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(a)
(b)
(c)
τ″
x
x 1
F
F
F
SH
L
L
L
SH
SH
θ″
RH
m
RH
m
m
RH
Figure 4.5 Determination of the displacements in the FAM: (a) Elastic displacement; (b) Plastic
bending displacement; (c) Plastic shear displacement.
4.2.2 Plastic Bending Displacement x 0 1
Assuming that there is no elastic displacement and the SH is locked, as shown in Figure 4.5(b),
the RH rotates θ 00 , which is the plastic rotation due to bending behavior, while other parts of the
system remain rigid. According to the kinematic relationship, the plastic bending displacement
x 1 00 can be written as:
x 0 1 = θ 00 L
ð4 : 10Þ
4.2.3 Plastic Shear Displacement x 0 2
Similar to the procedure for x 00 1 , as shown in Figure 4.5(c), assume that there is no elastic
displacement of the system and the RH is locked. The SH begins to slide due to the lateral
load F , while other parts of the SDOF system remain rigid. Then the plastic shear displacement
x 0 2 equals to the sliding
τ 00 of SH, which is the plastic shear deformation due to shear
behavior as:
x 0 2 = τ 00
ð4 : 11Þ
4.2.4 Combination of the Bending and Shear Behaviors
The displacement decomposition and inelastic mechanisms of the SDOF system subjected to
the lateral load F are illustrated in Figure 4.6, in which the displacement x contains the elastic
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