We develop a new numerical model based on eigenfunction matching method and the method of images to investigate the influence of tank wall reflection on the hydrodynamic behaviors of a cylinder with moonpool, which is defined as an opening from the deck to the bottom of a floating structure or ship. The new numerical model is first validated by comparing its results to experimental data in the existing literature and WaveAnalysisMIT results and then is used to analyze the effects of different tank widths on the heave radiation and diffraction problems. When the tank is not too narrow, the results only show a significant difference from those in open water around the transverse sloshing frequencies of the tank, i.e., when the tank width is an integer times the wavelength. It is noticed that the reflection effects induce spikes of the amplitude of free-surface elevations at the center of the moonpool in the radiation problem but induce troughs in the diffraction problem. This is explained by estimating the phase of the waves in moonpool induced by the wall reflections. For the narrow tank that does not allow transverse sloshing in the given frequencies, the results deviate from those in open water in a width range of frequencies. The free-surface elevations outside the cylinder are also investigated.

1.
B.
Molin
, “
On the piston sloshing modes in moonpools
,”
J. Fluid Mech.
430
,
27
50
(
2001
).
2.
B.
Molin
,
X.
Zhang
,
H.
Huang
, and
F.
Remy
, “
On natural modes in moonpools and gaps in finite depth
,”
J. Fluid Mech.
840
,
530
554
(
2018
).
3.
X.
Zhang
,
H.
Huang
, and
X.
Song
, “
On natural frequencies and modal shapes in two-dimensional asymmetric and symmetric moonpools in finite water depth
,”
Appl. Ocean Res.
82
,
117
129
(
2019
).
4.
B.
Chu
and
X.
Zhang
, “
On the natural frequencies and modal shapes in two-dimensional moonpools with recesses in finite water depth
,”
Appl. Ocean Res.
115
,
102787
(
2021
).
5.
A.
Das
,
S.
De
, and
B.
Mandal
, “
Wave interaction with an elliptic disc submerged in a two-layer fluid
,”
Appl. Math. Modell.
117
,
786
801
(
2023
).
6.
S. A.
Mavrakos
, “
Wave loads on a stationary floating bottomless cylindrical body with finite wall thickness
,”
Appl. Ocean Res.
7
(
4
),
213
224
(
1985
).
7.
S. A.
Mavrakos
, “
Hydrodynamic coefficients for a thick-walled bottomless cylindrical body floating in water of finite depth
,”
Ocean Eng.
15
(
3
),
213
229
(
1988
).
8.
R. W.
Yeung
and
R. K. M.
Seah
, “
On Helmholtz and higher-order resonance of twin floating bodies
,”
J. Eng. Math.
58
,
251
265
(
2007
).
9.
X.
Feng
and
W.
Bai
, “
Wave resonances in a narrow gap between two barges using fully nonlinear numerical simulation
,”
Appl. Ocean Res.
50
,
119
129
(
2015
).
10.
J. K.
Heo
,
J. C.
Park
,
W. C.
Koo
, and
M. H.
Kim
, “
Influences of vorticity to vertical motion of two-dimensional moonpool under forced heave motion
,”
Math. Probl. Eng.
2014
,
424927
.
11.
S.-C.
Jiang
,
W.
Bai
, and
B.
Yan
, “
Higher-order harmonic induced wave resonance for two side-by-side boxes in close proximity
,”
Phys. Fluids
33
(
10
),
102113
(
2021
).
12.
A. G.
Fredriksen
,
T.
Kristiansen
, and
O. M.
Faltinsen
, “
Wave-induced response of a floating two-dimensional body with a moonpool
,”
Philos. Trans. R Soc., A
373
,
20140109
(
2015
).
13.
O. M.
Faltinsen
,
O. F.
Rognebakke
, and
A. N.
Timokha
, “
Two-dimensional resonant piston-like sloshing in a moonpool
,”
J. Fluid Mech.
575
,
359
397
(
2007
).
14.
X.
Guo
,
H.
Lu
,
J.
Yang
, and
T.
Peng
, “
Resonant water motions within a recessing type moonpool in a drilling vessel
,”
Ocean Eng.
129
,
228
239
(
2017
).
15.
L.
Tan
,
L.
Lu
,
G.-Q.
Tang
,
L.
Cheng
, and
X.-B.
Chen
, “
A viscous damping model for piston mode resonance
,”
J. Fluid Mech.
871
,
510
533
(
2019
).
16.
S.
Ravinthrakumar
,
T.
Kristiansen
,
B.
Molin
, and
B.
Ommani
, “
A two-dimensional numerical and experimental study of piston and sloshing resonance in moonpools with recess
,”
J. Fluid Mech.
877
,
142
166
(
2019
).
17.
J.
Han
,
X.
Zhang
, and
H.
Huang
, “
Experimental and numerical studies of piston-mode resonance in a three-dimensional circular moonpool
,”
Phys. Fluids
35
(
8
),
082106
(
2023
).
18.
L.
Tan
,
L.
Cheng
, and
T.
Ikoma
, “
Damping of piston mode resonance between two fixed boxes
,”
Phys. Fluids
33
(
6
),
062117
(
2021
).
19.
A.
Feng
,
A.
Magee
, and
W. G.
Price
, “
Experimental and numerical study for drillship moonpool gap resonances in stationary and transit conditions in wave flume
,”
J. Offshore Mech. Arct. Eng.
142
(
2
),
021205
(
2020
).
20.
C.
Zhang
and
D.
Ning
, “
Hydrodynamic study of a novel breakwater with parabolic openings for wave energy harvest
,”
Ocean Eng.
182
,
540
551
(
2019
).
21.
J.
Xu
,
D.
Ning
,
R.
Mayon
, and
M.
Zhao
, “
Hydrodynamic investigation of a parabolic breakwater for wave energy focusing
,”
Phys. Fluids
35
(
9
),
097145
(
2023
).
22.
Z. Y.
Tay
, “
Effect of resonance and wave reflection in semi-enclosed moonpool on performance enhancement of point absorber arrays
,”
Ocean Eng.
243
,
110182
(
2022
).
23.
R.
E. Taylor
and
S.
Hung
, “
Mean drift forces on an articulated column oscillating in a wave tank
,”
Appl. Ocean Res.
7
(
2
),
66
78
(
1985
).
24.
S.
Mavrakos
and
P.
Koumoutsakos
, “
Hydrodynamic interaction among vertical axisymmetric bodies resstrained in waves
,”
Appl. Ocean Res.
9
(
3
),
128
140
(
1987
).
25.
R. W.
Yeung
and
S. H.
Sphaier
, “
Wave-interference effects on a truncated cylinder in a channel
,”
J. Eng. Math.
23
,
95
117
(
1989
).
26.
G.
Thomas
, “
The diffraction of water waves by a circular cylinder in a channel
,”
Ocean Eng.
18
(
1
),
17
44
(
1991
).
27.
S.-c.
Jiang
,
W.
Bai
, and
G.
Tang
, “
Numerical investigation of piston-modal wave resonance in the narrow gap formed by a box in front of a wall
,”
Phys. Fluids
31
(
5
),
052105
(
2019
).
28.
L.
Lu
,
L.
Tan
,
Z.
Zhou
,
M.
Zhao
, and
T.
Ikoma
, “
Two-dimensional numerical study of gap resonance coupling with motions of floating body moored close to a bottom-mounted wall
,”
Phys. Fluids
32
(
9
),
092101
(
2020
).
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