Technical Papers
Oct 23, 2020

Axial Stress–Strain Model for FRCM Confinement of Masonry Columns

Publication: Journal of Composites for Construction
Volume 25, Issue 1

Abstract

Masonry columns often exhibit a lack of load-carrying capacity that is due to overloads and do not provide any ductility or dissipation capacity under seismic forces. Column confinement has been extensively studied as an effective technique, which could mitigate these structural vulnerabilities. The confinement of masonry columns will be studied in this paper, by considering fabric–reinforced cementitious matrix (FRCM) materials as external jackets. Due to the lack of information in the scientific literature, a new analysis-oriented model (AOM) for the prediction of the axial stress–strain law will be presented and discussed in this paper. The proposed AOM consists of a system of equations that make several assumptions: crossing the predicted peak point (strength and relative strain), crossing the ultimate point (80% residual strength and relative strain), and the horizontal tangent at the peak point and the initial (linear elastic) slope derived from the geometry and mechanical properties of the materials involved. The AOM was demonstrated to be simple and accurate, based on Pearson's test (χ2); therefore, the proposed approach could be considered for future design equations. In addition, this paper will illustrate and discuss the validation of two available design-oriented models (DOMs), which could predict the axial strength of FRCM jacketed columns, by comparing the theoretical results with a database of experimental results that is available in the scientific literature. Novel formulas for the computation of both the peak and ultimate axial strains will be further proposed, as the basis for a design procedure. Their accuracy was demonstrated by considering an experimental versus theoretical comparison.

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Acknowledgments

The authors want to acknowledge the important support of the RELUIS program 2019–2021, funded by the Civil Protection Department of the Italian Government.

Notation

The following symbols are used in this paper:
Ac
net cross-sectional area of the compression member equal to bxh (mm2);
Ae
area of the effectively confined concrete (mm2);
a, b, c, d, e, f, g
constants of the polynomial equation of the simplified AOM (dimensionless);
cb
spacing between the bars (mm);
cbs
spacing between the bars and the border of the cross section (mm);
D
diagonal of the cross section of the column assumed equal to the square root of the sum of the squares of width and length of the cross section itself (mm);
Ef
slope of the cracked behavior of the FRCM in tensile stress state; approximately equal to Young modulus of the fabric (MPa);
Em
Young's modulus of the unconfined column (MPa);
e
expected value in the χ2 test;
f(x)
PDD of the variable x (dimensionless);
fc
generic axial stress of the FRCM-confined column related to ɛc (MPa);
fc,mat
average compressive strength of the FRCM matrix (MPa);
fccm,ex
experimental compressive strength of the FRCM-confined masonry column (MPa);
fccm,th
theoretical compressive strength of the FRCM-confined masonry column (MPa);
fl
confining pressure (MPa);
fl,eff
effective confining pressure (MPa);
fm
average compressive strength of the unconfined masonry column (MPa);
fmu
characteristic (i.e., calculated as the 5% fractile) compressive strength of the unconfined masonry column (MPa);
fmud
design compressive strength of the unconfined masonry column calculated as fmu divided by a safety factor equal to 2.0 in agreement with the Eurocode provisions (MPa);
gm
mass density of the masonry (kg/m3);
h
height of the cross section of the column (mm);
k
dimensionless confinement effectiveness coefficient;
k′′
reduction factor for the ultimate axial strain of the FRCM-confined masonry column (dimensionless);
kb
efficiency factor computed as =(Ae/Ac)(h/b)2;
kH
cross section shape factor (dimensionless);
kmat
dimensionless coefficient affecting the confining pressure to achieve the FRCM matrix effect;
nb
number of bars introduced in the masonry (dimensionless);
nf
number of FRCM layers (dimensionless);
o
observed value in the χ2 test;
R2
coefficient of determination calculated by comparing experimental and analytical axial stress–strain curves (dimensionless);
rc
radius of curvature after the rounding of the edges (mm);
tf
equivalent thickness of the fabric (mm2/mm);
tmat
total thickness of mortar (mm);
w
width of the cross section of the column (mm);
x
fccm,ex/fccm,th (dimensionless);
α1, α2, α3, α4, α5, α6, α7, α8
dimensionless coefficient assumed equal to 0.5, 1, 1, 1.81, 0.7, 2.2, and 0.5 respectively;
γf
fabric reduction factor (dimensionless);
γk
compressive strength safety factor (dimensionless);
γm
masonry reduction factor (dimensionless);
ɛc
generic axial strain of the FRCM-confined column (dimensionless);
εc
compressive strain of the unconfined concrete that corresponds to fc (dimensionless);
ɛcc
ultimate axial strain of the FRCM-confined concrete column according to ACI-549.4R (ACI 2013) (dimensionless);
ɛccm
peak axial strain of the FRCM-confined masonry column (dimensionless);
ɛccmu
ultimate axial strain of the FRCM-confined masonry column (dimensionless);
ɛccu
ultimate axial compressive strain of FRCM-confined concrete according to ACI-549.4R (ACI 2013) (dimensionless);
ɛfe
effective tensile strain level in the FRCM limited to the minimum of the design tensile strain of the FRCM itself and 0.012 according to ACI-549.4R (ACI 2013) (dimensionless);
ɛfu
rupture strain of FRCM in tensile stress state; approximately equal to the ultimate strain of the fabric (dimensionless);
ɛfud
design value of the ultimate tensile strain of the FRCM (dimensionless);
μ
mean value of the x variable (dimensionless);
ρf
geometrical percentage of FRCM fabric (dimensionless);
ρmat
geometrical percentage of FRCM matrix (dimensionless);
σ
SD related to the x variable (dimensionless): and
χ2
Pearson's chi-squared test (dimensionless).

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Journal of Composites for Construction
Volume 25Issue 1February 2021

History

Received: Mar 16, 2020
Accepted: Aug 5, 2020
Published online: Oct 23, 2020
Published in print: Feb 1, 2021
Discussion open until: Mar 23, 2021

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Dept. of Innovation Engineering, Univ. of Salento, Lecce 73100, Italy. ORCID: https://orcid.org/0000-0002-1751-7343. Email: [email protected]
Gennaro Maddaloni [email protected]
Dept. of Structures for Engineering and Architecture, Univ. of Naples “Federico II”, Naples 80125, Italy. Email: [email protected]
Fabio Longo [email protected]
Dept. of Innovation Engineering, Univ. of Salento, Lecce 73100, Italy (corresponding author). Email: [email protected]
Andrea Prota [email protected]
Dept. of Structures for Engineering and Architecture, Univ. of Naples “Federico II”, Naples 80125, Italy. Email: [email protected]

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