ln

20

1

6. Mechanical Properties

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Work Hardening

Pro

per

ty

Degree of Deformation

6. Mechanical Properties

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6. Mechanical Properties

bD

ds

The Fine-Kelly-Mechanism

particle diameter surface energy

Burgers-vector

The Orowan-Mechanism

)(dfD

bGo

shear-modulus

particle distance

Volume fraction of particles

Dispersion and precipitation hardening

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6. Mechanical Properties

Texture hardening

Strengthening effect due to:• bad orientation between applied stress and „slip system“ • morphological texture (Hall-Petch!!)

A

B

Loading in direction A shows an enhanced yield stress

compared to direction B

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Mechanisms to enhance strength

1. Plastic deformation - at lower temperatures (no recyrstallization)

2. grain refinement – Hall Petch

3. solid solution hardening – solubility and lattice distortion

4. dispersion hardening – input of highly dispers particles

5. precipitation hardening – creation of particles (solubility)

6. texture hardening (morphology, orientation and slip systems,

6. Mechanical Properties