Liquefaction potential sand-silt mixtures under static loading
Failures Due to Static Loading
-
Upload
myra-buchanan -
Category
Documents
-
view
27 -
download
0
description
Transcript of Failures Due to Static Loading
1
Failures Due to Static Loading
Section IV
2
Static Loading? Failure Theories:
Maximum-Normal Stress Theory Maximum-Shear Stress Theory The Distortion-Energy Theory
Factor of Safety for each Failure Theory
Talking Points
3
Static Load is a stationary force or moment acting on a member.
Stationary means that the force or moment does not change in magnitude.
Sometime the load is assumed to be static when it is known that some variation to be expected. Such assumptions are made to simplify the design computations when variations in load are few or minor in nature.
Static Loading?
4
This theory states that failure occurs whenever the largest principal stress equals the strength.
Suppose the principal stresses are ordered as:
Then if yielding is the criteria of failure, then
failure occurs whenever:
where:
If ultimate tensile strength is used (in case of brittle materials), failure occur whenever:
where:
Failure Theoriesi. Maximum-Normal Stress Theory
Principal
Element
321
ycyt SS 31 or
stress yield ecompressiv
stress yield tensile
yc
yt
S
S
ucut SS 31 or
stress ultimate ecompressiv
stress ultimate tensile
uc
ut
S
S
Pure tensionPure torsion
Note: For pure torsion 1 = = 3 and 2 = 0. This
means that the part fails in torsion when = Sy. But
experiments show that a part in torsion will deform
at about 60% of the yield strength. This is one of
the reasons the maximum-normal stress theory is
not recommended.
5
This theory is used only in the ductile materials. It states that yielding begins whenever the maximum shear stress
becomes equal to the maximum shear stress in a tension test specimen of the same material when that specimen begins to yield.
The maximum-shear stress theory predicts that failure will occur whenever:
Shear yield strength is given by:
Failure Theoriesii. Maximum-Shear Stress Theory
torsion)pure(for 2
tension)simple(for 2
31max
1max
yy SS
3121
max or 22
ysy SS 5.0
6
This theory is called the shear-energy theory.
It is used also for ductile materials. Like the maximum-shear stress theory,
this theory is employed to define the beginning of yield. It predicts that yielding will occur whenever the distortion-energy in a unit volume equals the distortion energy in the same volume when uniaxially stressed to the yield strength.
The distortion energy is obtained by subtracting equation (5) from equation (2):
So yielding is predicted to occur when:
Shear yield strength is given by:
Failure Theoriesiii. The Distortion-Energy Theory
b) volume change c) distortion without volume change
a) both volume change and angular distortion
For figure (a): For unit cube, the work done in any of the
principal directions is: , where n= 1,2,3
The total strain energy is: or
The average value avg: The remaining stress, (1-avg), (2-avg), (3-avg)
will produce angular distortion, figure (c). Substituting (avg for 1, 2, 3) in equation (2) gives the amount of strain energy producing only volume change.
Substituting in equation (4) gives:
321
(1) 2nnnU
321 UUUU
(5) 26
21313221
23
22
21v
E
U
(3) 3321 avg
(4) 2123 2v EU avg
23212 3 avg
(2) 221 3132212
32
22
1 EU
2 where,
3
1
213
232
221
2d
EU
ysy SS 577.0
yS
7
Factor of Safety for each Failure Theory
For maximum-normal stress theory
For maximum-shear stress theory
For the distortion-energy theory:
materials) brittle(for or
materials) ductile(for or
31
31
usus
ysys
SnSn
SnSn
31 ys Sn
2 where, 213
232
221
ys Sn
8
Example A material has a yield strength of 600 MPa. Compute the fator of safety for
each of the failure theories for ductile materials. Use the following stress states:
a)- 1 = 420 MPa: 2 = 420 MPa, 3 = 0
b)- 1 = 420 MPa, 2 = 180 MPa, 3 = 0
c)- 1 = 420 MPa, 2 = 0 MPa, 3 = -180 MPa
d)- 1 = 0 MPa, 2 = -180 MPa, 3 = -420 MPa.