Example of Determination of the Traction Within a Steel Retrofit Tendon for a Masonry Wall
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Transcript of Example of Determination of the Traction Within a Steel Retrofit Tendon for a Masonry Wall
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1.1 Example of determination of the traction within a steel
retrot tendon for a masonry wall
In this paragraph an example of calculation of the force within a retrofit tendon for a masonry wall
will be shown. The tendon is meant to prevent the out-of-plane overturning of a masonry wall of a
two story masonry building, shown in Figure 1. In order to perform calculations earthquaes
referring to the following !ones will be too into consideration"
Locatio
n
Class of use Type of soil
Ferrara III #
$imini III %
&quila III %Table 1 Sesmic zones, class of use, type of soil.
Figure 1 asonry building considered in the example.
1. Calculation of the tendon
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'oad analysis
$oof"
(ermanent load" qp) * + dam)
/ariable load" qac) * 100 da m)
Floor"
(ermanent load" qp1 * 11 dam)
/ariable load" qac1 * )00 dam)
& specific weight for the masonry of 2 * )000 dam3will be assumed.
In Figure )the static scheme of the forces acting on the wall is reported.
The geometrical specifications of the wall are as follows"
b1* 0.44 m
b) * 0.50 m
d1 * 0.54 m
d) * 0.30 m
h1 * 3.30 m
h) * 3.30 m
& constant stress distribution on the overturning section will be
assumed. The stress will be equal to the crushing stress of the masonry,
i.e. 6 * )0 dacm).
The length of the stress bloc is given by the equilibrium equation"
s
Nc
k.=
'et7s consider the overturning mechanism at the first floor. For the sae of safety, only permament
loads will be considered within the calculation of 81 and 8). The load interaxes for the first floor
and the second floor are respectively"
i1 * ).)3 m
i) * 1.) m
Figure ! "alculationscheme
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Calculation of stabilizing forces.
'et7s consider a portion of wall with a length of 1 m, 81 and 8) are"
81 * qp1 9 i1 9 1 * 34: da
8) * qp) 9 i) 9 1 * 151 da
Thus the length of the stress bloc is"
2
2 0.014.
k
Sc m
ss= =
The proper weights of the two walls are"
(1 * )000 9 3.3 9 0.44 9 1 * 330 da
() * )000 9 3.3 9 0.50 9 1 * )50 da
Calculation of the unstabilizing forces.
'et7s now calculate the seismic acceleration associated to the location of Ferrara. & nominal life /n
* 40 years will be assumed. If the class of use is III, %u will be equal to 1.4. Thus it follows that /r
* 40 9 1.4 *4 anni.
The probability of exceeding the intensity of the design earthquae in the reference period /r
related to the life limit state is equal to (/$*10;, with a return period of"
and the following
elastic spectra"
Ferrara #soil $%
&imini #soil
"%
'(uila #soil
"%
ag/g 0.162 0.212 0.3
F0 2.567 2.507 2.384
Tc*
0.276 0.304 0.356
Ss 1.776219 1.3811096 1.27088
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Cc 2.379334336 1.555396139 1.476422992
St 1 1 1
S 1.776219 1.3811096 1.27088
Figure ) Elastic spectra
The 8s and %c parameters are chosen following T% )00+ prescription"
The parameter 8, is calculated as 8 * 88 9 8T. In the paragraph .+.1.4.) of T%)00+ prescribes the
following equivalent static forces"
awa
a
aa WW
q
SF .. ==
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where"
?a * weight of the element.
qa * 3
2
1
. 3(1 / )
. 0.51 (1 / )
g
a
a
a S Z H
S g T T
+= + !
@ * centroid quota of the non structural element measured from the foundation.
A * height of the building measured from the foundation.
Ta * 0
In the following table the values of 8a and Bw for the two walls in each reference location are
shown"
Ferrara Rimini Aquila
8a1 0.3: 0.503 0.4)5
8a) 0.11 0.)) 0.+10
Bw1 0.13) 0.135 0.14Bw) 0.)05 0.)0 0.)0
The masses excited by the earthquae, are given by the formula"
++ kjj!! ))1
?here the values of C)Dare defined by T%)00+"
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Thus, for the first floor it is C)D* 0.3 =category &< whilst for the roof it is C)D* 0. Easses referred
to first floor and roof floor are respectively ?1* 5:3 da e ?)* 151 da.
8tatic force to be applied to each mass is given by"
=j
jjiihi WzWzFF ..
%oefficients 2ito be applied to each force are"
#$1
0,52702
9
#%1
1,05405
7
#$2
1,58108
6
#%2
2,10811
5
Thus, corresponding forces are equal to"
F$1
1913&1
14
F%1 519&47
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11
F$2
4174&0
67
F%2
297&11
77
2. Overturning assessment
"#erturning aroun$ %oint &'(
The tractions T1and T) for the Ferrara location are being calculated. 8tabili!ing moment is given by"
))))
))
)) .)))
hTcb
Pc
$S)stab +
+
=
)stab* 151 9 0.): )50 9 0.1: T) 9 3.3 *45).4 T) 9 3.3
Gverturning moment is given by"
+=
).. )))))h
FhF) %wwrib
)rib* Bw)=):,11.3,3 515,1.1,4< * Bw)9 ++
Thus"
T** Bw)9 )3+5.) H 15.5
eeping in mind that Bw)* 0.)05, it follows that"
T** 31: da
"#erturning aroun$ %oint +'(
11)1)11
11
111)
)1
))
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T1* B 9 +331H 1131.5 * 41 da
&ssuming a steel resistance of 6f* )500 dacm)the section of the tendon for unit length of the
wall is""
&1* T1 6f* 4+)500 * 0.)3+ cm)m
&)* T) 6f* 31:)500 * 0.133 cm)m
Aere7s reported the values of the tractions in the tendons for the three locations.
Ferrara Rimini LAquila
T1 KdamL 41 00 11))
T) KdamL 31: 3)+ 5
&tir1
Kcm)mL
0.)3+ 0.)40 0.5+
&tir)
Kcm)mL
0.133 0.13 0.1::
1.2 !"ample of calculation of a CFR# reinforcement $ithin a ringing retrofit
intervention for masonry %uildings
Figure & !"ample of the use of CFR# in the retrofit of masonry %uildings
'et7s assume that the wall at ris of overturning has a length of6l =
m and eeping in mind the
values of the tractions within the tendons calculated in the previous paragraph"
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Ferrara Rimini LAquila
T1 KdamL 41 00 11))
T) KdamL 31: 3)+ 5
The force that the %F$( reinforcement is given by
/ 2i
F T l= '
, thus the forces acting on the
reinforcements in the three location are"
Ferrara Rimini LAquila
T1 KdaL 11) 1+01 33
T) KdaL :4 :+3 1531
The reinforcement for the ground floor wall in $imini and l7&quila is being calculated. The F$(
properties will be assumed as follows"
'oung (odulus !
)da*+cm2,
Traction Resistance -t
)da*+cm2,
%arbon Fiber )30 x 105 541 x 10)
The reinforcement will be designed in both cases of good and low quality masonry.
In the first case, a masonry characteristic compression resistance of40bkf =
E(a will be assumed,
with mortar of class E14 i.e. with a characteristic compression resistance of
14.3k mk
= =
E(a.
Introducing the suitable safety factors the design compression resistance will thus be
7.15bd
f =
E(a and the average traction resistance will be assumed lie 110 of the compression resistance"
1.43mtm
f =
E(a.
In the second case, a masonry characteristic compression resistance of
5bk
f =
E(a will be
assumed, with mortar of class E14 i.e. with a characteristic compression resistance of
3.5k mk
= =
E(a. Introducing the suitable safety factors the design compression resistance will
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thus be
1.75bd
f =
E(a and the average traction resistance will be assumed lie 110 of the
compression resistance"
0.35mtm
f =
E(a.
The reinforcement will be designed both considering the masonry resistance and the bric
resistance. & one-directional carbon fiber strip of Type % will be used, thus its equivalent thicness
will be =cfr. point ).3.) #T )00)005
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-
/ 2fd b mk mtm m
s c k g* = ' ' ' '
-
fs
is the interface sliding, between 0.1-0.3 mm. 'et7s assume
0.2f
s =
mm.
-
0.06lc =
from experimental tests.
-b
k
is a geometric factor, assumed 1.
-rd
g
is a partial coefficient in case of applications of type J.
The height of the reinforcement
fb
may also be obtained through the following formula giving the
average failure loadP
"
f eP b lt= ' '
wheret
may be assumed equal to the traction resistance of masonry. & further formula for the
evaluation off
b
is the following"
(a) 2
F b E t = ' ' ' '*
where mk mtmc * = ' '
. In the following tables the value offbfor three different values of
acting force 1000, )000 e 3400 da using respectively the three formulas presented"
OO/ 0ALT' (A3O*R' OO/ 0ALT' 4RC5
F )da*, %1)mm, %2 )mm, %6 )mm, %1 )mm, %2 )mm, %6 )mm,
1000 445 0 : 331 3 51
)000 110: 1)0 13+ 3 ) +)
3400 1:50 )10 )51 110 1) 155
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LO7 0ALT' (A3O*R' LO7 0ALT' 4RC5
F )da*, %1 )mm, %2 )mm, %6 )mm, %1 )mm, %2 )mm, %6 )mm,
1000 11)0 1)1 13: :3 101 11
)000 ))51 )5) )+ 1+4 )03 )33
3400 3:)1 5)5 5+ 3)+1 344 50+