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7/31/2019 Curs 05 2012
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1
Reinforced and Prestressed ConcreteReinforced and Prestressed Concrete -- CC 55 --
Arh. Juergen Mayer
Arh. Santiago Calatrava
Ciudad de las Artes y las Ciencias, Valencia, Spain
Designed by Santiago Calatrava and Flix Candela
2
Rectangular Section with Compression Reinforcements
(Double Reinforced Rectangular Beams)
1) to reversal moment for the beams of a reinforced frame (the
tension reinforcement provided for the negative moment
becomes the compression steel under positive moment).
2) to increase the moment resisting capacity of the section (when is
not possible to change the dimensions of the beam).
3) to reduce the long-term deflection of an element under service
loads (when the concrete begins to creep, the compressive force
in the beam is transferred from the concrete to the steel, thus
the concrete stress is lowered and deflection due to creep is
much reduced).
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A. Design of rectangular reinforced concrete section with compression reinforcement
4
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B. Analysis of doubly reinforced
rectangular section
the resistance moment of the section:
ssccRd zFzFM += 2
x
xdcus
= 31
x
dxcus
232
=
003503 .cu =MPaGPaEs
310200200 ==
13
1 =x
d
cu
s
1
3
1 +=cu
s
x
d
13
3
scu
cu
+=
131 700
700
1020000350
00350
ss
MPa.
.
+=
+
=
the strains of the reinforcements bars are:
x
d
cu
s 2
3
2 1=
3
22 1cu
s
x
d
=
23
3
scu
cu'
=
232 700
700
1020000350
00350
ss
MPa.
.'
=
=
6
the steel in tension yields if:
the steel in compression yields if:
s
ydsE
f>1
yds fd
x
+
+==
700
700
700
700
1
s
ydsE
f>2
yds fd
x'
==
700
700
700
700
22
for tension
for compression
if the steel not yields, then the steel is in the elastic domain
and the stresses are:
== 1170011
sss E
=='
Esss
1
170022
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Example 1: The resistance moment when the tension stell yields and the compression steelis in the elastic domain:
21 scs FFF += = 0X
221 sscdyds AfxbfA +=
+=x
dAfxbfA scdyds
221 1700
2222
1 700700 dAxAfxbxfA sscdyds +=
0700700 22122 =+ dAxfAxAfxb sydsscd
0700700 22212 =
cd
s
cd
syds
fb
dAx
fb
AfAx
=
cd
sydsx
fb
AfAb
70021
1=xa
=cd
sx
fb
dAc
22 700
x
xxxx
a
cabbx
+
=2
42
8
Conclusion: the compression reinforcements is not used for calculus if :
( )2222
ddAx
dfxbM sscdRd +
=
2dx > If:
and
cds f=1
ukuds . =< 901
then
x
dxs
22 700
=
and
2dx If:
=
2
xdfxbM cdRd
then
2dx
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Example 2: double reinforced section with compression reinforcement in el astic rangeversus simple reinforced section. (C20/25, PC52)
10
cm.fb
fAx
cd
yds547
1 =
=
=
2
xdfxbM cdRd
mkN.MRd = 5422
only tension reinforcement: (Example 1 Lecture 4)
Conclusion: the increasing of the resistance moment
of a double reinforced section is small compared
with a similar section simply reinforced if the
compression reinforcement is in the elastic domain
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Example 3: singly versus double reinforced sections
singly reinforceddouble reinforced
mkN.MRd = 5422mkN.MRd = 3823
1.57cm2
0.57cm2
1.00cm2
if this difference is added to the tension reinforcement and the section is consideredas simply reinforced, then an important increasing of resistance moment is obtained:
singly reinforced
mkN.MRd = 1527
12
Example 4: if we double the reinforcing percentage of the resistance steel both in the case ofsingly and double reinforced sections, we obtain:
mkN.MRd = 5422
%.p 241=
singly
reinforced
section
mkN.MRd = 8037
%.p 472=
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mkN.MRd = 3823
Double reinforced section
mkN.MRd = 1244
the steel yields both in
tension and compression
reinforcements
mkN.MRd = 0551
the compression reinforcement
is in elastic domain (not yields)
( )222
2
ddA
xdfxbM
ss
cdRd
+
+
=
xAs1 As2( ) fyd
b fcd=
MRd b x fcd d x2
As2
fyd
d d2
( )
+
...=
14
Conclusions:
in normal reinforcing situations, the compression reinforcement not leads to a significant increase
of the resistance capacity,
to over-reinforced elements, the compression reinforcement leads to a significant increase
of the resistance capacity,
it is not economic to use compression reinforcement in a section before all the singly reinforcing
possibilities are used
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Sections with resistance reinforcements on multiple rows:
==
=c
jsjsj
t
isisicd AAfxb
11
= 0X
x
dxh i
cu
si =3
13
=x
dhE i
cu
s
si
=
= 170013
x
dh
x
dhE iicussi
x
dx j
cu
sj =3
x
dE j
cu
s
sj
=13
=
=
x
d
x
dE
jjcussj 170013
16
==
=
c
j
jsj
t
i
isicd
x
dA
x
dhAfxb
11
17001700
x - is the solution of the resulting quadratic equation
Once x calculated, the reinforcements strains and stresses values can be obtained:
for tension reinforcements:
x
dxh i
cu
si =3
=
= 1003503
x
dh.
x
dxh iicusi and
ssisi E= ifs
ydsiE
f
ydsj f= ifs
ydsjE
f
The resistance moment can be calculated with the following relation:
====
++=++=c
jsjsjsj
t
isisisiccd
c
jsjsj
t
isisiccRd zAzAzfxbzFzFzFM
1111