Unified Engineering
Lecture M21 12/2/2003
Materials Selection
Objective
Aim to provide coherent overview of material selection
Materials (and structural configurations and processes)
should be selected for applications based on
measurable criteria
Key Ideas
It is possible to compare the suitability of materials for a
given application according to quantifiable performance
metrics based on material properties
Properties (such as Youngs modulus, density,
strength) quantify material performance
Some materials properties are more invariant than others
Role of scale, role of manufacturing, microstructure
Fiber composite allow flexibility
Important to know what you can change - or not!
Central Problem - Interaction of
Function, Material, Process and Shape
Function
Transmits loads, heat
resonates, contains pressure
stores energy etc.
At minimum weight, cost, size,
or maximum efficiency,
safety etc.
(rest of Unified)
Material
Shape
Process
References
Material Selection in Mechanical Design, M.F Ashby,
Pergamon Press, Oxford, 1992
Ashby and Jones, Engineering Materials I, Chapter 6
Materials for Mechanical Elements
- performance indices
Design of a structural element is specified by three
parameters, or groups of parameters (performance
indices):
Functional requirements (F), Geometry (G) and
Material Properties (M)
We can quantify the interdependence if we can specify
performance, p, as a function of F, G and M:
p = f(F, G, M)
We can simplify further if the three groups of parameters
are separable, i.e:
p = f1(F) . f2(G) . f3(M)
Ex: Lightweight stiff rod - tensile load
A
L
Material, modulus E, density r - note these are a property of
the material, and cannot be independently selected
Mass of rod given by
m = rAL
P AE
Stiffness of rod, given by
k= =
d
L
Combining, by eliminating free variable, A:
kL2 r
2 r
m=
= kL
E
E
FG M
Choose material with low r/E ratio!!!
MATERIAL SELECTION FOR A
MICROMECHANICAL RESONATOR
Fatigue test device
(Courtesy of Stuart Brown.
Used with permission.)
Example 2 - High f Beam Resonator
d = A0 sin wt
L
Material, modulus E, density r
pr 4
I=
4
Natural (resonant) frequency, f
E r
EI
Er 2
b n = f ( B.C' s)
f
b
=
b
1
2
r
L2
rL4
ML3
For high frequency resonator select high E/r
Note frequency
1
f
L
for given
r
implies scale effect
Choose material with low r/E ratio,
MEMS allow high frequencies
MODULUS - DENSITY RATIOS OF
SOME MEMS MATERIALS
Material
Density, r,
Modulus, E,
E/ r
Kg/m3
2330
GPa
165
GN/kg-m
72
Silicon Oxide
2200
73
36
Silicon Nitride
3300
304
92
Nickel
8900
207
23
Aluminum
2710
69
25
Aluminum
Oxide
Silicon Carbide
3970
393
99
3300
430
130
Diamond
3510
1035
295
Silicon
Silicon performs well, diamond, SiC and SiN significantly better
DEFLECTION OF CIRCULAR PLATE
0.67 mga
d=
p Et 3
m = pa tr
2a
mg
The elastic deflection of a telescope mirror (shown as a flat disc), under its own weight.
(Adapted from Ashby.)
12
0.67 / g
m =
r 3 1 2
4
pa
E
r
M=
E
Example 3 - Telescope Mirror
Choose materials with high
r3
M=
E
The distortion of the mirror under its own weight can be corrected
by applying forces to the back surface. (Adapted from Ashby.)
MODULUS - DENSITY PROPERTY MAP
Note contours
of equal performance
Ashby
STRENGTH-MODULUS PROPERTY MAP
Might also want
Deflection at
minimum force polymers would
appear more
attractive
Ashby
STRENGTH-DENSITY MAP
Ashby
CTE-THERMAL CONDUCTIVITY
Ashby
CTE-MODULUS MAP
Determines thermal
stress, thermal
buckling limits for thin
tethers,
also
Feasibility of thermal
actuation
Ashby
SUMMARY
Aimed to provide coherent overview of material selection
Materials (and structural configurations and processes)
should be selected for applications based on
measurable criteria
Often combinations of material properties
Material properties group according to class of material
Metal, ceramic, polymers
Engineered materials (composites, foams)
Natural materials (wood, bone, etc)
