K. Youssefi and B. Furman Engineering 10, SJSU 1 Structures and Stiffness B. Furman K. Youssefi 20SEP2007
K. Youssefi and B. Furman Engineering 10, SJSU 1
Structures and Stiffness
B. FurmanK. Youssefi20SEP2007
K. Youssefi and B. Furman Engineering 10, SJSU 2
Outline
• Newton’s 3rd Law• Hooke’s Law• Stiffness• Area moment of Inertia• Orientation of cross section and stiffness• Comparison of cross sections• Materials and stiffness
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Newton’s 3rd Law
• Lex III: Actioni contrariam semper et æqualem esse reactionem: sive corporumduorum actiones in se mutuo semper esseæquales et in partes contrarias dirigi.
• To every action there is always opposed an equal reaction: or the mutual actions of two bodies upon each other are always equal, and directed to contrary parts.
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Newton’s 3rd Law - example
M M
Free body diagram T, tension
T, tension
M*g
•Isolate the body of interest
•Put back the forces that are acting
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Hooke’s Law
• Robert Hooke (1635-1702)– Materials resist loads (push or pull back) in
response to applied loads• This ‘resistance’ is accomplished by deformation of
the material (changing its shape)– Tension (stretching)– Compression (shortening)– Stretching or shortening of chemical bonds in atoms
• The science of Elasticity concerns forces and deformations in materials
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Hooke’s Law, cont.
• Hooke found that deflection was proportional to load
Load, N
Deflection, mm
slope, kSlope of Load-Deflection curve:
deflection
loadk =
The “Stiffness”
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Stiffness
• Stiffness in tension and compression– Forces F applied, length L, cross-sectional area, A,
and material property, E (Young’s modulus)
AE
FL=δF
δF
k =
AE
FLF=
L
AEk =
F
L
A
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Stiffness, cont.
• Stiffness in bending
• How does the material resist the applied load?– Think about what happens to the material as the beam
bends• Inner “fibers” (A) are in compression (radius of curvature, Ri)• Outer “fibers” (B) are in tension (radius of curvature, Ro)
A
Ri
B
Ro
F
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Review Question 1
• Stiffness is defined as:A. Force/Area
B. Deflection/ForceC. Force/Deflection
D. Force x DeflectionE. Mass/area
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Concept of Area Moment of Inertia
The Area Moment of Inertia, I, is a term used to describe the capacity of a cross-section (profile) to resist bending. It is always considered with respect to a reference axis, in the X or Y direction. It is a mathematical property of a section concerned with an area and how that area is distributed about the reference axis. The reference axis is usually a centroidal axis.
The Area Moment of Inertia is an important parameter in determine the state of stress in a part (component, structure), the resistance to buckling, and the amount of deflection in a beam.
The area moment of inertia allows you to tell how stiff a structure is.
The higher the area moment of inertia, the less a structure deflects (higher stiffness)
Mathematically, the area moment of inertia appears in the denominator of the deflection equation, therefore;
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Mathematical Equation for Area Moment of Inertia
Ixx = ∑ (Ai) (yi)2 = A1(y1)
2 + A2(y2)2 + …..An(yn)
2
A (total area) = A1 + A2 + ……..An
X X
Area, A
A1
A2
y1
y2
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Moment of Inertia – Comparison
Load
2 x 8 beam
Maximum distance of 1 inch to the centroid
I1
I2 > I1 , orientation 2 deflects less
1
Load
Maximum distance of 4 inch to the centroid I2
2
2 x 8 beam
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Moment of Inertia Equations for Selected Profiles
π (d)4
64I =
Round solid section
Rectangular solid section
b
hbh31I =
12
b
h
1I =
12hb3
d Round hollow section
π
64I = [(do)
4 – (di)4]
do
di
BH3 -1I =
12bh31
12
Rectangular hollow section
H
B
h
b
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Example – Optimization for Weight & StiffnessConsider a solid rectangular section 2.0 inch wide by 1.0 high.
I = (1/12)bh3 = (1/12)(2)(1)3 = .1667 , Area = 2
(.1995 - .1667)/(.1167) = .20 = 20% less deflection
(2 - .8125)/(2) = .6 = 60% lighter
Compare the weight of the two parts (same material and length), compare areas. Material and length is the same for both profiles.
I = (1/12)bh3 = (1/12)(2.25)(1.25)3 – (1/12)(2)(1)3= .3662 -.1667 = .1995
Area = 2.25x1.25 – 2x1 = .8125
So, for a slightly larger outside dimension section, 2.25x1.25 instead of 2 x 1, you can design a beam that is 20% stiffer and 60 % lighter
2.0
1.0
Now, consider a hollow rectangular section 2.25 inch wide by 1.25 high by .125 thick.
H
B
h
b
B = 2.25, H = 1.25
b = 2.0, h = 1.0
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Review Question 2
• Which cross section has the larger I?A.
B.
Rectangular Horizontal
Rectangular Vertical
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Stiffness Comparisons for Different sections
Square Box Rectangular Horizontal
Rectangular Vertical
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Material and Stiffness
E = Elasticity Modulus, a measure of material deformation under a load.
Y = deflection = FL3 / 3EI
F = forceL = length
The higher the value of E, the less a structure deflects (higher stiffness)
Deflection of a Cantilever Beam
Fixed end
Support
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Modulus of Elasticity (E) of Materials
Steel is 3 times stiffer than Aluminum and 100 times stiffer than Plastics.
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Density of Materials
Plastic is 7 times lighter than steel and 3 times lighter than aluminum.
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Wind Turbine Structure
The support structure should be optimized for weight and stiffness.
Support Structure
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Review Question 3
• Which material has the higher stiffness?A. Steel
B. Aluminum C. Alumina ceramic
D. NylonE. Unobtanium
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Examples of Achieving Structural Stiffness
‘Ribbing’‘Gusset’
‘Boss’
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Examples of Achieving Structural Stiffness, cont.
http://en.wikipedia.org/wiki/Image:FT_Rail.jpg
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Examples of Achieving Structural Stiffness, cont.
Welded ‘box’construction
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Examples of Achieving Structural Stiffness, cont.
‘Flange’