Topic 1 - Structures Workshop, Inc.

RISD 2154
STEEL STRUCTURES
Topic 1: Intro to Steel Design
Erik Anders Nelson, PE, SE
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Fall 2014
New Science of Strong Materials - JE Gordon
Great Division in Technology: Metals and Non – Metals
Decreasing Costs* and Improvements of iron and steel in the 18th
and 19th century “perhaps the most important event in history”
Future non-metals (carbon crystals / ceramics) may have higher
strength and will resemble “improved versions of wood and
bone” using sophisticated techniques
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Strength depends on Molecular Scale
We know pretty well how things behave, but not necessarily why
Engineering have little “why”
why knowledge,
knowledge we only have “how”
how – we
reviewed materials and wrote down testing data in unreadable
books. With things like “strength” and “stiffness” properties we
have been pretty good and predicting behavior and scaling up
to large scale proportioning of structures.
We need a good background in “The Science of Elasticity” - which
requires us to abandon our instinctive knowledge of materials
materials.
It is the preconceptions that cause the difficulty in learning
something new….can you answer objectively the difference
between chocolate and caramel?
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Microstructure – Intro Chemistry
Solids are held together by chemical and physical bonds
Strength is related to these chemical bonds (so classical physics
and chemestry) but also related to new concepts such as
dislocations and stress concenrations.
There are about 100 different types of atoms, and 20-30 of those
effect materials related to us. Each kind of atom is called an
element.
Iron (Fe) and Carbon (C) are homogenous atoms that can be
combined to create entirely different types of stuff (Steel). Or
chlorine (poisines green gas) with sodium (a metal) creates
NaCl or table salt. Elements/atoms form “matter”
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Does Steel Meet these Assumptions?
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Crystal Lattices
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Engineering Assumptions
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1650 Robert Hooke
“as the deflection, so is the force.“ P = kx
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Force and Displacement F = kx (Tension)
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Force to Stress
Force = F = 10 kips or 10,000 lbs
Stress = F/A = 2 ksi or 2000 psi (or KN/m2 or ksf
Elongation to Strain
Elongation = x (in units of length like inches)
Strain, e = x/L = unit less = change in length over original length
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Stress – Strain Curve of Caramel and Chocolate
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Deformations Under Axial Loading
From Hooke’s Law:
  E


E

P
AE
From the definition of strain:


L
Equating and solving for the deformation,
PL
 
AE
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Consider L0 = 100 inch long tension member.
∆Yield
∆Onset of Strain Hardening
∆Peak Load
= approx. 0.002(100)
= approx. 0
0.02(100)
02(100)
= approx. 0.20(100)
= 0.2”
= 2”
= 20”
Excessive deformations defines “Failure” for tension member
yielding. Limit to FyAg.
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8
Design of Structural Systems
Key design elements
– Load calculation
– Proportioning elements to resist loads
– Refine elements for serviceability
•
•
•
•
Deflection
Interaction with architectural and mechanical systems
Vibration
Occupant-specific requirements
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Fall 2014
Approx Engineering Properties of Materials
Steel
– Maximum stress: 50,000 lb/in2 ( can be 270,000)
– Maximum strain: 0.003
– Modulus
M d l off elasticity:
l ti it 29
29,000,000
000 000 lb/i
lb/in2
Concrete
– Maximum stress: 5,000 lb/in2 (can be 12000)
– Maximum strain: 0.004
– Modulus of elasticity: 3,600,000 lb/in2
Wood
Values depend on wood grade
grade.
– Maximum Stress: 1200 lb/in2
– Modulus of elasticity: 1,400,000 lb/in2
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Types of Loads
Reference: ASCE 7-10 “Loads on Buildings and Other Structures”
Dead Loads
– Weight of structure
– Partition loads
Live Loads
– Occupant load
– Snow
Lateral Loads
– Seismic
– Wind
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Dead Load (Self Weight)
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ASCE-7
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Common Live Loads
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Snow Loads
Basic snow load
– 30 psf throughout RI, 30-40 psf in MA, up to 90 psf in NH, ME, VT
Drift
– Can add up to 150 psf additional snow load
– At low roof/high roof areas
Unbalance loading
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ASCE-7 - Ground Snow Load, Pg
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Load Notation
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Apply Dead and Live Loads
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Presentation Based on Spec Chapters
Chapter A - General
Chapter B - Design Info
Chapter C - Stability
Chapter D - Tension
Chapter E - Compression
Chapter F - Flexure
Chapter G - Shear
Chapter H - Combined
Chapter J - Connections
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New ASD and LRFD
Allowable Strength Design (henceforth, NEW ASD) approach.
Although the NEW ASD bears a similar name to the older
Allowable Stress Design (henceforth, OLD ASD), the two are
not to be confused
LRFD hasn’t changed.
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2010 ASD Combinations
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2010 LRFD Combinations
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ASD and LRFD Load Combinations
D+L
1.2D + 1.6L
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AISC Steel Design Manuals
1963 AISC ASD 6th Edition
1969 AISC ASD 7th Edition
1978 AISC ASD 8th Edition
1989 AISC ASD 9th Edition
ASD = actual stress values are
compared to the AISC allowable
stress values
1986 AISC LRFD 1st Edition
1993 AISC LRFD 2nd Edition
1999 AISC LRFD 3rd Edition
LRFD = ultimate forces and
moments are compared to the
AISC limiting forces and
moments capacity
2005 AISC 13rd Edition
2010 AISC 14th Edition
LRFD and “New
New ASD”
ASD
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Limit State Expressions, Demand < Capacity
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Strength Design vs. Allowable Stress Design
Allowable Stress
Design or Working
Stress Design,
ASD-89
Load and Resistance
Factor Design or
Ultimate Design,
LRFD
ASD-05 / 10
Loads
Service
Ultimate 1.2D + 1.6L
Service
Useable
p
y
Capacity
Some fraction of
yyield
(Ex. 0.66 FyS)
Full strength, incl. postyyield
(Ex. 0.9FyZ)
Full strength, incl.
post-yield
p
y
(Ex. FyZ/1.67)
D+L
Allowable
Strength Design
D+L
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Compare ASD to LRFD
ASD
1.0D + 1.0L
LRFD 1.2D + 1.6L
OLD ASD
LRFD
0.6Fy
× (1.5) = 0.9Fy (LRFD)
0.5Fu
× (1.5) = 0.75Fu (LRFD)
NEW ASD
LRFD
Fy /1.67
× (1.5) = 0.9Fy (LRFD)
Fu /2
× (1.5) = 0.75Fu (LRFD)
ASD × 1.5 = LRFD
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L/D Calibration
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