Technical Papers
Sep 23, 2020

Wave–Structure Interactions of Flexible Bags with Elastic Tendons: Application to Wave Energy Conversion

Publication: Journal of Waterway, Port, Coastal, and Ocean Engineering
Volume 147, Issue 1

Abstract

A new type of wave energy device has recently been proposed with the key component being a flexible air-filled bag, which is constructed such that the fabric is encased by an array of tendons. The behavior of the bag in still water under hydrostatic loading and its dynamic response when subjected to hydrodynamic loading in waves were previously analyzed using a numerical model developed with the assumption of inextensible tendons. In the present work, the model is extended to include the effects of tendon elasticity. The behavior of the bag with tendons of various moduli of elasticity is then compared with that of the bag with inextensible tendons. It is found that adding elasticity to the tendons has a similar effect to that of increasing the air volume connected to the bag, that is, it increases the resonance period of the device. Consequently, a bag with elastic tendons can be made even smaller in size than a bag with inextensible tendons in order to match the same target resonance period.

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Acknowledgments

Dr. Thanh Toan Tran from the National Renewable Energy Laboratory (NREL) provided the hydrodynamic coefficients for the dynamic response calculations. A.K. is supported by the Wave Energy Research Centre, jointly funded by The University of Western Australia and the Western Australian Government, via the Department of Primary Industries and Regional Development (DPIRD). Part of this study was conducted while A.K. was with the Department of Civil Engineering, Aalborg University. S.B. and D.F would also like to acknowledge support from Wave Energy Scotland through the project “A feasibility study on Elastomeric-based WECs” (ELASTO).

Notation

The following symbols are used in this paper:
A
combined mean cross-sectional area of the tendons;
An, An+1
angles (measured in the vertical plane relative to horizontal) at the element endpoints (in the dynamic model, these angles are denoted as An−1, An);
an−1, an
angular displacements at the element endpoints (complex);
BPTO
power take-off damping;
C
power take-off coefficient;
CWR¯
mean capture width ratio for the wave climate;
E
modulus of elasticity of the tendon;
FBexc
vertical excitation force on the substructure (complex);
FB,kR
vertical wave radiation force on the substructure due to a unit normal displacement of node k (complex);
FB,3R
wave radiation force on the substructure due to a unit heave displacement of the mean geometry (complex);
fBh
vertical hydrodynamic force on the substructure (complex);
g
acceleration due to gravity;
Hn+0.5
unit step function;
Hs
significant wave height;
h
arc length of element, including static extension;
h0
original length of element before extension;
i
imaginary unit;
J¯
mean wave energy transport for the wave climate;
MB
mass of the substructure;
Ms
mean mass of air in secondary volume;
m
increase in air mass in the compressible volume (complex);
ms
increase in air mass in the secondary volume (complex);
N
number of discretized tendon elements;
N
N + 1;
nwl
index of the first node below the waterline;
P
mean internal bag pressure relative to atmospheric;
P
mean absorbed power;
P¯
mean absorbed power for the entire wave climate;
Patm
atmospheric pressure;
Prob(Hs, Tz)
long-term probability of occurrence of the sea state;
p
pressure increase in the bag (complex);
pnexc
wave excitation pressure on node n (complex);
pnh
hydrodynamic pressure on node n (complex);
pn,kR
wave radiation pressure on node n due to a unit outward normal displacement of node k (complex);
pn,3R
wave radiation pressure on node n due to a unit heave displacement of the mean geometry (complex);
ps
pressure increase in the secondary volume (complex);
R
radial coordinate;
Rwl
mean waterplane radius;
rn
radial displacement of node n (complex);
S(ω, Hs, Tz)
wave spectrum for the sea state;
T
sum of mean tension in all tendons;
Te
wave energy period;
Tp
spectral peak period;
Tz
mean wave period;
V
mean compressible air volume;
Vs
secondary air volume;
v
increase of bag volume (complex);
Z
vertical coordinate;
zn
vertical displacement of node n relative to ξ3 (complex);
γ
heat capacity ratio;
δAn
An+1An;
δRn
Rn+1Rn;
δZn
Zn+1Zn;
η
incident wave amplitude (complex);
θ
angular coordinate;
ξ3
vertical displacement of substructure (complex);
ρ
water density;
ρair
mass density of air in the system at the mean pressure P;
ρn
radius of curvature of element n;
τ
increase in total tendon tension (complex);
ϕn
half of the arc sector angle of element n; and
ω
wave angular frequency.

References

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Information & Authors

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Published In

Go to Journal of Waterway, Port, Coastal, and Ocean Engineering
Journal of Waterway, Port, Coastal, and Ocean Engineering
Volume 147Issue 1January 2021

History

Received: Feb 26, 2020
Accepted: Jun 15, 2020
Published online: Sep 23, 2020
Published in print: Jan 1, 2021
Discussion open until: Feb 23, 2021

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Authors

Affiliations

Wave Energy Research Centre, Univ. of Western Australia, 35 Stirling Terrace, Albany, WA 6330, Australia (corresponding author). ORCID: https://orcid.org/0000-0002-9176-3702. Email: [email protected]
School of Engineering, Computing and Mathematics, Univ. of Plymouth, Drake Circus, Plymouth, PL4 8AA, UK. ORCID: https://orcid.org/0000-0002-9176-3702.
David Forehand
School of Engineering, Univ. of Edinburgh, Edinburgh, EH9 3JL, UK.
Hugh Wolgamot
Oceans Graduate School, Univ. of Western Australia, 35 Stirling Highway, Perth, WA 6009, Australia.

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