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ACES Workshop: Innovative Materials and
Techniques in Concrete ConstructionHoliday Palace Hotel, Corfu (GR) - October 10-12, 2010
Sustainable Roof elements:
a proposal offered by cementitious
composite technology
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. ZaniPolitecnico di Milano, Department of Structural Engineering
� research significance
� material properties
Outline
� material properties
� sandwich plates: test results
� open problems
� concluding remarks
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
uplifting device
TRMPolystyrene
HPFRCC
• small weight (about 70 kg/m2)
• high quality finishing
Main advantages P (kN)
2.5 m
1.25 m
P P
6
δ
4
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
• high quality finishing
• good fire resistance
• high insulation
• no need of waterproofing layer δ (mm)9 36
6040
4
Dosage (kg/m3)
Cement type I 52.5 600
Slag 500
Water 200
Table 1 Composition of mix
HPFRCC material
Water 200
Superplasticizer 33 (l/m3)
Sand 0-2 mm 983
Fibers (lf = 13mm;
df = 0.16mm)100 730-800 mm
> 750 mm
γ = 2450 – 2530 kg/m3
R = 66.3 Mpa
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
Rcm, 24h = 66.3 Mpa
Rcm, 7d = 99.1 Mpa
Rcm, 28d = 116.5 Mpa
Esm = 45249 Mpa
5EXPERIMENTAL PROGRAM : MANUFACTURING
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
40 mm
30 mm
Temperature exposure2h
12°C/h
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
30°C/h in the heating process
7Bending tests on unnotched flow-oriented fibres specimens
600 °C400 °C200 °C20 °C
N[MPa]
30
27.5
25
22.5
20
17.5
15
12.5
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
COD [mm]
σN[M
9876543210
12.5
10
7.5
5
2.5
0
Polystyrenemortar
F
δ1,δ2 δ3,δ4
60
20
A A
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
F
Spacing
[mm]
Weight
[g/m2]
Failure load
[N/m]
Max elongation
[%]
Gross
mesh
Coated
mesh
Warp Weft Warp Weft
4.5x5.0 125±5% 155±5% 40000 46000 4.5±1 4.5±1
TRC
AR Glass fabric
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
dg,max = 0.6 mm
Two overlapped layers
0.6 mm
P (N)70 mm
10
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
δ (mm)
ρgf ~ 5%
Pcr,th= 3.5 kN
25
AR Glass Fabric
Textile Reinforced Concrete Under static loading
Courtesy by Alva Peled
10
15
20
nsi
le S
tres
s, M
Pa
AR Glass FabricVf = 4.5%
GFRC Vf =5%
Short glass fibers
Tensile static test
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
0 0.01 0.02 0.03Strain, mm/mm
0
5Ten
Fabrics exhibit:
• high resistance under static
loading
• multiple cracking with small
opening
Plain matrix
Cement
Composite
laminates board
Squeezed
rollers
Fabric
locationPultrusion Technology
Cement
bath
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
Peled & Mobasher, 2003
Full Scale Structural Tests
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
P (kN) P (kN)
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
δ (mm) δ (mm)
P (kN)M
(kNm)
P (kN) P (kN) P (kN)
δ (mm) θ (mm-1)*10-5
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
δ (mm)
δ (mm) δ (mm)
M(kNm/m)
sandwich plate
sandwich beam
M(kNm/m)
UHPFRC plate
sandwich plate
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
θθθθ (mm-1)*10-5 θθθθ (mm-1)*10-5
Technological and design problems
• fiber orientation is a technology in progress (large
scattering in the bending response) scattering in the bending response)
• production of suitable AR glass fabrics is in progress
• polystyrene could be substituted by other materials with
better energy performance
• which design parameters for UHPFRC (SLS and ULS)?
• which characteristic length for Textile?
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
• which characteristic length for Textile?
• which model to predict the experimental behavior?
beam
T2
beam
T1
50 150150150 500
beam L2
beam L1 015
015
050
casting
direction
T1-BT2-B
T1-AT2-A L1-A
L2-AL2-B
L1-B
10
15
20
25
[MPa]
beam L1
150
supposed flow lines
T1-AT2-A L1-AL1-B
Slab A
20
30
mm
2)
beam L1
beam L2
500 mm - 20 in.
150 mm - 6 in.
200 mm - 8 in.
A
A sect. A-A
150 mm
6 in.
30 mm - 1.2 in7 mm
0 1 2 3
0
5 20° C
20° C av
3.6
COD [mm]
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
0 2 4 6 8 10
COD (mm)
0
10
σN (N
/m beam L1
beam T2
beam T1
450 mm - 18 in.
200 mm - 8 in.
σ
0.9 fIf/β
σN,peak/β1
arctg E
25+2h0.7
2h0.7
Ec = 22000 (fc/10)0.3 = 43600 N/mm2
for fc = 96 N/mm2
= 2.16 (for h = 30 mm)β =
ε
M = σN,peak bh2/6
σ
εpeak σpeak
0.9fIf/β
Εχx
χ
x
500 mm - 20 in.
150 mm - 6 in.
450 mm - 18 in.
200 mm - 8 in.
A
A
7 mm
σ
σN, peak
κ1 feq,2 0.10
ε
M = feq (0.1h) bh2/6σ(0.02)
σσpeak
Compression
force0.02
σ(0.10)
β1
ε
M = feq2 bh2/6
σ(0.02)
σ
0.02
σpeakχ
x Εχx
12
16
mm
2)
beams L1/2
slab A
DEWS L1/2-B
12
16
mm
2)
beams L1/2
slab A
DEWS L1/2-B
εεpeak = CMODpeak
lCOD
arctg Ec
for fc = 96 N/mm
crack opening w0.02 h
κ2 feq, wu
wu = 0.10 h
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
0 0.002 0.004 0.006 0.008 0.01
strain ε
0
4
8
σ (N
/m
arctg Ec
DEWS T1/2-B
0.6 3
crack opening w (mm)
0
4
8
σ (N
/m
0 3 6 9
DEWS T1/2-B
Standard specimen test
UNI 11039PIf
U2U1
P
CTOD
P’F
l/2 l l/2l l
45
mm l
l
l=150 mm
l
CTOD0 CTOD0+3mm CTODCTOD
[mm]+0.6 + 3.0
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
fIf ,av = 7.10 Mpa
feq 0-0.6 = 12.06 Mpa
feq 0.6-3 = 9.76 Mpa
22STATE OF ART: THE MATERIAL
HPFRCC at low strain rates
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
� small specimens tested
� increasing the specimen size the material homogeneity decrease
� A standard does not
The ultimate tensile strength fFtu in the linear model depends on
the required ductility that is related to the allowed crack width.
Ultimate COD condition: a ductility requirement
The ultimate crack width can be calculated as
wu = lcs * εεεεFu
by assuming εFu equal to 2% for variable strain distribution
along the cross section and 1% for only tensile strain
distribution along the cross section.
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
distribution along the cross section.
The max. crack width may not exceed 2.5 mm.
wu* = (0.02 - εpeak) *h + εpeakLCOD
24TEST RESULTS: RESIDUAL STRENGTHS
Temperature [°C]
Sample number
fIf [MPa]fIf,av[MPa]
(std)feq1
[MPa]feq1,av[MPa]
(std)feq2
[MPa]feq2,av[MPa]
(std)
20 1 11.5011.30(0.35)
16.4115.98(0.46)
22.5422.81(0.39)
20 2 11.50 15.50 23.26
20 3 10.90 16.02 22.63
200 1 9.51 17.46 23.29
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
200 1 9.519.10
(0.36)
17.4617.37(0.22)
23.2923.42(0.47)
200 2 8.91 17.12 23.94
200 3 8.88 17.53 23.02
400 1 5.544.93
(0.53)
15.0313.97(0.93)
21.9223.23(1.92)
400 2 4.65 13.53 25.44
400 3 4.59 13.35 22.31
600 1 4.784.64
(0.19)
13.6113.16(0.47)
3.644.36
(1.36)600 2 4.72 13.20 3.51
600 3 4.42 12.67 5.92
25Interpretazione dei risultati
1. Imbarcamento dei provini dovuto a fenomeni di ritiro plastico
2. Effetto dimensionale
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
3. Presenza di difetti
σS
p=
6m
m
A
A
Sezione AA
26Interpretazione dei risultati
4. Fenomeni di scorrimento del rinforzo
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
exp.
model Which characteristic length
for TRC material?
� weft spacing� weft spacing
� layer thickness
� is it variable?
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
Which models ?
Plane section
exp. results (average)
exp. results (envelope)
M(kNm/m)
exp. results (envelope)
exp. results (average)
exp. results (envelope)
FE model (ch. length = 400 mm)M(kNm/m)
θθθθ (mm-1)*10-5
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
UHPFRCC elements
Polystyrene elements
TRC elements
FE model (ch. length = 400 mm)
FE model (ch. length = 400 mm)
M(kNm/m)
θθθθ (mm-1)*10-5
Concluding Remarks
•� Light and sustainable roof elements can be produced
and they improve fire resistance and lightness with and they improve fire resistance and lightness with
reasonable costs;
� structural specimen is needed to characterize thin
structural elements, but DEWS tests allows the use of
compression test to identify softening behavior in
uniaxial tension and characterize material orthotropy;
� TRC can be improved in order to increase the total
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani
� TRC can be improved in order to increase the total
load at SLS: its characteristic length has to be identified
� plane section model seems able to fit reasonably
experimental results, while FE model requires further
improvements
ThankThank youyou forfor youryour attentionattention!!
M. di Prisco, A. Caverzan, L. Ferrara, M., A. Magri, G. Zani