2. Materials at High Temperature
Microstructure Change – Stability of Materials
Grain growth
Second-phase coarsening
Increasing vacancy density
Mechanical Properties Change
Softening
Increasing of atoms mobility
Increasing of dislocations mobility (climb)
Additional slip systems
3. Time-dependent Mechanical Behavior
- Creep
Creep: A time-dependent and permanent deformation
of materials when subjected to a constant load at a high
temperature (> 0.4 Tm). Examples: turbine blades, steam
generators.
6. Creep Curve
1. Instantaneous deformation, mainly elastic.
2. Primary/transient creep. Slope of strain vs.
time decreases with time: work-hardening
3. Secondary/steady-state creep. Rate of
straining is constant: balance of work-hardening
and recovery.
4. Tertiary. Rapidly accelerating strain rate up to
failure: formation of internal cracks, voids, grain
boundary separation, necking, etc.
7. Creep Curve – Constant Stress
Comparison between constant load and constant stress
8. Parameters of Creep Behavior
The stage secondary/steady-state creep is of
longest duration and the steady-state creep
rate is the most important parameter of the
creep behavior in long-life applications.
Another parameter, especially important in
short-life creep situations, is time to rupture,
or the rupture lifetime, tr.
10. Power-Law Creep
By plotting the log of the steady creep-rate ss, against log
(stress, ), at constant T, in creep curve, we can establish
ss = Bn
Where n, the creep exponent, usually lies between 3 and
8. This sort of creep is called “power-law” creep.
13. Creep: Stress and Temperature Effects
With increasing stress or temperature:
The instantaneous strain increases
The steady-state creep rate increases
The time to rupture decreases
14. Creep: Stress and Temperature Effects
The stress/temperature dependence of the steady-
state creep rate can be described by
where Qc is the activation energy for creep, K2 is
the creep resistant, and n is a material constant.
(Remember the Arrhenius dependence on temperature for
thermally activated processes that we discussed for diffusion?)
17. Larson-Miller Relation for Creep
exp( / )
ln( ) ln( )
(ln( ) ln( ))
s
s
s
A G RT
G
A
RT
G
T A
R
tan
s r
t Cons t
Since
( ln( ))
( log( ))
r
r
G
T B t
R
LMP T C t
20. Creep Relaxation
tot = el + cr (1)
But el = /E (2)
and (at constant temperature)
cr = Bn (3)
Since tot is constant, we can differentiate (1) with respect
to time and substitute the other two equations into it give
(4)
21. Creep Relaxation
Integrating from = i at t = 0 to = at t = t gives
As the time going on, the initial elastic strain i/E is slowly
replaced by creep strain, and the stress relaxes.
(5)
22. Creep Damage & Creep Fracture
Void Formation and Linkage
24. Creep Damage & Creep Fracture
Since the mechanism for void growth is the same as
that for creep deformation (notably through diffusion),
it follows that the time to failure, tf, will follow in
accordance with:
25. Creep Damage & Creep Fracture
As a general rule:
ss tf = C
Where C is a constant, roughly 0.1. So, knowing the
creep rate, the life can be estimated.
27. Creep Design
In high-temperature design it is important to make sure:
(a) that the creep strain cr during the design life is
acceptable;
(b) that the creep ductility f
cr (strain to failure) is adequate
to cope with the acceptable creep strain;
(c) that the time-to-failure, tf, at the design loads and
temperatures is longer (by a suitable safety factor) than
the design life.
28. Creep Design
Designing metals & ceramics to resist power-law creep
(a)Choose a material with a high melting point
(b)Maximize obstructions to dislocation motion by alloying
to give a solid solution and precipitates; the precipitates
must be stable at the service temperature
(c)Choose a solid with a large lattice resistance: this means
covalent bonding.
29. Creep Design
Designing metals & ceramics to resist diffusional flow
(a)Choose a material with a high melting point
(b)Arrange that it has a large grain size, so that diffusion
distances are long and GBs do not help diffusion much
(c)Arrange for precipitates at GBs to impede GB sliding.
33. Case Study – Turbine Blade
General Electric TF34 High Bypass Turbofan Engine
For (1) U.S. Navy Lockheed S-3A anti submarine warfare aircraft
(2) U.S. Air Force Fairchild Republic A-10 close support aircraft.
37. Turbine Blade Materials –
Nickel-base Superalloys
Microstructures of the alloy:
(1)Has as many atoms in solid solution as possible ( Co,
W, Cr)
(2) Forms stable, hard precipitates of compounds like
Ni3Al, Ni3Ti, MoC, TaC to obstruct the dislocations
(3) Forms a protective surface oxide film of Cr2O3 to
protect the blade itself from attack by oxygen