Civil Engineering Reference
In-Depth Information
The tensile strain
ε r can now be checked:
Equation 15
ε r
= ε + ε t ε d =
0
.
00798
+
0
.
00234
+
0
.
0005
=
0
.
01082
0
.
0108 (assumed) OK
Check
σ 1 :
Equation 9 a
f =
413 MPa (extensively yielded since
ε =
0
.
0079
0
.
00207)
Equation 10 a
f t
=
413 MPa (shortly after yielding since
ε t =
0
.
00234)
ρ f =
0
.
0103(413)
=
4
.
26 MPa
ρ t f t
=
0
.
0103(413)
=
4
.
26 MPa
=
ρ t f t )
+
ρ f )
=
.
.
.
.
=
B
m (
m t (
0
5(4
26)
0
5(4
26)
0
C
=
(
ρ f )(
ρ t f t )
=
(4
.
26)(4
.
26)
=
18
.
15 MPa
B
4 SC
15)
B 2
(0) 2
1
2 S
1
σ 1 =
±
=
±
.
Equation 17
0
4(
1)(18
2(
1)
=−
0
.
5(
8
.
52)
=
4
.
26 MPa
=
4
.
26 MPa (assumed)
OK
ε d ,
ε r ,
ε , and
ε t and the stresses,
σ d and
σ 1 , are calculated from the
Now that the strains
trial-and-error process, we can determine the angle
α r , the shear stress
τ t and the shear strain
γ t :
ε t ε d
ε ε d =
0
.
00234
+
0
.
0005
Equation 16 tan 2
α r
=
0005 =
0
.
334
0
.
00798
+
0
.
tan
α r
=
0
.
577
30
60
α r
=
2
α r =
τ t
=
σ d )sin
α r cos
α r =
.
.
.
Equation 3
(
(8
54)(0
500)(0
866)
=
3
.
69 MPa
Equation 6
γ t /
2
=
(
ε r ε d )sin
α r cos
α r
=
(0
.
0108
+
0
.
0005)(0
.
500)(0
.
866)
=
0
.
00489
The applied stresses at the level near ultimate where both steel have yielded are:
σ =
m σ 1 =
0
.
5(4
.
26)
=
2
.
13 MPa
σ t
=
m t σ 1 =−
0
.
5(4
.
26)
=−
2
.
13 MPa
τ t
=
m t σ 1 =
0
.
866(4
.
26)
=
3
.
69 MPa
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