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Lecture 12, 2015.
Design of Composites / Hybrid Materials, or
Filling Holes in Material Property Space (2/2)
Textbook Chapter 12, Tutorial 6
Papers:
Microtruss core 1
Microtruss core 2
Foam Topology
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Hybrid Materials: four families of configurations
Composite
Sandwich
Lattice
Segment
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Review: Fibre and particulate composites: the math
Rule of
mixtures
Reuss’
bound
Voigt’s
bound
Possible Mg-matrix fibre reinforced composites
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Reuss'
bound
Voigt's
bound
E1/2/(criterion of excellence
for beams)
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Hybrid Materials: four families of configurations
Composite
Sandwich
Lattice
Segment
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Hybrid Materials of Type 2: Sandwich Panels
Strong/stiff faces
carry most of the load
(flexural stiffness)
Core is
lightweight,
Resists shear
Rule of mixtures for density
Fibre composites Sandwich panels
Rule of mixtures for stiffness
Fibre composites (tension) Sandwich panels (bending)
equivalentflexural modulus (P.320)
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A Sandwich Panel as a Monolithic Material: the Maths
f = 2t/d
E face
face
c = t – d, Ec ~0c = t – d, Ec ~0
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The efficiency of Sandwich Structures: S/W Panels vs Monolithic Materials
E1/3/
face
core
Optimum
at f = 0.04
E
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Hybrid Materials: four families of configurations
Composite
Sandwich
Lattice
Segment
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Hybrid Materials of Type 3 and 4:
Cells, Foams and Lattices & Segmented structures
There are two main types of Lattices:
Bending dominated and Stretch dominated
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Bending dominated structures
Cable Leaf
spring
We use Shaping to give the sections a LOWER flexural stiffness
per kg than the solid sections from which they are made.
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Bending dominated structures: Foams
F
F
F
F
Very flexible structure = low effective E*
Prove this
Prove:
Proportionality
constant of
order 1
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metallic foam
(plastic hinges)
elastomeric
foam
(elastic
buckling)
ceramic foam
(hinges crack)
Collapse of foams
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Stretch dominated structures
flexible over-constrainedrigid
bending-dominated
(mechanism)stretch-dominated structures
2D lattice
3D lattice
b for beams
j for joints
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Stretch dominated structures:
A micro-truss structure
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Micro-truss core designs for panels and towers
http://www.cellularmaterials.com/coredesigns.asp
Periodic cellular material cores are based on a regularly repeating
geometric unit, or cell, like a cube (square honeycomb) or pyramid.
This technology allows for consistently spaced open-cells, which
facilitate the addition of materials like magnets, cables, or ceramics,
for example and therefore increase functionality. The open cells also
permit fluid flow that can achieve more efficient thermal management.
Communications Tower
Guangzhou City
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http://etd.gatech.edu/theses/available/etd-11222005-162952/unrestricted/wang_hongqing_v_200512_phd.pdf
http://www.srl.gatech.edu/publications/2005/DETC2005-85366.pdf
Bone = Foam (bending dominated) or
= Micro-truss (stretch dominated)?
A foam in a panel’s core behaves like a micro-truss structure:
shear stretches the diagonals of the cell walls, whereas the
panel’s faces are under “stretching” stresses. (See the bubble
charts in slides 28-29 later on)
(Zhang et al, 2015) Distribution of local strains. Stretched in tension by Mg-La (30% solid) (a) ~0.4% and (b) ~0.6% strain and (c) ~0.8% strain.
Mg-Nd (7.5% solid) (a) 0.4% (b) 0.8%
22
Stretch-dominated vs bending-dominated behaviour
23
Mg-La
Mg-La
Stretch-dominated
30% vol. fraction of solid
Mg-Nd Bending-dominated
7.7% vol. fraction of solid
Mg-Nd
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(2/2)24/35
.
Stretch dominated
Bending
dominatedIsotropic
foams
Transition between
S-D to B-D at 20%
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Micro-truss hybrids: ultraligth, high flexural stiffness
Micro-truss (Stretch dominated)
linear relationships Design assumes
flexural macroscopic loading
Stretch Dominated vs. Bending Dominated hybrids
Panels with foamed cores: linear relationship as well
E(flex)/Ef ~ (/s) (panel stretch dominated structure)
(prove it!)
1/3 of the bars are
loaded in tension
Foams: ultralight, very flexible
Foams: power law relationships
(involve the second moment I)
Design assumes compressive loading
Linear at
low f=t/d
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Open Cell Foam
properties
“sound”
polymer
Textbook pp. 333-334
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Open Cell Foam
properties
Stretch
dominated
lattice
Stretch dominated:
doubles the stiffness Stretch dominated:
trebles the strength
Bending-dominated vs Stretch dominated
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Foams: form a line of
Slope 2 (E = (ρ/ρs)2Es)
Micro-truss: line of
Slope 1 (E = (ρ/ρs)Es)
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Foams
Ef =(/s)2 Es
Slope 2
Micro-truss
Slope 1
Micro-truss structures fill up another hole in property space
E (tension or
flexural)
Sandwich panels also
belong in here (slope 1)
Eflex /Eface~ /o
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http://www.cellularmaterials.com/advantages.asp
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Hybrid Materials: four families of configurations
Composite
Sandwich
Lattice
Segment
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bricks take compression but not tension or shear
carry out-of-plane forces and bending
carry in-plane loads
require a continuous clamping edge
Examples of topological interlocking
Unbonded structures
that carry load
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Ashby & Brechet, 2003
Scale effects on the
strength of micro-
truss structures
metals ceramics
Gain in
strength
Loss of
strength
*s / *t = 1
Finer
this way
Weibull
modulus m
The strength of low Weibull
modulus (ceramics) micro-
truss structures increases
with segmentation
The strength of high Weibull modulus
(metals) micro-truss structures does not
increase with segmentation
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The strength of ceramic foams of different cell sizes
5x
Colombo and Bernardo, Composites Sci. Tech., 2003, 63, 2353-2359.
For given density, foams
with fine cells are some 5
times stronger than
foams with coarse cells
Compressive
strength
density
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Hybrids: The main points
Combining properties may help filling holes and
empty areas in material property-space maps.
Appropriate Hybrid materials can be created by
combining material properties and shape, the latter at
either micro or macro scale.
Properties of hybrid materials can be easily
bracketed by simple mathematical relationships
which allow straight forward description of behavior .
These functional relationships allow exploring new
possibilities.
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The End
Lecture 12 (Hybrids, 2/2)
Tutorial 6 due on Sat Oct. 31st
at midnight.
Lneed strong electrically
conductive material for power line
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Example of a segmented structure filling a hole in the Material Property Space
Trade-off
surface
Best point
empty
Resistivity
1/TS
A + B + conf + scale
Cu => min elect. resist.
Fe => max TS
interleaving fine strands
Pareto Plot
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Example of a segmented structure filling a hole in the Material Property Space
Natural materials
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Natural fibre composites: Comprehensive Ashby-type materials selection charts
Darshil U. Shah ⇑Oxford Silk Group, Department of Zoology, University of Oxford, Oxford OX1 3PS, UK