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=
sEI = L scEI = L
scEI = L sEI = L
1718 : 1 1076 : 0
1076 : 0 1718 : 1
K 0 o =
ð7 : 138bÞ
Then, the governing equations of the FAM in Eqs. (7.128) and (7.129) become
=
x k +1
Δθ 0 1
Δθ 0 2
θ 0 1
θ 0 2
m 1
m 2
1718 : 1 1076 : 0
1076 : 0 1718 : 1
698 : 5
698 : 5
1718 : 1 1076 : 0
1076 : 0 1718 : 1
+
k +1
k
ð7 : 139Þ
θ 0 1
θ 0 2
1
224 : 3 698 : 5
x 0 k +1 =
½
698 : 5
ð7 : 140Þ
k +1
At the axial compressive force of P = 500 kN, assume that the yieldmoments are m y 1 = 200 kNm
and m y 2 = 220 kNm. Let both plastic hinges exhibit bilinear kinematic hardening behavior with
K t 1 = 300 kNm/rad and K t 2 = 200 kNm/rad, then the corresponding moment versus plastic rota-
tion relationships can be written as:
θ 0 1 =0
m 1 = 200 + 300 × θ 0 1
m 1 ≤ 200
m 1 > 200 ,
ð7 : 141aÞ
if
then
θ 0 2 =0
m 2 = 220 + 200 × θ 0 2
m 2 ≤ 220
if
m 2 > 220 ,
then
ð7 : 141bÞ
60
300
Inelastic
Elastic
Inelastic
Elastic
40
200
20
100
0
0
-20
-100
-40
-200
-60
-80
-300
0
5
10
15
20
0
5
10
15
20
Time (s)
Time (s)
1.5
5
Inelastic
Elastic
0
1
-5
-10
0.5
-15
0
-20
-25
-0.5
-30
-35
-1
-40
-1.5
-45
0
5
10
15
20
0
5
10
15
20
Time (s)
Time (s)
Figure 7.14 Global responses of the SDOF column with geometric nonlinearity.
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