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Dean Hackett
Structures
Week 2
Dean Hackett
In previous sessions…
• Brief review of previous learning:– Types of motion– Classes of lever– Turning moments
Dean Hackett
Types of structure
• Mass• Frame• Shell
Dean Hackett
Forces
• Compression• Tension• Torsion• Shear• Bending
Dean Hackett
Applying forces
• Distributed (UDL)• Concentrated (point)
• Static• Dynamic
Dean Hackett
Reinforcing structures
• Create the following shapes from the modelling materials supplied. Ensure free-moving pin joints.
• Reinforce each shape internally using pin joints• Reinforce each shape internally using only string
Dean Hackett
Combining external forces
Force A
Force B
What direction will the ball move in?
Resultant force C
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Using vectors
Force A10N
Force B10N
Any value that has both magnitude and direction can be drawn as a vector
Resultant force C
Draw forces accurately and to scale
Complete the parallelogram (in this case a square)
Draw in the resultant
Measure magnitude and angle
Dean Hackett
Parallelogram of forces
Force A15N
Force B10N
Resultant force C
Draw forces accurately and to scale
Complete the parallelogram (in this case a rectangle)
Draw in the resultant
Measure magnitude and angle
Dean Hackett
Parallelogram of forces
Force A15N
Force B10N
Resultant force C
Draw forces accurately and to scale
Complete the parallelogram (in this case a parallelogram)
Draw in the resultant
Measure magnitude and angle
60°
Dean Hackett
Parallelogram of forces
Force A15N
Force B10N
Resultant force C
Draw forces accurately and to scale
Complete the parallelogram
Draw in the resultant
Measure magnitude and angle
60°
Dean Hackett
Parallelogram of forces
Force A37N
Force B25N
Resultant force C
Draw forces accurately and to scale
Complete the parallelogram
Draw in the resultant
Measure magnitude and angle45°
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Triangle of forces
Force A260N
Force B180N
Resultant force D
Redraw forces accurately and to scale, with arrows nose to tail
Complete the triangle by drawing in the resultant
Note that the resultant runs from start point ‘a’ to end point ‘c’
60°The equilibrant completes the triangle with all arrows running nose to tail
a
bc
This closed shape with all vectors running in sequence means the forces are in equilibrium
Equilibrant force E
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Triangle of forces
Force A236N
Force B115N
Redraw forces accurately and to scale, with arrows nose to tail
Draw in equilibrant, completing the triangle20°
Calculate equilibrant for these forces using triangle of forces
Equilibrant
AA
BB
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Polygon of forces
Force A27N
Force B18N
Redraw forces accurately and to scale, with arrows nose to tail,
Draw in equilibrant ensuring flow of arrows is continued
50°
Force C20N
60°
45°
Force D6N
Note that the order in which the forces are drawn does not matter, as long as the flow is consistent
AABB
CC
DD
AA BB
CCDD
Dean Hackett
Polygon of forces
Force A150kN
Force B70kN
Redraw forces accurately and to scale, with arrows nose to tail,
Draw in equilibrant ensuring flow of arrows is continued
60°
Force C180kN
30°
Force D160kN Note magnitude and
direction.
AA
BBCC
DD
Equilibrant
Dean Hackett
Internal forces If a compressive force is applied to the top of the column, what force must the column be applying back, in order to remain in equilibrium?
What is happening at the base of the column?
The red arrows indicate that the column is under compression and is, therefore, a strut
Dean Hackett
Internal forces If a load is applied to the top of the structure, what do the internal forces look like?
Are these struts or ties?
The red arrows indicate that the members are under compression (they are pushing back) and are, therefore, struts
Dean Hackett
Internal forcesIf we do not know what the internal forces are
doing, we can still construct a triangle of forces:
150N
45° 45°
Label spaces as per Bow’s Notation
A B
C
Draw the force that you do know, ab
We don’t know if bc is in compression or tension, so draw a line across the end of ab at the correct anglea
b
Assuming the structure is in equilibrium, there is only one way to complete the triangle using the force ca
Measure the magnitude and note direction of the constructed vectors.
c
Transfer findings to original problem
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Internal forces
150N
60° 60°
Redo the calculations using a steeper angle
A B
C
What do you notice about the forces in individual members?
What are the problems in designing a structure in this way?
Dean Hackett
Internal forcesRedo the calculations using a shallower angle
What do you notice about the forces in individual members?
What are the problems in designing a structure in this way?
150N
30° 30°
A B
C
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Hookes' Law
0
1
2
3
4
5
6
7
8
9
10
0 100 200 300 400 500
Extension
Lo
ad
• Gradually load up and measure extension of a spring or other materials
Hookes’ Law
• Complete at least two full sequences, completing table as you go
• Use Excel to plot graphs of load/extension
Dean Hackett
Stress
• Nominal Stress σ = Load Р/Original area А (N/m2)
2.4kN5kN
0.15m2
0.08m2Which rod is under the most stress?
Bar A
5000/0.15 = 33333N/m2
= 33.3kN/m2
Bar B
2400/0.08 = 30000N/m2
= 30kN/m2
A B
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Strain
• Strain ε = extension e/original length L (no units!)
Which rod is under the most strain?
215m
m
180m
m
180m
m
150m
m
A B
Bar A
35/180 = 0.19
Bar B
30/150 = 0.2
Dean Hackett
Young’s Modulus
• Modulus of elasticity E = stress σ /strain ε (N/m2)
Which rod is the most elastic?A B
Bar A
33300/0.19 =
175kN/m2 (175 kPa)
Bar B
30000/0.2 =
150kN/m2 (150 kPa)
33.3kN/m2 30.0kN/m2
0.19 0.2
Note that a lower modulus of elasticity means more flexibility
Pascals are a measure of load over an area or ‘pressure’.
Dean Hackett
Young’s ModulusComplete the table on Excel to calculate Young’s modulus for your test pieces
Mass (g) Load (N)
Stress = load / area area =
1.57mm2
Length (mm)
Extension (mm)
Strain = Extension /
original length
Young’s modulus = stress /
strain
0 0 0 205 0 0
100 0.981 0.624841 230 25 0.121951 5.12
200 1.962 1.249682 285 80 0.390244 3.20
300 2.943 1.874522 340 135 0.658537 2.85
400 3.924 2.499363 390 185 0.902439 2.77
500 4.905 3.124204 440 235 1.146341 2.73
600 5.886 3.749045 490 285 1.390244 2.70
700 6.867 4.373885 540 335 1.634146 2.68
800 7.848 4.998726 590 385 1.878049 2.66
900 8.829 5.623567 640 435 2.121951 2.65
Plot a graph of stress/strain
Youngs modulus = stress / strain
0
1
2
3
4
5
6
0 0.5 1 1.5 2 2.5
Strain (extension / original length)
Str
ess
N/m
m2
(lo
ad /
are
a)
Compare elasticity of the springs with other groups
Dean Hackett
Young’s ModulusWhat does the graph show?
The modulus of a material can be plotted against many other characteristics such as cost, thermal conductance, working temperature range, etc.
Dean Hackett
Common Beam Sections
Closed Sections Open Sections
Which of these sections is the most efficient?
What problems might you expect to be associated with the different sections?
Dean Hackett
Task: Avoiding stress
• Devise a method for testing the strongest practical way of producing a box corner in acrylic.
• Create test pieces and test your ideas.
Dean Hackett
Weblinks
• www.greenhomebuilding.comBig resources for sustainable home design
• www.sustainableabc.comFantastic resources for sustainable design
• www.architect.org/links/sustainable_architecture.html Good set of eco links
• www.ecosustainable.com.au Huge set of eco links
• www.naturalspace.com Fantastic site, beautiful case studies
• www.lanxun.com/pce/index.htmRange of design programs to try
• www.architecturalresources.infoNice but problematical site with good tutorials