PSI - Issue 11
Gloria Terenzi et al. / Procedia Structural Integrity 11 (2018) 161–168
166
6
Terenzi G,
Costoli I, Sorace
S, Spinelli P / St
ructural Integrity
y Procedia 00 (2
018) 000–000
beam dam syst acco
s consists in aged welds f em in 16 ver rding to the c
welding sh rom the risk o tical alignmen riterion discu
aped plates o f collapse. Th ts, all adjace ssed in the fo
n the diagona e global seis nt to the buil llowing sectio
l profiles ov mic retrofit st ding corners. ns.
er their entir rategy is repr The incorpo
e length, in o esented by th rated FV dev
rder to prote e installation ices were des
ct the of the igned
SDE FDE
BDE
BDE
FDE
LS
LS
MCE
SDE
MCE
OP
OP
Storey
Storey
DL
DL
Y Direc
tion
X Di
rection
a )
b )
ix
iy
Fig. 6. C
urrent condition
s. Normalized int
erstorey drift env
elops in X ( a ) an
d Y ( b ) direction
s for the four seis
mic levels.
1. Mechanica e dissipative ure 3), on th storey. A vi dampers are trated by the
l characterist braces were e ground stor ew of the fini installed in p drawings in t
ics of FV dev incorporated ey, and the B te element m airs at the tip he same Figu
ices in the B2-B3 1-C1, B2-B3 odel includin of the supp re.
4. Th
, B2-C2, B5-B , B5-B6, B7-C g the seismic orting diagon
6, B6-C6, E 7, E1-F1, E7 protection sy al trusses, wi
2-F2, E6-F6, -F7, F5-F6, stem is show th inverted V
F2-F3, F5-F6 F2-F3 bays, o n in Figure 7 -shaped layo
bays n the . The ut, as
(Fig first FV illus
Fig.
7. Finite elemen
t model of the bu
ilding incorporat
ing the dissipativ
e bracing system
and installation
details.
D effe beh 199
ifferently from cts, which re aviour of FV 9; Sorace and � = 2 ( ) = F t k x ne t
other classe presents an e devices is ch Terenzi 2001 � � ( �| � ( | k k )
s of dampers ffective prop aracterized by ): �
, FV devices erty for rathe the followin
provide a ver r stiff structu g damping an
y high dissipa res, like the d elastic resp
tive action w case study on onse force co
ith small stiff e. The mech mponents (Te
ening anical renzi
(1) (2)
5 1/5 ) ( ) x t
1 ( ) (
1 + + −
2
0 F k x t 1 (
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