Abstract

Chilled gas pipelines generally traverse a long distance through various soils and may operate for decades with varying temperatures of gas, surrounding soil, and ground surface. The present study investigates the effects of key factors on frost heave using two-dimensional finite-element modeling of the coupled thermomechanical process by implementing the Konrad–Morgenstern segregation potential model. A simplified approach is proposed to estimate the thaw-back effects on long-term frost heave. The seasonal variation of ground surface temperature significantly affects the heave, especially for pipelines at shallow burial depths and for long-term heaving. An increase in cohesion of the frozen soil and a reduction in the initial ground temperature reduce the heave. Modeling of frozen fringe and stress effects on segregation potential are discussed. Subzero gas temperature has a smaller effect on heave for lower initial ground temperatures; however, it significantly affects long-term heave for higher ground temperatures.

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Acknowledgments

The work presented in this paper has been supported by InnovateNL, formerly the Research Development Corporation, Newfoundland and Labrador, through the ArcticTECH program, Equinor Research Chair, and the Natural Sciences and Engineering Research Council of Canada.

Notation

The following symbols are used in this paper:
a
soil constant;
Ca
apparent volumetric heat capacity of soil;
c
cohesion of unfrozen soil;
cf
cohesion of frozen soil;
ci
specific heat of ice;
cs
specific heat of soil particle;
cw
specific heat of water;
D
pipe diameter;
E
Young’s modulus of unfrozen soil;
Ef
Young’s modulus of frozen soil;
gradT
temperature gradient;
gradTff
temperature gradient in frozen fringe;
H
burial depth;
h
frost heave;
k
constant for thawing with temperature increase;
L
latent heat of water;
n
porosity;
P
percentage of total water content that remains unfrozen well below 0°C;
Pe
stress parameter for segregation potential;
p
effective mean stress;
Q
factor controls unfrozen water content with temperature;
q
heat flux;
qx, qy
heat flux in x- and y-directions;
R
parameter related to P;
r
radial distance from the current pipe center;
r0
radial distance from the initial pipe center;
SP0
segregation potential at zero applied pressure;
T
temperature;
Tf
in situ freezing temperature;
Tg
initial ground temperature;
Tp
pipe temperature;
Ts
ground surface temperature;
Tsf
segregation freezing temperature;
Tsm
mean annual ground surface temperature;
Tsv
seasonal ground surface temperature;
T50
temperature at the highest rate of thawing;
t
time;
tff
thickness of frozen fringe;
vm
migrated water influx;
Wu
fraction of total water that remains unfrozen;
wu
unfrozen water content basis of the dry mass of soil;
w0
soil water content basis of the dry mass of soil before freezing;
x, x0
horizontal distance measured from pipe center;
Y0
depth of frost front from initial pipe invert position;
y
vertical distance measured from current pipe center;
y0
vertical distance measured from initial pipe center;
α
rate of increase of cohesion of frozen soil with ice content;
β
angle from the y-axis to a point with respect to the current pipe center;
β0
angle from the y-axis to a point with respect to the initial pipe center;
φ
direction of heat flux with respect to the y-axis;
λe
equivalent thermal conductivity of soil;
λi
thermal conductivity of ice;
λs
thermal conductivity of soil particle;
λw
thermal conductivity of water;
θi
volumetric fraction of ice;
θis
volumetric fraction of segregate ice;
θis_max
maximum volumetric fraction of segregate ice lens prior to start of thawing;
θs
volumetric fraction of soil particle;
θw
volumetric fraction of unfrozen water;
ρd
dry density of soil;
ρi
density of ice;
ρs
density of soil particle;
ρw
density of water;
σn
effective normal stress;
σov
effective overburden pressure;
ν
Poisson’s ratio of unfrozen soil;
νf
Poisson’s ratio of frozen soil;
ϕ
angle of internal friction of unfrozen soil;
ϕf
angle of internal friction of frozen soil;
ψ
dilation angle of unfrozen soil; and
ψf
dilation angle of frozen soil.

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Go to Journal of Cold Regions Engineering
Journal of Cold Regions Engineering
Volume 36Issue 4December 2022

History

Received: Mar 11, 2021
Accepted: Jun 17, 2022
Published online: Aug 25, 2022
Published in print: Dec 1, 2022
Discussion open until: Jan 25, 2023

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Rajith Dayarathne [email protected]
Intermeadiate Geotechnical Engineer, C-CORE, Captain Robert A Bartlett Building, Morrissey Rd., St. John’s, NL, Canada A1B 3X5. Email: [email protected]
Professor, Faculty of Engineering and Applied Science, Dept. of Civil Engineering, Memorial Univ. of Newfoundland, St. John’s, NL, Canada A1B 3X5 (corresponding author). ORCID: https://orcid.org/0000-0001-9392-1498. Email: [email protected]
Principal Consultant, C-CORE, Captain Robert A Bartlett Building, Morrissey Rd., St. John’s, NL, Canada A1B 3X5. ORCID: https://orcid.org/0000-0002-5668-3475. Email: [email protected]
Dilan Robert [email protected]
Senior Lecturer, School of Engineering, RMIT Univ., GPO Box 2476, Melbourne, VIC 3001, Australia. Email: [email protected]

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  • Two-dimensional finite element modeling of long-term frost heave beneath chilled gas pipelines, Cold Regions Science and Technology, 10.1016/j.coldregions.2023.103781, 208, (103781), (2023).

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