• No results found

Mechanical Failure

N/A
N/A
Protected

Academic year: 2022

Share "Mechanical Failure"

Copied!
31
0
0

Loading.... (view fulltext now)

Full text

(1)

Unit-IV

Mechanical Failure

(2)

Mechanical failures involve a complex interaction of load, time, and environment (i.e. temperature and corrosion).

Loads may be monotonic, steady, variable, uniaxial or multiaxial.

The loading duration may range from centuries to years, as in steel bridges, or to seconds or milliseconds, as in firing a handgun.

Temperatures can vary from cryogenic with rocket motor fuels, to over a thousand degrees Celsius, with gas turbine engines.

Temperatures may be isothermal or variable.

MECHANICAL FAILURE

(3)

MECHANICAL FAILURE MODES OF METALS

Excess deformation–elastic, or yielding (i.e. onset of plasticity)

Excess deformation by yielding is probably the most commonly studied failure mode. It is based upon the maximum shear stress criterion or the octahedral shear stress criterion.

Failure by excess deformation may also be elastic such as in rotating machinery where seizure can occur.

Ductile fracture

Ductile fracture involves significant plasticity.

It is associated with high-energy absorption with fracture.

(4)

MECHANICAL FAILURE MODES OF METALS

Brittle fracture

Brittle fracture contains little plasticity.

It involves low energy absorption.

Impact or dynamic loading

Can cause excess deformation or fracture.

Impact or dynamic loading conditions that create high strain rates in metals tend to cause lower toughness and ductility.

Creep

can cause excess deformation or fracture.

In metals it is most predominant at elevated temperatures.

Example: Gas turbine engine blades due to centrifugal forces.

(5)

MECHANICAL FAILURE MODES OF METALS

Relaxation

• Relaxation is primarily responsible for loss of residual stress and loss of external load that can occur in bolted fasteners at elevated or ambient temperature.

Thermal shock

• Thermal shock tends to promote cracking and/or brittle fracture.

• Example: quenching operation during heat treatment of metals.

(6)

MECHANICAL FAILURE MODES OF METALS

Wear

Can occur at any temperature and include many possible failure mechanisms.

Dominant in roller or taper bearings and in gear teeth surfaces.

Buckling

Buckling failure can be induced by external loading or by thermal conditions.

Can involve elastic or plastic instabilities.

Most dominant in columns and thin sheets subjected to compressive loads.

(7)

FRACTURE

Fracture: separation of a body into pieces due to stress, at temperatures below the melting point.

Steps in fracture:

crack formation

crack propagation

Depending on the ability of material to undergo plastic deformation before the fracture two fracture modes can be defined - ductile or brittle

• Ductile fracture - most metals (not too cold):

Extensive plastic deformation ahead of crack

Crack is “stable”: resists further extension unless applied stress is increased

Brittle fracture - ceramics, ice, cold metals:

Relatively little plastic deformation

Crack is “unstable”: propagates rapidly without increase in applied stress

(8)

Brittle vs. Ductile Fracture

Ductile materials - extensive plastic deformation and

energy absorption (“toughness”) before fracture

• Brittle materials - little plastic deformation and low

energy absorption before fracture

(9)

Brittle vs. Ductile Fracture

A. Very ductile, soft metals (e.g. Pb, Au) at room

temperature, other metals, polymers, glasses at high

temperature.

B. Moderately ductile fracture, typical for ductile metals

C. Brittle fracture, cold metals, ceramics.

A B C

(10)

Ductile Fracture (Dislocation Mediated)

Crack grows

90degreeto applied stress

45degree-Maximum

shear stress Cup-and-cone

fracture (a) Necking

(b) Formation of microvoids

(c) Coalescence of microvoids to form a crack

(d) Crack propagation by shear deformation

(e) Fracture

(11)

Brittle Fracture (Limited Dislocation Mobility)

• No appreciable plastic deformation

• Crack propagation is very fast

• Crack propagates nearly perpendicular to the

direction of the applied stress

• Crack often propagates by cleavage - breaking

of atomic bonds along specific crystallographic

planes (cleavage planes).

(12)

Brittle Fracture

A. Transgranular fracture:

Fracture cracks pass through grains. Fracture surface have faceted texture because of different orientation of cleavage planes in grains.

B. Intergranular fracture:

Fracture crack propagation is along grain

boundaries (grain boundaries are weakened or

embrittled by impurities segregation etc.)

(13)

PRINCIPLES OF FRACTURE MECHANICS

• The measured fracture strengths for most materials are significantly lower than those predicted by theoretical calculations based on atomic bonding energies. This

discrepancy is explained by the presence of microscopic flaws or cracks that always exist under normal conditions at the surface and within the interior of a body of

material. These flaws are a detriment to the fracture strength because an applied stress may be amplified or concentrated at the tip, the magnitude of this

amplification depending on crack orientation and

geometry. This phenomenon is demonstrated in Figure a

(14)

14

Crack Propagation

Cracks having sharp tips propagate easier than cracks having blunt tips

A plastic material deforms at a crack tip, which

“blunts” the crack.

deformed region

brittle

Energy balance on the crack

Elastic strain energy-

energy stored in material as it is elastically deformed

this energy is released when the crack propagates

creation of new surfaces requires energy ductile

(15)

15

Fracture Toughness Ranges

Based on data in Table B.5, Callister & Rethwisch 8e.

Composite reinforcement geometry is: f

= fibers; sf = short fibers; w = whiskers;

p = particles. Addition data as noted (vol. fraction of reinforcement):

1. (55vol%) ASM Handbook, Vol. 21, ASM Int., Materials Park, OH (2001) p. 606.

2. (55 vol%) Courtesy J. Cornie, MMC, Inc., Waltham, MA.

3. (30 vol%) P.F. Becher et al., Fracture Mechanics of Ceramics, Vol. 7, Plenum Press (1986). pp. 61-73.

4. Courtesy CoorsTek, Golden, CO.

5. (30 vol%) S.T. Buljan et al., "Development of Ceramic Matrix Composites for Application in Technology for Advanced Engines Program", ORNL/Sub/85-22011/2, ORNL, 1992.

6. (20vol%) F.D. Gace et al., Ceram. Eng. Sci.

Proc., Vol. 7 (1986) pp. 978-82.

Graphite/

Ceramics/

Semicond Metals/

Alloys

Composites/

fibers Polymers

5

K

Ic

(M P a · m

0.5

)

1

Mg alloys Al alloys

Ti alloys Steels

Si crystal Glass -soda Concrete

Si carbide

PC

Glass6

0.5 0.7 2 4 3 10 20 30

<100>

<111>

Diamond

PVC PP

Polyester PS

PET

C-C(|| fibers) 1

0.6 67 40 5060 70 100

Al oxide Si nitride

C/C( fibers)1 Al/Al oxide(sf) 2

Al oxid/SiC(w) 3 Al oxid/ZrO 2(p)4

Si nitr/SiC(w) 5 Glass/SiC(w) 6 Y2O3/ZrO2(p)4

(16)

Baldwin Hydraulic Machine for Tension & Compression test

(17)

Click START Tensile Test

(18)

Elastic Region:

•This is the region where stress is proportional to strain

Tensile Test

(19)

Yielding Region:

•Upper yield point is where when there is no

application of any additional force the material will elongate.

Tensile Test

(20)

Lower yield point :

•This is the point where yielding will end .

Tensile Test

(21)

Proportionality region:

•This is the region where stress is proportional to strain.

Tensile Test

(22)

Ultimate Tensile Strength:

•The maximum loading occurs in this region.

Tensile Test

(23)

Necking:

•Fracture of material occurs by reduction of area.

Tensile Test

(24)

The failure of specimen used in tensile testing for ductile material is by necking .

The failure is a cup and cone failure

Failure Analysis

(25)

Charpy Izod

Energy ~ h - h’

Impact Fracture Testing

(testing fracture characteristics under high strain rates)

(26)

Charpy V-Notch Test:

- Charpy test is an impact toughness measurement test because the energy is absorbed by the specimen very rapidly.

- The potential energy of the pendulum before and after impact can be calculated form the initial and final location of the pendulum.

- The potential energy difference is the energy it took to break the material absorbed during the impact.

- Purpose is to evaluate the impact toughness as a function of temperature

Material Properties

(27)

Temperature (°F)

C ha rp y T ou gh ne ss (l b· in )

Brittle

Behavior

Ductile Behavior Transition Temperature

Material Properties

Charpy V-Notch Test:

(28)

Charpy V-Notch Test:

- At low temperature, where the material is brittle and

not strong, little energy is required to fracture the material.

- At high temperature, where the material is more ductile and stronger, greater energy is required to fracture the material

-The transition temperature is the boundary between brittle and ductile behavior.

The transition temperature is an extremely important parameter in selection of construction material.

Material Properties

(29)

High Carbon Steel Stainless Steel Charpy V-Notch Test:

(30)

Example:

Mooring line length =100 ft diameter=1.0 in

Axial loading applied=25,000 lb

Elongation due to loading=1.0 in mooring line

loading 1) Find the normal stress.

2) Find the strain.

2 2

2

2

785 .

0 )

(0.5 r

A

800 ,

31 785 .

0

000 ,

25

in in

in psi lb A

F

) / ( 00083 .

0 1

100 12

1 in in

ft ft in

in L

e

o

(31)

Example:

- Salvage crane is lifting an object of 20,000 lb.

- Characteristics of the cable

diameter=1.0 in, length prior to lifting =50 ft 1) Find the normal stress in the cable.

2) Find the strain.

3) Determine the cable stretch in inches.

)

785 .

0 )

(0.5 r

(A

478 ,

25 785 .

0

000 ,

20

2 2

2 2

in in

in psi lb A

F

) /

( 000728 .

0 10 35

478 ,

25

6 in in

psi psi

E

 

psi 10

35

psi 000 ,

70

psi 000 ,

60

6 UT

E

y

ft in ft in

in in

L e

L e

o o

44 . 0 1 )

50 12 ( ) / 000728 .

0

(   

References

Related documents

SEM micrographs of impact fracture surfaces showing (a) networks of fine ductile dimples in OQ condition (1⋅25 kX), (b) predominantly quasi cleavage pattern and large microvoids

The role of strain-rate dependence on ductile crack Initiation at high loading rates, and the specimen geometry effect on the variation of dynamic

This is to certify that the thesis entitled &#34;Analysis of Some Indentation Models related to Incipient Deformation of Brittle and Ductile Workmaterials during Orthogonal

In order to confirm the above assertion, the plastic zone (which is defined here as the contour of macroscopic equivalent stress a, = O-o) is shown in figure 4 corresponding to a

In this paper the various aspects of dynamic plastic deformation and fracture of common engineering materials are reviewed and contrasted with their behaviour under static

A fracture criterion based on critical plastic strain has been imposed to obtain (theoretically) the variation of dynamic fracture toughness with crack speed, when

The objective of this thesis is to derive a single finite element material model for long bones, which can predict both mechanical response as well as the different fracture

The strain field analysis has revealed the stress wave propagation to outer plastic deformation zones (OPDZ) from the inner fracture process zones (IFPZ) as the