Technical Papers
Jun 20, 2023

Numerical Simulations and Simplified Design Approaches for Large-Rupture-Strain FRP-Strengthened Reinforced Concrete Beams under Impact

Publication: Journal of Composites for Construction
Volume 27, Issue 5

Abstract

Due to the ductile properties of large-rupture-strain fiber-reinforced polymer (LRS-FRP) laminates and their confined concrete, the failure patterns and ultimate deformation capacities of LRS-FRP-strengthened reinforced concrete (RC) beams were considerably different from those of their carbon FRP (CFRP)-strengthened counterparts under static and impact conditions. This study investigates the dynamic behaviors of LRS-FRP-strengthened beams under impact using high-accuracy numerical models and simplified analytical approaches. First, high-fidelity finite-element (FE) models were created to evaluate the static and impact responses of LRS-FRP-strengthened RC beams with varied failure patterns recorded in prior experiments. Subsequently, based on the validated FE model, the effects of critical variables, such as impact energy, longitudinal FRP strengthening ratio, wrapping length, and types of FRP, on the dynamic response were investigated. In addition, a simplified design model for a rapid evaluation of the performance and safety conditions of FRP-strengthened RC beams under impact was presented, which considered the energy conservation during the impact process, material strain rates, and influences of failure patterns. Extensive data from the static and impact tests with various failure patterns were used to verify the accuracy of the model. Finally, the simplified model yielded an impact mass/impact velocity (mv) diagram, demonstrating that LRS-FRP-strengthened RC beams outperform their CFRP counterparts in terms of anti-impact performance by obtaining a larger ultimate deformation capacity and greater safety margin.

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Acknowledgments

This research was supported by the National Natural Science Foundation of China (Grant Nos. 52178292 and 52090084).

Notation

The following symbols are used in this paper:
Asc
area of the compression reinforcement;
Ast
area of the tensile reinforcement;
Af
area of the FRP;
a
height of equivalent concrete stress block;
as
distance from the beam top to the center of the compression reinforcement;
b
beam cross section width;
bc
width of the loading plate;
c
height of concrete in the compression zone;
d
effective height of the beam section;
ED
dissipation energy consisting of deformation energy of the beam;
Ecd
dynamic elastic modulus of concrete;
Ef
elastic modulus of FRP;
Ei
inputted impact energy;
Ek
kinetic energy of the hammer;
EL
energy loss due to hammer–beam collision;
EP
potential energy of the hammer and beam;
Es
static energy-dissipating capacity;
Esc
elastic modulus of the compressive steel bar;
Est
elastic modulus of the tensile steel bar;
fc
peak stress of the unconfined concrete;
fc1
peak stress of the confined concrete;
fcd
dynamic compressive strength of concrete;
fla
actual ultimate confining stress;
fscd
dynamic compressive stress of steel;
fstd
dynamic tensile stress of steel;
futd
ultimate strength of the tensile rebar;
fytd
dynamic yield stress of the tensile rebar;
g
acceleration of gravity;
h
height of the beam;
k
elastic depth to the cracked neutral axis;
L
beam span;
Lp
plastic hinge length;
Ln
distance between the two loading points;
mbe
equivalent mass of the beam in elastic deformation stages;
mbp
equivalent mass of the beam in plastic deformation stages;
mh
mass of the hammer;
My,f
contribution of FRP for the yield moment;
My,st
contribution of tensile reinforcements for the yield moment;
n
ratios of dynamic elastic moduli of the tensile reinforcement to that of concrete Ecd;
n
ratios of dynamic elastic moduli of compressive reinforcement to that of concrete Ecd;
nf
ratios of dynamic elastic moduli of FRP to that of concrete Ecd;
Pmax
maximum impact load;
Pu
ultimate resistance;
Py
bearing capacity at the yield point;
tf
thickness of the FRP;
vc
velocities of a drop hammer after collision;
vi
initial velocity of the hammer;
w
wrapping length of transverse FRP strips;
β1
height factor of equivalent concrete stress block;
ε˙c
strain rate of concrete;
ɛc1
strain corresponding to the peak stress of confined concrete;
ɛf
strain of the FRP;
ε˙f
FRP strain rate;
ɛfu
rupture strain of the longitudinal FRP laminate;
ɛsc
strain of the compressive steel bar;
ε˙sc
strain rate of the compressive steel;
ε˙st
strain rate of the tensile steel;
ɛsu
ultimate strain of the tensile rebar;
ɛyd
dynamic yield strain of reinforcement;
ɛyt
yield strain of the tensile rebar;
δ
midspan deflection;
δ˙
deflection rate of the midspan section;
δmax
maximum midspan deflection;
δu
ultimate deflection;
δre
residual deflection under impact;
δy
deflection at the yield point;
ϕ˙
curvature rate of the midspan section;
ϕs
curvature corresponding to the ultimate state;
ϕy
curvature corresponding to the yield state;
λ
factor depending on the load distribution;
ρ
tensile reinforcement ratio;
ρ
compression reinforcement ratio;
ρb
density of the beam;
ρf
FRP reinforcement ratio; and
σf
tensile stress of FRP.

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Journal of Composites for Construction
Volume 27Issue 5October 2023

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Received: Jun 15, 2022
Accepted: Apr 11, 2023
Published online: Jun 20, 2023
Published in print: Oct 1, 2023
Discussion open until: Nov 20, 2023

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Ph.D. Candidate, College of Civil and Transportation Engineering, Shenzhen Univ., Shenzhen 518060, China. ORCID: https://orcid.org/0000-0003-0061-3774. Email: [email protected]
Yingwu Zhou [email protected]
Professor, Key Laboratory of Coastal Urban Resilient Infrastructures (MOE), Shenzhen Univ., Shenzhen 518060, China. Email: [email protected]
Assistant Professor, Key Laboratory of Coastal Urban Resilient Infrastructures (MOE), Shenzhen Univ., Shenzhen 518060, China (corresponding author). ORCID: https://orcid.org/0000-0001-8303-6460. Email: [email protected]

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