Abstract

Geosynthetic-reinforced soil (GRS) retaining walls have been widely adopted in engineering practice based on the development of several design methods. However, the temperature effect, which was proved to be an important influencing factor of retaining wall performance, was not considered in the existing design methods. This study investigates the temperature distributions of a (GRS) wall subjected to freeze–thaw (FT) cycles using (1) a lab-scale physical model test within a custom-made temperature-controlled tank; and (2) a commercial finite-element computer program for conducting numerical modeling. The numerical model was first validated using the lab-scale model test data obtained in this study, and then a full-scale numerical model was created for achieving an in-depth understanding of the temperature distribution behaviors of a real GRS wall subjected to FT cycles. Both model test and numerical results demonstrate that (1) the periodic variation of the ambient temperature during the FT process induces a temperature fluctuation in a sinusoidal shape in the soil, and the temperature distributions of the soil are distinctly related to its location inside the GRS wall; (2) the soil temperature in zones with a distance of 2.0 m to the exposed boundaries (i.e., back of facing panels and road pavement) of the GRS wall is more sensitive to the variation of the ambient temperature. Also, the temperature amplitudes in these regions during each FT cycle are greater than those in the zones far away from the exposed boundaries of the GRS wall; and (3) the frost depth in the vertical direction or frost thickness in the horizontal direction increases constantly with a decrease of the ambient temperature lower than 0°C, and vice versa. The maximum frost depth or thickness behind the GRS wall is lagged to the lowest ambient temperature and decreases with the increase of the distance to the exposed boundaries. In addition, a mathematical model was proposed for predicting the soil temperature amplitudes at different locations inside the GRS wall.

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Acknowledgments

The work presented in this paper was supported by the National Natural Science Foundation of China (Grant Nos. 52078182 and 41877255) and the Tianjin Municipal Natural Science Foundation (Grant No. 20JCYBJC00630). This financial support is gratefully acknowledged.

Notation

The following symbols are used in this paper:
C
mass heat capacity;
Cf
C in a frozen area;
Cu
C in an unfrozen area;
c
cohesion;
DH
distance to the back of the facing blocks;
DV
distance to the bottom of a pavement;
E
elastic modulus;
Gs
specific gravity;
h
wall height;
hg
laying height of geogrids from the bottom;
hh
horizontal frost thickness;
hv
vertical frost depth;
Ip
plasticity index;
T
temperature;
Tair
air T;
Tair,m
air T in a temperature chamber;
TFT
T at an FT interface;
Tf
T in a frozen zone;
TR
ambient T of a GRS wall considering the solar radiation effect;
TR,amp
T amplitude of a GRS wall considering the solar radiation effect;
TR,ave
average T of a GRS wall considering the solar radiation effect;
Ts
soil T;
Ts,amp
Ts amplitude;
Ts,ave
average Ts;
Ts,max
maximum Ts;
Ts,min
minimum Ts;
TT
tensile strength of geogrids;
Tu
T in an unfrozen zone;
T0
initial T;
t
elapsed time;
v
Poisson’s ratio;
wi
ice content per unit volume;
wL
liquid limit;
wP
plastic limit;
wopt
optimum water content;
x
distance to the outside surface of facing blocks;
y
distance to the bottom of a GRS wall;
α
thermal expansion coefficient;
γdmax
maximum dry unit weight;
ΔTs
Ts fluctuation range;
T
average temperature gradient;
TH
horizontal average temperature gradient;
V
vertical average temperature gradient;
κ
coefficient of thermal diffusivity;
κf
κ in a frozen zone;
κu
κ in an unfrozen zone;
λ
thermal conductivity;
λf
λ in a frozen zone;
λu
λ in an unfrozen zone;
ρi
density of ice;
ϕR
annual ambient temperature phase shift of a GRS wall considering the solar radiation effect;
ϕs
soil temperature phase shift; and
φ
internal friction angle.

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Go to International Journal of Geomechanics
International Journal of Geomechanics
Volume 22Issue 12December 2022

History

Received: Feb 28, 2022
Accepted: Jun 30, 2022
Published online: Sep 28, 2022
Published in print: Dec 1, 2022
Discussion open until: Feb 28, 2023

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Professor, School of Civil and Transportation Engineering, Hebei Univ. of Technology, Tianjin 300401, China. ORCID: https://orcid.org/0000-0002-8754-9711. Email: [email protected]
Fei-long Cui [email protected]
Ph.D. Candidate, School of Civil and Transportation Engineering, Hebei Univ. of Technology, Tianjin 300401, China. Email: [email protected]
Lu-qiang Ding, Ph.D. [email protected]
Lecturer, School of Civil and Transportation Engineering, Hebei Univ. of Technology, Tianjin 300401, China (corresponding author). Email: [email protected]
Assistant Professor, Mayfield College of Engineering, Tarleton State Univ., Stephenville, TX 76402. ORCID: https://orcid.org/0000-0003-0238-7598. Email: [email protected]
Wen-Ling Tian, Ph.D. [email protected]
Professor, School of Civil and Transportation Engineering, Hebei Univ. of Technology, Tianjin 300401, China. Email: [email protected]

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  • Numerical simulation of the performance of GRS walls considering freeze-thaw cycles, Geosynthetics International, 10.1680/jgein.22.00368, (1-18), (2023).
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