Defects in Solids 0-D or point defects –vacancies, interstitials, etc. –control mass diffusion...
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Transcript of Defects in Solids 0-D or point defects –vacancies, interstitials, etc. –control mass diffusion...
Defects in Solids• 0-D or point defects
– vacancies, interstitials, etc.
– control mass diffusion
• 1-D or linear defects– dislocations
– control deformation processes
• 2-D or planar defects– grain boundaries, surfaces, interfaces,
– heterophase boundaries
• 3-D or volume defects– voids, secondary components (phases)
(mechanical properties – yield, metals)
(mechanical props – fracture, ceramics)
Volume Defects / Heterophase Boundaries
• Composites– Two or more distinct types of materials, “phases”– Boundary between them is a heterophase interface
A
B
• At grain boundaries– Second phase concentrated at triple
contacts of host grain boundaries– Typical when liquid phase forms at
high temperature
liquid / amorphous
grain 1grain 3
grain 2
Balance of forces
interphase boundary
SS
LS LS
SS = 2SLcos(/2)
• Pores– 2nd phase is a void– increases scattering– thermal insulation– white, not transparent
Volume Defects and Mechanics• A secondary (different) material: “phase”
– in metals: secondary phases tend to pin dislocations
• Pores– in ceramics: tend to be source of failure
= F/A
= L/L
ceramic
metal
Mechanical Behavior
y
frac
Y
Y
Y – from chemical bonds
y – due to dislocation glide
y (obs) << y (theo)
frac – due to volume defects
frac (obs) << frac (theo)
F
F
L
x
“graceful” failure
“catastrophic” failure
Evaluate frac(theoretical)
F = dE/dR
attr
activ
ere
puls
ive
F
RR0
ER (interatomic distance)
E0
R0
bond energy curve
bond force curve
= F/A
theofrac
approximate as sinusoidal
x
th
2πsinth
x
R0 ~ a0
0
xY
a
linear region: Y
2π~ th
x 0
xY
a
02πth
Y
a
fracture plane
F
F
???
/2
x = 0
simultaneous failure
0
RY
R
Evaluate frac(theoretical)
02πth
Y
a
1. ~ ao 2πth
Y
2. Obtain by equating mechanical energy (work) of creating two surfaces to their surface energy
a0
th
/2
x = 0
x
E Fdx /E area dx2
0
2π/ sinth
xwork area dx
πth
surface energy / area of fracture = 22 π
th
2 π
2πtho th
Y
a
12
tho
Y
a
Griffith’s equation If some plastic deformation occurs:
eff = surf + plastic
Evaluate frac(observed)1
2
0
~obs thfrac frac
Y
a
Stress concentration at crack tips
12
2tip app
c
1122
2 appo
c Y
a
Why??
2c only this region of the material supports the load
can show:radius of curvature
take fracture to occur when:th
tip frac
12
4appo
Y
a c
obsfrac ao
12
4obsfrac
Y
c
in general:½obs
frac c
measured fracture stress is not an “inherent” material property
= F/A
inte
rnal
forc
e lin
es
atomically sharp crack tip
Evaluate frac(observed)
Alternative derivation: again, consider energy balance
0( )E c E
+ surface energy
take fracture to occur when: c > c*obsfrac
122
πobsfrac
Y
c
as before:½obs
frac c
measured fracture stress is not an “inherent” material property
= initial energy
- released strain energy
22π0 4
E c
c Y
E(c)
c
energy per unit thickness
crack length
crack energy
c*
2 2π c
Y
4c
2c
Mechanical Properties• Elastic properties
– depend on chemical bonding, not so sensitive to slight variations in composition, processing
• Yield stress (metals)– depends on details of processing– fairly reproducible
• Fracture stress (ceramics)– an almost meaningless property– depends on details of crack/pore distribution– achieving reproducibility is a major effort
Fracture Behavior• In general:
@ failure:
custom:
not @ failure:
K, KC units: pressure (length)½
in practice, need to specify geometry of the experiment
shear vs. tension, etc. geometric constant
characterization: put in a crack of known length and defined geometry
½,geometrytip app appf c kc
½frac fractip app kc
½
theofracobs
frac kc
½ ½(π ) (π )
theofracobs C
frac
K
k c c
fracture toughness
stress intensity factor
critical stress intensity
indep. of geometry depends on crack length
depends on geometry
theofrac
k
To strengthen ceramics, pay attention to cracks
½)π( cK appl
½(π )obsC fracK c
molten potassium
salt
Strengthening of Ceramics• Process to eliminate cracks (internal)• Polish to eliminate surface cracks• Blunt crack tip• Anneal (heat treat) to eliminate randomly
distributed internal stresses• Quench (a silicate glass) to induce
compressive stress on surface• Ion exchange to induce surface compressive
stress
tension
compression
tension
compression
NaO*SiO2
K
Na
once crack penetrates compressive region, material shatters explosively
Strengthening of Ceramics• Transformation toughening
• Cool ZrO2: cubic tetragonal monoclinic
• Modify with CaO: cubic tetragonal monoclinic + cubic
• Rapid cooling: tetragonal monoclinic is slowobtain tetragonal + cubic
cubic
tetragonal
crack catalyzes tetragonal monoclinic transition
increase in volume upon transition
V places compressive stress on crack (closes it)