Lecture 5-6 Beam Mechanics of Materials Laboratory Sec. 3-4 Jiangyu Li University of Washington
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Transcript of Lecture 5-6 Beam Mechanics of Materials Laboratory Sec. 3-4 Jiangyu Li University of Washington
Lecture 5-6Beam
Mechanics of Materials Laboratory Sec. 3-4
Jiangyu LiUniversity of Washington
Mechanics of Materials Lab
Inclined Load
Notice the sign convention: positive Mz compress upper part, negative stress; positive My extend front part, positive stress!
Inclined Load
z
z
y
yx I
yMI
zM
Stress
Neutral axis
0z
z
y
yx I
yMI
zM
yz
zy
IM
IM
zy tan
Asymmetrical Beam
The origin of y and z axes must be placed at centroid C; orientation isarbitrary.
0ydA
0zdA
Sign Convention for Curvature
yy
Ey
Similar equation apply toBending toward z axis
Note difference with sign convention in bending moment
Asymmetric Beam
zy
yxz
EI
dAyEydAM
2
yzy
yxy
EI
yzdAEzdAM
If z is a principal axis, My=0, bending in x-y plane, analogous to a symmetric beam
z
yz
z
y
I
I
M
M
When z axis is the neutral axis;
Asymmetric Beam
yzz
zxz
EI
yzdAEydAM
yz
zxy
EI
dAzEzdAM
2
y
yz
y
z
I
I
MM
If y is a principal axis, Mz=0, bending in x-z plane, analogous to a symmetric beam
When y axis is the neutral axis;
Asymmetric Beam
• When an asymmetric beam is in a pure bending, the plane in which the bending moments acts is perpendicular to the neutral surface only if the y and z axes are principle centroidal axes and the bending moment acts in one of the two principle plane. In such case, the principle plane in which bending moment acts becomes the plane of bending and the usual bending theory is valid
Analysis of Asymmetric Beam
• Locating the centroid, and constructing a set of principal axes
• Resolving bending moment into My and Mz
• Superposition
z
z
y
yx I
yMI
zM
tantany
z
yz
zy
II
IM
IM
zy
Principle Axes
dAyIx2 dAxI y
2
xydAIxy
2sin2cos221 xyyxyx
x IIIII
I
2cos2sin211 xyyx
yx III
I
yx
xyp II
I
2
2tan
Analysis of Asymmetric Beam
A channel section C 10x15.3
c=0.634
Iy=2.28 in4, Iz=67.4 in4
yA=5.00 in, zA=-2.6+0.634=-1.966 in
Calculating bending stress
Locating neutral axis
Analysis of Asymmetric Beam
ink605.2sin MM y
ink77.14cos MM z
psi3340z
z
y
yx I
yMI
zM
o
y
z
II
zy
1.79
212.5tantan
Normal Stress in Beam
yy
Ey
Curved Beams
Neutral axis is no longer the centroidal axis
Positive M
i
ii AerMc
o
oo Aer
Mc
)(
1/
yrAeMy
dAr
Ar
n
n
Curved Beam
in641.3
1/
i
o
n
r
rIn
h
drrbbh
dAr
Ar
)( yrAeMy
AF
n
cFrM rry n
Curved Beams
rr
IMs
ArI
e
yrAeMy
c
c
n
)(
rrs c
Curvature is large, e is small, rn is cloase to rc
Recover to straight beam
Curved Beam
sbsrb
rc
srsb
sbsr
s
e
c
c
Pay attention to the sign of s
Curved Beam
srsb
sbsr
s
e
c
c
222 sRb
Pay attention to the sign of s
• Read Mechanics of Materials Lab Sec. 4
• 4.26(e), 4.72 posted online
Assignment