Title: Hardness Ductile Force extension curves Malleable Brittl
1Solid Materials
2Index
Properties of Solid Materials
Uses of Solid Materials
Maths Help
Hardness
Hookes Law
Finding the Gradient of a Graph
Force extension curves
Stiffness
Toughness
Elastic Strain Energy
What does proportional mean?
Brittle
Stress
Strong
Strain
Area Under A Graph
Malleable
The Young Modulus
Ductile
Energy Density
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3Properties of Solid Materials
- Hardness is a surface phenomenon. The harder the
material, the more difficult it is to indent or
scratch the surface - The Mohs scale of hardness grades minerals from
talc (1) to diamond (10), i.e. From softest to
hardest. - BHN is the British Hardness Number used in
engineering.
4Properties of Solid Materials
- Stiffness A stiff material deforms very little
even when subject to large forces. - Stiff materials have a high Young Modulus, i.e. a
high gradient on a stress strain curve
5Properties of Solid Materials
- Toughness A tough material is able to absorb
energy from impacts and shocks without breaking - Tough metals often undergo considerable plastic
deformation in order to absorb this energy - Car tyres use a mixture of rubber and steel so
the can absorb the energy from the impacts with
road surfaces.
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6Properties of Solid Materials
- Brittle objects will shatter or crack easily when
they are subjected to impacts and shocks - Brittle materials undergo very little plastic
deformation before they break - Glass is often brittle it cracks or breaks with
relatively small amounts of energy
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7Properties of Solid Materials
- Strong objects can withstand large forces before
they break - The strength of a material depends on its size
and so therefore is defined in terms of its
breaking stress - (where stress force / area)
8Properties of Solid Materials
- Malleable materials can be hammered out into thin
sheets or beaten into shape - Gold leaf is very malleable and so can be easily
made into gold leaf
9Properties of Solid Materials
- Ductile materials can be drawn into wires.
- Copper is very ductile and so copper wires are
often used as electrical cables. - The copper is drawn out from cylinders until it
reaches the desired diameter. - Ductile materials are often malleable however,
malleable materials will often break when
extended.
10Hookes Law
- A material obeys Hookes Law if the extension
produced by a force is directly proportional to
that force.
F a ?x F k ?x
K spring constant or stiffness, in N m-1
Maths Help What does proportional mean?
11Force Extension Curves
- When copper wire is extended, you may get a curve
like this
- From O to A Hookes Law is Obeyed
- This means that the wire is behaving elastically
and so loading and unloading are reversible - The bonds between atoms are stretched like
springs but return to their original lengths when
the deforming force is removed
O
More
12Force Extension Curves
- When copper wire is extended, you may get a curve
like this
- Beyond point B, the wire is no longer elastic
- Although the wire may shorten when the load is
removed it will not return to its original length - It has gone past the point of reversibility has
therefore undergone permanent deformation
O
More
13Force Extension Curves
- When copper wire is extended, you may get a curve
like this
- As the load is increased the wire yields and will
not contract at all if the load is reduced - This is the yield point (C on the graph)
- The wire is now plastic (it can be pulled like
plasticine until it breaks) - In the plastic region the bonds are no longer
being stretched - Layers of atoms stretch across each other with no
restoring forces
C
O
More
14Force Extension Curves
- If the load is now removed from the copper wire
during the plastic phase and reloaded, the
following graph could be produced
- The wire regains its springiness and has the
same stiffness as before - The ability of some metals to be deformed
plastically and then regain elasticity is very
useful - Sheets of mild steel can be pressed into the
shape of a car door and then pressed again when
the stiffness and elasticity of the steel are
regained
15Elastic Strain Energy
- Elastic strain energy is sometimes referred to as
elastic potential energy - It is analogous to gravitational potential energy
- It is therefore the ability of a deformed
material to do work as it regains its original
dimensions - For example the energy stored in a catapult is
transferred to kinetic energy as it is released
More
16Elastic Strain Energy
- Remember work done energy transferred
- The work done, and therefore the elastic strain
energy can be worked out from a force extension
graph - For an object obeying Hookes Law the following
graph would be obtained
- Work done force x displacement
- i.e. ?W Fave?x
- This is equal to the area under the curve and so
- i.e. ?W ½ Fmax?x
-
Fmax
Maths Help Area of a triangle
17Stress
- Stress is the force (or tension) per
cross-sectional area - i.e. Stress tension
- cross-sectional area
- Units of stress are N m-2 Pa (pascal)
More
18More Stress
- This is sometimes referred to as tensile stress
when a material (e.g. A wire) as a force pulling
it or compressive stress when a material has a
force squashing it - The stress needed to break a material is called
the breaking stress or ultimate tensile stress
19Strain
- Strain is the ratio of the extension of a wire to
its original length when a stress is applied - Strain extension
- length
- Strain has no units, although it may sometimes be
referred to as a age
Careful! The extension is sometimes x, ?x or ?l
20The Young Modulus
- The Young modulus of a material is a property of
materials that undergo tensile or compressive
stress - Young modulus stress
- strain
- Since stress is in Pa and strain has no units,
the Young Modulus also has the units of Pa
More
21The Young Modulus
- The Young Modulus is a measure of the stiffness
of a material, i.e. a stiff material has a high
Young Modulus - Since
If the sample breaks or behaves elastically, the
line wont be straight. However the Young Modulus
can still be found from the gradient of the
straight line section of the graph
Maths Help Calculating Gradient
22Energy Density - 1
- Remember work done energy transferred
- The energy density is the work done in stretching
a specimen (or the strain energy stored) per unit
volume of the sample. - For a wire that obeys Hookes Law
- energy density work done
- volume
- Therefore energy density stress/strain
-
More
23Energy Density - 2
- From the last slide, energy density
stress/strain - It is therefore the area under a stress-strain
graph
If it is under the Hookes Law area of a graph,
you need to find the area of the triangle So
energy density ½ x stress x strain ½ x s
x e
Maths Help Area of a triangle
More
24Energy density - 3
- If you have a more complicated curve, you could
find the area under the graph by counting squares
If you do this, be careful to convert your square
count correctly, i.e. Calculate how much one
square is worth
More
25Energy Density - 4
- The ability of a material to absorb a large
amount of energy per unit volume (i.e. it has a
large energy density) before fracture is a
measure of the toughness of the material, e.g.
mild steel - Materials which fracture with little plastic
deformation and so the area under the
stress-strain graph is small (i.e. It has a low
energy density) is brittle, e.g. glass
26Gradient of a graph
- The gradient of a graph can be found be dividing
the up by the across or in mathematical terms by - Gradient change in y axis ?y
- change in x axis ?x
Back To The Young Modulus
x
27Maths Help What Does Proportional Mean?
- Direct proportionality is shown by a straight
line graph through the origin - As x is doubled, y is doubled, etc
- The proportionality sign is a, so
- we can write y a x
- To turn this into an equation without the
- proportionality sign we need a constant,
- so it becomes
- ykx
- k is the constant of proportionality and
- is represented by the gradient of the graph
Back To Hookes Law
28Maths Help Area of a triangle
- The area of a triangle ½ x base x height
- This is useful for finding the area under
straight line graphs
- Area under the graph
- area of the triangle
- ½xy
Back To Elastic Strain Energy
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