es 13 lecture 3
TRANSCRIPT
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MECHANICS OF MATE
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OUTLINE REVIEW
STRESS
NORMAL STRESS
SHEAR STRESS
BEARING STRESS
PUNCHING STRESS
STRAIN
NORMAL STRAIN
SHEAR STRAIN
MATERIAL PROPERTIES
STRESS-STRAIN DIAGRAM AND HOOKES LAW
STRAIN ENERGY
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Average Normal Stress Distributio
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Normal Stress
An element subjected to a normal stress must have an opposite
normal stress. UNIAXIAL STRESS P is equivalent to the volume under the stress diagram
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Maximum Average Normal Stres
Sometimes, a member experiences multiple loads. This would mdifferent sections, different internal forces are induced.
It is very important to find the section where P/A is maximum
Axial or Normal Force Diagram
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Average Shear Stress
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Single Shear
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Double Shear
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Bearing Stress
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Punching Shear Stress
Punching Shear:
=P/Area ResistingPunching Shear
Punching Shear ArePerimeter of hole Thickness
Link ABC:
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Link ABC:- Upper portion: 3/8 in th- Lower portion: 1/4 in t- Upper and lower portio
are glued @ B
Pin A: 3/8 in diameterPin C: 1/4 in diameter
Find:a) Shear stress in pin A
b) Shear stress in pin Cc) Largest normal stress
link ABCd) Average shear stress i
glued arese) Bearing stress in link a
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STDeformations: Shape/a
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DEFORMATIONS
Changes in the shape and size of a body that is subjected to an force or temperature change
Can either be highly visible or practically unnoticeable
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Normal Strain,
Can be defined as:
The change in length of a line per unit le
Dimensionless
Elongation (+)
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Shear Strain,
Change in angle between two previously perpendicular lines
If is less than pi/2, (+)
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Small Strain Analysis
For small strains
Sin = , Cos = 1, Tan =
Paths of deformed member can be approximated as straight lines
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A rigid lever is attached to a cable. A force P makes the lever 0.05degrees. Determine the strain on the cable.
D t i th Sh St i t E if id CD i di l d b
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Determine the Shear Strain at E if side CD is displaced b
shown.
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MATERIAL PROPERSTRESS-STRAIN DIAGRAM,HOOKES LAW,ST
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TENSILE TEST (video)
http://www.cyberphysics.co.uk/topics/forces/young_modulus.htm
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STRESS-STRAIN DIAGRAM (Stee
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Types of Stress-Strain Diagrams:
1. Conventional Stress-Strain Diagram uses
the original dimensions of a material
2. True Stress-Strain Diagram uses theactual dimensions of a material at the instantthe load is applied
Stress-Strain Diagram
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STRESS-STRAIN DIAGRAM (Stee
Elastic Region
Upon removal of load, material returns
to its original shape
Plastic Region Material has permanent deformation upon
increase of load
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STRESS-STRAIN DIAGRAM (Stee
Proportional Limit
Stress is proportional to strain
Elastic Limit
Material still returns to its original shape
beyond the proportional limit
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STRESS-STRAIN DIAGRAM (Stee
Yield stress
Stress at the region where material deforms
without any increase in load
Ultimate Stress Maximum stress achieved upon increase of load
after the material yields
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STRESS-STRAIN DIAGRAM (Stee
Necking
decrease in the cross-sectional area in
a localized region
Rupture
Point where material breaks or fails
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STRESS-STRAIN DIAGRAM (Concr
http://www.diracdelta.co.uk/science/source/s/t/stress-strain%20diagram/source.html#.U9F0lPmSxrs
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Ductile vs Brittle
http://www.cyberphysics.co.uk/topics/forces/young_modulus.htm
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HOOKES LAW
=
E- Modulus of Elasticity/Youngs Modulus
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STRAIN ENERGY Energy that is stored in a material due to its deformation
Strain-Energy Density
=
Modulus of resilience
Modulus of toughness
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Modulus of Resilience (ur)
- Amount of energy a material can take beforeexperiencing permanent deformation.
- It is the area under the stress-strain diagramwhere stress is proportional to strain.
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Modulus of Toughness (ut)
- Amount of energy a material can take before it
fractures/ breaks.
- Represents the entire area under the stress-straindiagram