2. STRESS: Force/unit area (lbs/sq.in.)
Load F
Reaction = F
Compression (e.g., pier pylon)
Cross-
section
area A
Compressive
Stress
sc = F/A
Load F
Reaction = F
Tensile
Stress
st = F/A
Cross-
section
area A
Tension (e.g., bridge suspension cable)
3. STRAIN: deformation in length
Load F
Reaction = F
Compression Strain negative)
Load F
Reaction = F
Tensile Strain (Strain) positive
L L
d
d
STRAIN: d/L
(dimensionless)
4. Hooke’s Law: Stress ∝ Strain
STRAIN: d/L
STRESS:
F/A
y = mx
s = E d/L
Slope, E =
Modulus of
Elasticity
Structural steel
Yield
point
Proportional
Limit
Ultimate
strength Fracture
point
Maximum
working stress
Factor of Safety
Re: to lower stress:
Reduce LOAD, or
Increase AREA
6. Since there is both tension &
compression in bending …
we need to look at
Bending
Moments:
Distributed load: w lbs/ft
L
wL/2 wL/2
LOAD
diagram x
x
SHEAR
diagram
Cumulative Load:
Vx = ∫w dx
x
0
x
BENDING
diagram
Cumulative Area:
Mx = ∫Vx dx
x
0
Note: Bending is maximum at the location where Shear is zero
7. STRESS in Bending:
Remember: Stress = Force/Area (psi)
And Stress (in bending) increases as we
move away from the neutral axis
NA
C T Still need to know:
Distance from NA (c)
Something about how the
cross-sectional area is
distributed N & S of the
neutral axis …
Moment of Inertia, I
c1
c2
8. Moment of Inertia:
For rectangular beams, I = bh3/12
NA
b
h
Thus for a 2x4:
I = bh3/12 = 2 x 43/12 = 32/3 = 10.67
And for a 2 x 12:
I = 2 x 123/12 = 288!
Note that a 2x12 lying “flat” (b=12; h=2)
I = bh3/12 = 12 x 23/12 = 8
(less than a 2x4 standing up)
9. Moment of Inertia: (cont’)
In general, the more area farther from the NA,
the greater the moment of inertia
Distributing the same
area at a greater
distance from the NA
produces a stronger
beam of the same
weight
10. STRESS in Bending: (reprise)
Maximum Stress (in bending), smax = Mc/I
Where: M = maximim bending moment
unit: lb-in (lb-ft x 12)
c = maximum distance from NA
unit: inches
I = moment of inertia of beam cross-section
unit: inches4
Shorthand notation for I/c is Z (section modulus)
in units of in4/in = in3
Thus, smax = M / Z (in psi—lb-in/in3 = lb/in2)
11. STRESS in Bending: (reprise)
Consider the sections examined under a bending
moment of 1200 ft-lb (14400 in-lb)
Upright 2x4
I = 10.67 in4
c = 2 in
Z = 5.33 in3
smax = 2700 psi
Upright 2x12
I = 288 in4
c = 6 in
Z = 48 in3
smax = 300 psi
Flat 2x12
I = 8 in4
c = 1 in
Z = 8 in3
smax = 1800 psi
If the maximum allowable working stress for this
material were 3000 psi, which would you choose?
12. Moment of Inertia: (cont’)
There are tables of I (and Z) for standard steel
“sections”
I-beam Tee Channel L
And I for any shape can (with
some effort) be calculated
13. How about this shape?
Ship sections can
be reduced to an
equivalent (if
irregular) I-beam
The section
modulus, Z, can
then be calculated
… and the I-beam
examined under
different bending
load conditions
Yes, it is
complicated
14. Remember:
Load Shear Bending Moment?
Distributed load: w lbs/ft
L
wL/2 wL/2
LOAD
diagram x
Cumulative Load:
Vx = ∫w dx
x
0
Cumulative Area:
x
SHEAR
diagram
x
BENDING
diagram
Mx = ∫Vx dx
x
0
15. How Complicated? Consider …
Irregular loading:
downward forces of
cargo & structure
Buoyant (upward)
forces proportional
to underwater
volume of hull
… and that’s in
still water
Shear forces &
bending moments
vary as wave
crests amidships
or fore & aft
16. If fact, stresses are dynamic …
rolling pitching
yawing
racking hogging & sagging