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Dave’s Revision Notes

       STRUCTURES
         Outcome 3




                        Gary Plimer 2008
STRUCTURES Outcome 3



OUTCOME 3

Use and interpret data from a tensile test in studying properties of
materials.

When the students have completed this unit they should be able to:

 Plot a load extension graph from given test data
 Identify important points on the graph
 Describe the effect of increased loading on a test piece
 Calculate Young’s Modulus, stress and strain
 Describe the properties of a material from test data
STRUCTURES Outcome 3


1. STRENGTH - the ability of a material to resist force. All materials have
   some degree of strength - the greater the force the material can resist, the
   stronger the material. Some materials can be strong in tension but weak in
   compression, for example mild steel. The converse can also be true, as is
   the case with concrete, which is strong in compression but weak in tension.
    Hence, the reason that concrete is often reinforced with mild steel.

2. ELASTICITY - the ability of a material to return to its original shape or
   length once an applied load or force has been removed. A material such
   as rubber is described as elastic because it can be stretched but when it is
   released it will return to its original condition.

3. PLASTICITY - the ability of a material to change its shape or length under
   a load and stay deformed even when the load is removed.
STRUCTURES Outcome 3

4. DUCTILITY - the ability of a material to be stretched without fracturing
   and be formed into shapes such as very thin sheets or very thin wire.
   Copper, for example, is very ductile and behaves in a plastic manner when
   stretched.

5. BRITTLENESS - the property of being easily cracked, snapped or
   broken. It is the opposite of ductility and therefore the material has little
   plasticity and will fail under loading without stretching or changing shape.
   Cast iron and glass are obvious examples of materials that are brittle.

6. MALLEABILITY - the ability of a material to be shaped, worked or
   formed without fracturing. It is closely related to the property of plasticity.

7. TOUGHNESS - the ability to absorb a sudden sharp load without
   causing permanent deformation or failure. Tough materials require high
   elasticity.

8.    HARDNESS - the ability to resist erosion or surface wear. Hard
     materials are used in situations where two surfaces are moving across or
STRUCTURES Outcome 3


MATERIALS TESTING

In order to discover the various properties of a material we must carry out
    material tests. There are many different types of tests available but the
    most common is the tensile test. As the name suggests the material is
    subjected to a tensile force or in other words, the material is stretched or
    pulled apart.

Results from tensile tests allow us to determine the following properties:

1. The elasticity of a material

2. The plasticity or ductility of the material

3. The ultimate tensile strength of the material.
STRUCTURES Outcome 3


Tensometer or tensile testing machine is designed to apply a controlled
tensile force to a sample of the material.




                                                      TEST SAMPLE




                  HANDLE


                                       BEAM GAUGE
STRUCTURES Outcome 3

In order for tests to be carried out on a consistent basis, the shape of the
specimen to be tested must conform to British Standards.
A typical test specimen is shown below.




                                                END OF
                          LENGTH BEING TESTED
                                                SPECIMEN SHAPED
                             (GAUGE LENGTH)     TO FIT MACHINE




The principle of tensile testing is very simple. As the force is applied to the
specimen, the material begins to stretch or extend. The tensometer applies
the force at a constant rate and readings of force and extension are noted
until the specimen finally breaks. These readings can be plotted on a graph
to show the overall performance of the material.
STRUCTURES Outcome 3

Typical Tensile Test Graph



Between points 0 and ‘A’ the                               C
material behaves elastically and this




                                        LOAD (N)
                                                       B
part of the graph is known as the                  A                  D

elastic region. This means that the
material stretches under the load
but returns to its original length
when the load is removed.
In fact, the force and extension
produced are proportional and this         0
                                                               EXTENSION (mm)
part of the graph will be a straight
line. This relationship is known as
Hooke’s Law and is very important
to structural engineers.
STRUCTURES Outcome 3

‘A’ is called the Limit of Elasticity and any loading beyond this point results in
plastic deformation of the sample.

‘B’ is called the yield point and a permanent change in length results even
when the load is removed. Loading beyond this point results in rapidly
increasing extension.

Between points ‘B’ and ‘D’ the material behaves in a plastic or ductile manner.

At point ‘C’ the maximum or ultimate tensile force that the material can
withstand is reached.

Between ‘C’ and ‘D’ the cross-sectional area of the sample reduces or ‘necks’.




                   NECKING
STRUCTURES Outcome 3




CUP AND CONE
 FRACTURE
STRUCTURES Outcome 3

STRESS STRAIN GRAPHS

Far more useful to an engineer than a load extension graph is a stress strain
graph.

Stress
When a direct force or load is applied to the member of a structure, the effect will
depend on the cross-sectional area of the member. Lets look at column 1 and 2
below. Column 2 has a greater cross-sectional area than column 1. If we apply
the same load to each column, then column 1 will be more effected by the force.
                                         F             F




                                         F              F
                                 C O LU M N 1   C O LU M N 2
STRUCTURES Outcome 3



         Force
Stress =
         Area
                   STRESS N/mm2
                   FORCE N
                   AREA   mm2
   F
σ=
   A
STRUCTURES Outcome 3


                                                     Force
                                            Stress =
                                                     Area
Worked examples: Stress

A square bar of 20 mm x 20 mm cross-           F
section is subjected to a tensile load of   σ=
500 N. Calculate the stress in the bar.        A

                                               500
                                            σ=
                                               400

                                            σ = 1.25 N / mm 2
STRUCTURES Outcome 3


A column of section 0.25 m2 is required to act as a roof support. The
maximum allowable working stress in the column is 50 N/mm2. Calculate
the maximum compressive load acting on the column.

                               Force
                      Stress =
                               Area

                      Force = Stress × Area


                      Force = 50 × 0.25 × 10 6


                      Force = 12.5MN
STRUCTURES Outcome 3

The stress in a steel wire supporting a load of 8 kN should not exceed 200 N/mm2.
Calculate the minimum diameter of wire required to support the load.


   Stress =
            Force                          πd 2
                                    Area =
            Area                            4

            Force                        4A
   Area =                           d=
            Stress                       π

            8000
   Area =                                4 × 40
             200                    d=
                                           π

   Area = 40mm 2                    d = 7.14mm
STRUCTURES Outcome 3


Strain

The result of applying a load or force to a
structural member is a change in length.
Every material changes shape to some extent
when a force is applied to it. This is
sometimes difficult to see in materials such
concrete and we need special equipment to
detect these changes.

If a compressive load is applied to a structural
member, then the length will reduce. If a
tensile load is applied, then the length will
increase. This is shown in the diagrams
below.
STRUCTURES Outcome 3



            Change in Length
   Strain =
            Original Length


            ∆L
         ε=
             L
         STRAIN HAS NO UNITS
STRUCTURES Outcome 3

Worked examples: Strain

1. A steel wire of length 5 m is used to support a tensile load. When the load
   is applied, the wire is found to have stretched by 2.5 mm. Calculate the
   strain for the wire.

                                  ∆L
                               ε=
                                   L

                                   2.5
                               ε=
                                  5000

                               ε = 0.0005
STRUCTURES Outcome 3

2. The strain in a concrete column must not exceed 5 x 10-4. If the column is 3
   m high, find the maximum reduction in length produced when the column is
   loaded.


                                 ∆L
                            ε=
                                  L

                            ∆L = ε × L


                            ∆L = ( 5 × 10 − 4 ) × 3000

                            ∆L = 1.5mm
STRUCTURES Outcome 3


As we have already learned, vital information can be obtained from tensile
tests when the data is plotted in the form of a stress strain graph. The graph
below represents the relationship between stress and strain for common
materials.


                                   MILD STEEL
                   STRESS




                            CAST
                            IRON
                                                FRACTURE


                                     COPPER


                                                           FRACTURE




               0                                           STRAIN
STRUCTURES Outcome 3
1. Yield Stress

  The yield stress is the maximum stress that can be applied to a structural
   member without causing a permanent change in length. The loading on any
   structural member should never produce a stress that is greater than the yield
   stress. That is, the material should remain elastic under loading.

2. Yield Strain

  The yield strain is the maximum percentage plastic extension produced in a
   material before it fails under loading. A ductile material such as copper needs to
   be formed and shaped into items such as pipes. For this to be effective, the
   material requires a high value of yield strain.

3. Ultimate Tensile Stress

  The ultimate tensile stress (UTS) of a material is the maximum stress the
   material can withstand before it starts to fail. If a member in a structure is
   loaded beyond the UTS, the cross-section will reduce and the member will
   quickly fail.
STRUCTURES Outcome 3



YOUNG’S MODULUS

When a material is constantly loaded past its elastic limit, its performance
becomes unpredictable. This could be disastrous, even fatal, if we consider
the scale and type of structures we use every day. For this reason, structural
engineers must ensure that projected stresses in structural members are held
within the materials elastic limit.

When we test a range of common material we find that they all behave in an
elastic manner up to a certain level of loading, even very brittle materials.
STRUCTURES Outcome 3

We also find that within the
elastic limit, the graphs are a
straight line therefore
conforming to Hooke’s Law.




                                     STRESS
                                                  STEEL
This means that stress is
                                                          ALUMINIUM
proportional to strain. We use
the principle of Hooke’s Law
to find a value called young’s                             WOOD

Modulus. Young’s Modulus is
sometimes called the Modulus
of elasticity and is calculated
                                              0
using the formula:                                                    STRAIN

                            Stress
                         Ε=
                            Strain

                              σ
                         Ε=
                              ε
STRUCTURES Outcome 3



For any material, which obeys Hooke’s Law, the slope of the straight line
within the elastic limit can be used to determine young’s Modulus.




 Although any value of stress and strain can be taken from
within this region, it is customary for values to be taken from
the graph at 50% of yield stress.
STRUCTURES Outcome 3


Modulus of elasticity
determines the stiffness of a             A HIGH MODULUS
material.




                                 STRESS
The higher the modulus, the                     B MEDIUM MODULUS
greater the stiffness.
Stiffness is a measure of a
materials resistance to
buckling under compressive                   C LOW MODULUS
loading.
 If a structural member starts
to buckle it will bend and       0                   STRAIN
eventually collapse.
STRUCTURES Outcome 3

Worked example: Young ’s Modulus

An aluminum tie rod is 1.5 m long and has a square cross-section of 20 mm x 20
mm.
A tensile load of 5.6 kN is applied and produces a change in length of the rod of
0.3 mm.
Calculate young’s Modulus for the rod.




                                Stress
             Young ' sModulus =
                                Strain
STRUCTURES Outcome 3
                                               F
a) Calculate the stress in the rod.       σ=
                                               A

                                                5600
                                          σ=
                                               40 × 40
                                               20x20
b) Calculate the strain in the rod.

            ∆L                            σ = 14 N / mm 2
         ε=
             L

               0.3               c) Calculate Young’s Modulus
         ε=                                                          σ
              1500                                              Ε=
                                                                     ε

         ε = 0.2 × 10 −3
                                                                         14
                                                                Ε=
                                                                     0.2 × 10 −3

                                                                Ε = 70kN / mm 2

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Structures outcome-3

  • 1. Dave’s Revision Notes STRUCTURES Outcome 3 Gary Plimer 2008
  • 2. STRUCTURES Outcome 3 OUTCOME 3 Use and interpret data from a tensile test in studying properties of materials. When the students have completed this unit they should be able to:  Plot a load extension graph from given test data  Identify important points on the graph  Describe the effect of increased loading on a test piece  Calculate Young’s Modulus, stress and strain  Describe the properties of a material from test data
  • 3. STRUCTURES Outcome 3 1. STRENGTH - the ability of a material to resist force. All materials have some degree of strength - the greater the force the material can resist, the stronger the material. Some materials can be strong in tension but weak in compression, for example mild steel. The converse can also be true, as is the case with concrete, which is strong in compression but weak in tension. Hence, the reason that concrete is often reinforced with mild steel. 2. ELASTICITY - the ability of a material to return to its original shape or length once an applied load or force has been removed. A material such as rubber is described as elastic because it can be stretched but when it is released it will return to its original condition. 3. PLASTICITY - the ability of a material to change its shape or length under a load and stay deformed even when the load is removed.
  • 4. STRUCTURES Outcome 3 4. DUCTILITY - the ability of a material to be stretched without fracturing and be formed into shapes such as very thin sheets or very thin wire. Copper, for example, is very ductile and behaves in a plastic manner when stretched. 5. BRITTLENESS - the property of being easily cracked, snapped or broken. It is the opposite of ductility and therefore the material has little plasticity and will fail under loading without stretching or changing shape. Cast iron and glass are obvious examples of materials that are brittle. 6. MALLEABILITY - the ability of a material to be shaped, worked or formed without fracturing. It is closely related to the property of plasticity. 7. TOUGHNESS - the ability to absorb a sudden sharp load without causing permanent deformation or failure. Tough materials require high elasticity. 8. HARDNESS - the ability to resist erosion or surface wear. Hard materials are used in situations where two surfaces are moving across or
  • 5. STRUCTURES Outcome 3 MATERIALS TESTING In order to discover the various properties of a material we must carry out material tests. There are many different types of tests available but the most common is the tensile test. As the name suggests the material is subjected to a tensile force or in other words, the material is stretched or pulled apart. Results from tensile tests allow us to determine the following properties: 1. The elasticity of a material 2. The plasticity or ductility of the material 3. The ultimate tensile strength of the material.
  • 6. STRUCTURES Outcome 3 Tensometer or tensile testing machine is designed to apply a controlled tensile force to a sample of the material. TEST SAMPLE HANDLE BEAM GAUGE
  • 7. STRUCTURES Outcome 3 In order for tests to be carried out on a consistent basis, the shape of the specimen to be tested must conform to British Standards. A typical test specimen is shown below. END OF LENGTH BEING TESTED SPECIMEN SHAPED (GAUGE LENGTH) TO FIT MACHINE The principle of tensile testing is very simple. As the force is applied to the specimen, the material begins to stretch or extend. The tensometer applies the force at a constant rate and readings of force and extension are noted until the specimen finally breaks. These readings can be plotted on a graph to show the overall performance of the material.
  • 8. STRUCTURES Outcome 3 Typical Tensile Test Graph Between points 0 and ‘A’ the C material behaves elastically and this LOAD (N) B part of the graph is known as the A D elastic region. This means that the material stretches under the load but returns to its original length when the load is removed. In fact, the force and extension produced are proportional and this 0 EXTENSION (mm) part of the graph will be a straight line. This relationship is known as Hooke’s Law and is very important to structural engineers.
  • 9. STRUCTURES Outcome 3 ‘A’ is called the Limit of Elasticity and any loading beyond this point results in plastic deformation of the sample. ‘B’ is called the yield point and a permanent change in length results even when the load is removed. Loading beyond this point results in rapidly increasing extension. Between points ‘B’ and ‘D’ the material behaves in a plastic or ductile manner. At point ‘C’ the maximum or ultimate tensile force that the material can withstand is reached. Between ‘C’ and ‘D’ the cross-sectional area of the sample reduces or ‘necks’. NECKING
  • 10. STRUCTURES Outcome 3 CUP AND CONE FRACTURE
  • 11. STRUCTURES Outcome 3 STRESS STRAIN GRAPHS Far more useful to an engineer than a load extension graph is a stress strain graph. Stress When a direct force or load is applied to the member of a structure, the effect will depend on the cross-sectional area of the member. Lets look at column 1 and 2 below. Column 2 has a greater cross-sectional area than column 1. If we apply the same load to each column, then column 1 will be more effected by the force. F F F F C O LU M N 1 C O LU M N 2
  • 12. STRUCTURES Outcome 3 Force Stress = Area STRESS N/mm2 FORCE N AREA mm2 F σ= A
  • 13. STRUCTURES Outcome 3 Force Stress = Area Worked examples: Stress A square bar of 20 mm x 20 mm cross- F section is subjected to a tensile load of σ= 500 N. Calculate the stress in the bar. A 500 σ= 400 σ = 1.25 N / mm 2
  • 14. STRUCTURES Outcome 3 A column of section 0.25 m2 is required to act as a roof support. The maximum allowable working stress in the column is 50 N/mm2. Calculate the maximum compressive load acting on the column. Force Stress = Area Force = Stress × Area Force = 50 × 0.25 × 10 6 Force = 12.5MN
  • 15. STRUCTURES Outcome 3 The stress in a steel wire supporting a load of 8 kN should not exceed 200 N/mm2. Calculate the minimum diameter of wire required to support the load. Stress = Force πd 2 Area = Area 4 Force 4A Area = d= Stress π 8000 Area = 4 × 40 200 d= π Area = 40mm 2 d = 7.14mm
  • 16. STRUCTURES Outcome 3 Strain The result of applying a load or force to a structural member is a change in length. Every material changes shape to some extent when a force is applied to it. This is sometimes difficult to see in materials such concrete and we need special equipment to detect these changes. If a compressive load is applied to a structural member, then the length will reduce. If a tensile load is applied, then the length will increase. This is shown in the diagrams below.
  • 17. STRUCTURES Outcome 3 Change in Length Strain = Original Length ∆L ε= L STRAIN HAS NO UNITS
  • 18. STRUCTURES Outcome 3 Worked examples: Strain 1. A steel wire of length 5 m is used to support a tensile load. When the load is applied, the wire is found to have stretched by 2.5 mm. Calculate the strain for the wire. ∆L ε= L 2.5 ε= 5000 ε = 0.0005
  • 19. STRUCTURES Outcome 3 2. The strain in a concrete column must not exceed 5 x 10-4. If the column is 3 m high, find the maximum reduction in length produced when the column is loaded. ∆L ε= L ∆L = ε × L ∆L = ( 5 × 10 − 4 ) × 3000 ∆L = 1.5mm
  • 20. STRUCTURES Outcome 3 As we have already learned, vital information can be obtained from tensile tests when the data is plotted in the form of a stress strain graph. The graph below represents the relationship between stress and strain for common materials. MILD STEEL STRESS CAST IRON FRACTURE COPPER FRACTURE 0 STRAIN
  • 21. STRUCTURES Outcome 3 1. Yield Stress The yield stress is the maximum stress that can be applied to a structural member without causing a permanent change in length. The loading on any structural member should never produce a stress that is greater than the yield stress. That is, the material should remain elastic under loading. 2. Yield Strain The yield strain is the maximum percentage plastic extension produced in a material before it fails under loading. A ductile material such as copper needs to be formed and shaped into items such as pipes. For this to be effective, the material requires a high value of yield strain. 3. Ultimate Tensile Stress The ultimate tensile stress (UTS) of a material is the maximum stress the material can withstand before it starts to fail. If a member in a structure is loaded beyond the UTS, the cross-section will reduce and the member will quickly fail.
  • 22. STRUCTURES Outcome 3 YOUNG’S MODULUS When a material is constantly loaded past its elastic limit, its performance becomes unpredictable. This could be disastrous, even fatal, if we consider the scale and type of structures we use every day. For this reason, structural engineers must ensure that projected stresses in structural members are held within the materials elastic limit. When we test a range of common material we find that they all behave in an elastic manner up to a certain level of loading, even very brittle materials.
  • 23. STRUCTURES Outcome 3 We also find that within the elastic limit, the graphs are a straight line therefore conforming to Hooke’s Law. STRESS STEEL This means that stress is ALUMINIUM proportional to strain. We use the principle of Hooke’s Law to find a value called young’s WOOD Modulus. Young’s Modulus is sometimes called the Modulus of elasticity and is calculated 0 using the formula: STRAIN Stress Ε= Strain σ Ε= ε
  • 24. STRUCTURES Outcome 3 For any material, which obeys Hooke’s Law, the slope of the straight line within the elastic limit can be used to determine young’s Modulus. Although any value of stress and strain can be taken from within this region, it is customary for values to be taken from the graph at 50% of yield stress.
  • 25. STRUCTURES Outcome 3 Modulus of elasticity determines the stiffness of a A HIGH MODULUS material. STRESS The higher the modulus, the B MEDIUM MODULUS greater the stiffness. Stiffness is a measure of a materials resistance to buckling under compressive C LOW MODULUS loading. If a structural member starts to buckle it will bend and 0 STRAIN eventually collapse.
  • 26. STRUCTURES Outcome 3 Worked example: Young ’s Modulus An aluminum tie rod is 1.5 m long and has a square cross-section of 20 mm x 20 mm. A tensile load of 5.6 kN is applied and produces a change in length of the rod of 0.3 mm. Calculate young’s Modulus for the rod. Stress Young ' sModulus = Strain
  • 27. STRUCTURES Outcome 3 F a) Calculate the stress in the rod. σ= A 5600 σ= 40 × 40 20x20 b) Calculate the strain in the rod. ∆L σ = 14 N / mm 2 ε= L 0.3 c) Calculate Young’s Modulus ε= σ 1500 Ε= ε ε = 0.2 × 10 −3 14 Ε= 0.2 × 10 −3 Ε = 70kN / mm 2