Computational Fluid Dynamics Analysis of 3D Wind Flow around
Rhizophora Mangrove Tree and Drag Force Acting on the Wall of the
Tree
SINI RAHUMAN1, MOHAMED ISMAIL2, SHYLA MANAVALAN VARGHESE3, BINSON V. A.4
1Faculty of Foundation (Mathematics),
Bahrain Polytechnic,
Isa Town,
KINGDOM OF BAHRAIN
2Department of Mathematics,
Sathyabama Institute of Science and Technology,
Chennai,
INDIA
3Department of Developmental Mathematics,
Houston Community College,
Houston, Texas,
USA
4Department of Electronics Engineering,
Saintgits College of Engineering,
INDIA
Abstract: - Many natural disasters, such as cyclones, typhoons, mudslides, and tsunamis, are currently plaguing
the world. These tragedies, which have destroyed the coastal settlements, claim a great number of lives each
year. The characteristics and structure of the Mangrove tree have the significant impact on protecting the coast
from heavy wind, floods, mudslides, and other kinds of natural disasters. This research work investigates how
Mangroves can protect the area near the coast from a fluid dynamics point of view. Complex real world
problems require intelligent systems that combine knowledge and techniques. Hence Computational Fluid
Dynamics (CFD) technique namely the finite volume method is employed as a tool in this study. In this
research, a model Rhizophora Mangrove tree from Pichavaram Mangrove forest, Tamilnadu, India is generated
using Ansys Workbench design modeler. A computational domain is created around this tree to reduce the
boundary effect. Grid-independent research was carried out using various mesh sizes to determine the best grid
resolution for the analysis. An unstructured triangular mesh was generated for the simulation. The focus of this
study is to determine the 3D flow around the tree in order to determine the wind velocity, as well as the
coefficient of drag and drag force on the wall tree. This research helps to give a clear understanding of wind
flow around the 3D Rhizophora Mangrove tree. The velocity profile, pressure distribution, drag force, and drag
coefficient around the tree are captured, analysed, and presented in detail. The results show that the Rhizophora
mangrove trees can significantly reduce the flow velocity of the wind and will be able to safeguard the coast
and communities nearby from natural disasters.
Key-Words: - Rhizophora, wind velocity, steady flow, unsteady flow, coefficient of drag force, computational
fluid dynamics.
Received: January 17, 2023. Revised: November 22, 2023. Accepted: December 19, 2023. Published: December 31, 2023.
1 Introduction
Natural disasters are a huge danger to human beings
all around the earth every year. To defend the
coastline from tsunamis, storms, floods, tornadoes,
and hurricanes, coastal erosion is a serious
challenge. A mangrove is a shrub or tree that lives
in salty or brackish water along the coast. They
shield the surrounding areas from tsunamis and poor
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weather. Planting mangroves near the coast is one of
the most effective ways to defend the coast, as
mangroves can break up fluid movement. In 2004,
the Indian Ocean Tsunami caused damage to a
number of Asian and African countries. Many
villages located behind the forest were sheltered by
the mangrove forest during the Tsunami, according
to studies, [1].
Various numerical and analytical research, [2],
[3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13],
[14], [15], [16], [17], [18] have been undertaken to
examine and discover the importance of mangrove
forests. To examine wave attenuation over a finite-
area vegetated region, researchers, [19], established
a computer model based on small-amplitude
periodic waves traveling through a lattice-like
structure of vertical cylinders. Researchers
developed a refraction-diffraction wave model, [20],
for analyzing wave propagation along a moderate
slope zone on the shore in the presence of stiff
vegetation. A 3-D numerical technique was used to
explore the interaction of tsunami waves with
mangrove ecosystems, [21]. In a recent work [22],
numerical analysis was utilized to investigate
periodic long-wave run-ups on sloping beaches with
stiff vegetation. Another study [23], used a 2-D
Numerical Wave Tank based on a porous body
model to show energy dissipation after contact with
a tsunami. The results reveal that when plant height,
density and width increase, the coefficient of
transmission decreases but the reflection coefficient
remains constant.
Another study [24], revealed that in regions with
extensive mangrove trees, waves traveling through
the roots generate jets, which like to move around
and cause turbulence. According to the study,
friction between the mangrove forest and the waves
slows the velocity of the waves, as contrasted to
friction at the bottom. The wave height and drop in
water velocity differ depending on the type of
mangrove species, [25]. Some researchers, [26],
used a computer simulation to explore the features
of roots and their involvement in reducing the
velocity of water flow around Avicennia marina and
Rhizophora apiculate.
In [27], a three-dimensional numerical technique
based on IHFOAM was used to explore the
interaction of tsunami waves with mangrove forests.
Research carried out using green infrastructure and
coastal ecosystems offers a natural approach method
to overcome natural disasters, [28]. Another study
was conducted and included a detailed explanation
regarding the supplementary proof of the storm
protection ecosystem services offered by mangroves
in the area. This serves as an additional justification
for investing in mangrove ecosystems to enhance
resilience against coastal disasters such as storms,
[29]
The velocity of waves was reduced as the
breadth and density of the forest grew, according to
data acquired from Avicennia's numerical
simulation with the TUNA-RP model, [30].
According to a numerical simulation study, [31], on
energy dissipation within the mangrove forest, the
mean wave velocity decreased considerably for
every 20 m cross-section of the mangrove forest.
The flow's vertical and horizontal amplitude
velocities were both reduced by around 60% of their
original velocity, [32].
According to a CFD study, [3], mangrove roots
have an important role in lowering wave velocity
and protecting the coast. CFD has also been used to
study the vortex activity related to gravitational
water vortex power plants, [33].CFD investigation
of water flow patterns around the rhizophora tree
was conducted in [5] and it was revealed that the
fluid velocity was lowered by more than 70%.The
behavior and efficacy of stilt roots (prop roots) of
Rhizophora Mangroves in lowering the flow of the
velocity of the wind during severe tropical storms,
intense tropical cyclones, and extremely intense
tropical cyclones were analyzed in [34].
The goal of this study is to identify the 3D wind
flow around the Rhizophora mangrove tree using a
computational approach to analyze and discover the
efficiency of mangroves in reducing flow velocity.
To develop shoreline protection systems and
promote the planting of mangrove trees around the
coast to safeguard villages near the coast, it is
critical to strengthen and expand research in wave
velocity propagation across Mangrove forests in
actual weather scenarios.
2 Methodology
2.1 Study Approach
Pichavaram Mangrove Forest stands as India's
renowned and the world's second-largest mangrove
expanse. The M.S. Swaminathan Research
Foundation (MSSRF) in Chennai has meticulously
gathered data on the Rhizophora Mangrove tree
indigenous to Pichavaram. This valuable dataset
serves as the foundation for creating a
computational model of the Rhizophora Mangrove
tree. Such modeling aids in a deeper understanding
of the tree's ecological dynamics, supporting
conservation initiatives and promoting sustainable
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management practices in the Pichavaram Mangrove
forest.
This study (CFD) starts with the development of
a computational model of the Rhizophora mangrove
tree, which is visualized in Figure 1. Ansys
Workbench design modeler 18.1 is used for this
process in general. The mesh is generated around
this geometry and applied to the boundary
condition. Fine mesh is generated near and around
the roots as visualized in Figure 2. Iso surface
created at y=0.25m, z=0.25m, y=0.75m &z=0.75m,
which are shown in Figure 3 and Figure 4. The
problem is solved using Ansys fluent CFD software.
The CFD, k- epsilon turbulence model is used to
simulate the incompressible steady and unsteady
wind flow around the Rhizophora mangrove tree.
The following two cases are analyzed in this
study and this problem is solved using the finite
volume method.
Case 1: Steady incompressible turbulent flow with
velocity 50m/s
Case2: Unsteady incompressible turbulent flow with
velocity 50m/s
Fig. 1: Geometry created in Ansys workbench 18.1
Fig. 2: Mesh created in Ansys design modeler
Fig. 3: Iso surface created at Y=0.25m & Z=0.25m
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Fig. 4: Iso surface created at Y=0.75m & Z=0.75m
2.2 Governing Differential Equation
1)Navier-Stokes system of equations for a three-
dimensional, incompressible flow,
Continuity Equation: 
󰇛󰇜 (1)
x-momentum equation:
󰇛󰇜
 󰇛󰇜
󰇛󰇜 (2)
y-momentum equation:
󰇛󰇜
 󰇛󰇜
󰇛󰇜 (3)
z-momentum
󰇛󰇜
 󰇛󰇜
󰇛󰇜 (4)
Were the velocity vector ,
󰇍
󰇍
󰇍
with u,
v, and w representing the velocity components in the
x, y, and z directions. is coefficient of viscosity, ρ
is density, p is pressure and t is time. For steady
state conditions, the rate of change term, which is
the first term on the left hand side in the equations,
equals zero.
2) Drag Force
F = ½ ρ V2A CD (5)
F is drag force (kN);V is velocity (m/s);CD is Drag
Coefficient and A is Frontal Area(m2) andρ is air
density (Kg/m3).
2.3 Boundary Condition
This study is conducted by Computational fluid
dynamics using ansys software and the boundary
conditions were implemented on the mesh model.
The steady and unsteady three-dimensional airflow
simulation was driven by the inlet velocity of
50m/s.At the outlet, zero-gauge pressure was
applied. In this study, the Reynolds number is more
than 500000, and the k-epsilon turbulence model is
applied to simulate the flow. All body forces are
ignored and the walls are stationary (no slip
boundary condition). No slip boundary condition is
applied to the wall and all body forces are neglected.
This flow has a mach number of less than 0.3,
indicating that it is an incompressible viscous flow.
The density of air is 1.225 kg/m3 in this research,
and the coefficient of viscosity of the air is 1.7894e-
05 kg/m-s in Cases 1 and 2.
2.4 Grid Independent Study
Ansys workbench design Modeler is used to create a
3D model of the Rhizophora Mangrove tree, and
Ansys fluent is used to simulate steady and unsteady
velocity and also identify the coefficient of drag and
drag force on the wall tree. Tetrahedral grids are
used for meshing the surface of the mangrove tree
model in this work after comprehensive verification.
Finer grids were chosen along the wall to capture
the wall effect while also saving computing time. A
far field with an open boundary of 5000cm by
2400cm was developed around the mangrove tree to
produce a computational model of the geometry and
to minimize the boundary effect on the airflow.
Grid-independent research was carried out using
various mesh sizes to determine the best grid
resolution for the analysis, which is shown in Figure
5.
The simulation of this study is performed using a
mesh of 64,906,691 cells based on the Grid
convergence study. Mesh of high quality was
created with skewness less than 0.9 and the mesh is
imported to Ansys fluent for CFD study.
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Fig. 5: Grid Independent study
2.5 Finite Volume Method
In this study, the Finite Volume Method is used.
The first and foremost step in the finite volume
method is to divide the entire domain under
consideration into discrete cells or control volumes.
Nodes are placed at the cell center and a grid is
generated. Integration of the non-linear governing
partial differential equation over each control
volume is the key process of the finite volume
method. This yields a system of discretized
equations at the nodal points. The system is then
solved to obtain the unknown values of velocity and
pressure at the nodal points followed by post-
processing of the results.
The integral forms of the non-linear partial
differential equations are discretized over each
control volume and transformed into an algebraic
system of equations using the upwind difference
scheme in the following manner.
Continuity equation:
(ρuA)I,J (ρuA)I-1,J
Δx +
(ρvA)I,J (ρvA)I,J-1
Δy = 0 (6)
X-momentum:
󰇡ρuI,J
2A󰇢(ρuI-1,J
2A)
Δx +
󰇡ρui,j+1A󰇢vi,j+1 (ρui,JA) vi,j
Δy =
󰇡pI-1,J pI,J󰇢
Δx ΔU+
󰇡µ∂u
∂x󰇢i+1,J 󰇡µ∂u
∂x󰇢i,J
Δx +
󰇡µ∂u
∂y󰇢i,j+1 󰇡µ∂u
∂y󰇢i,J
Δy
ΔU (7)
󰇡ρuI,J
2A󰇢(ρuI-1,J
2A)
Δx +
󰇡ρui,j+1A󰇢vi,j+1 (ρui,JA) vi,j
Δy =
󰇡pI-1,J pI,J󰇢
Δx ΔU +
󰇯󰇡µui+1,J ui,J
ΔxPE 󰇢 󰇡µui,J ui-1,J
ΔxWP 󰇢
Δx 󰇰 +
µui,J+1 ui,J
ΔyNP i,J+1 µui,J ui,J-1
ΔyPS
Δy

ΔU (8)
ΔU is the u-control volume.
Δx is the width of the u-control volume.
Y-momentum:
 (ρvI-1,JA)-
Δx +
󰇡ρvi,j+1
A󰇢(ρvi,J
A)
Δy =󰇡pi,j pi,j+1󰇢
Δy ΔV+
󰇡
 󰇢󰇡-
 󰇢
Δx
µvi,J+1 vi,J
ΔyPW n 󰇡-
 󰇢
Δy

ΔV (9)
ΔV is the v-control volume.
Δy is the width of the v-control volume.
Similarly, Z - momentum equation also can be
calculated. The k model is used to represent the
impacts of turbulence in turbulent flow. In addition
to the equations of continuity and momentum, the k-
ε model provides two transport equations (10) to
(11) for turbulent kinetic energy k and turbulent
dissipation rate ε., are given by
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󰇛󰇜
󰇛󰇜
󰇡
󰇢

󰇜 (10)
󰇛󰇜
󰇛󰇜
󰇡
󰇢


󰇛󰇜
(11)
where ui is the x-direction velocity component, μ is
the viscosity, t is the turbulent viscosity, Mk is the
kinetic energy production due to shear stress, is
the kinetic energy generation due to buoyancy, and
Ym is the kinetic energy production due to
compressibility. The empirical constants are:
Cε1=1.44; Cε2=1.92; Cε3=1.0; σk=1, σε=1.3, and
Cμ=0.09 are empirical constants.
For three-dimensional flows, it is given by,

 
(12)

 
(13)


  (14)
The above equations (12) to (14) represent
discretized Navier Stokes Equations for steady state
flow where and  are the volume of u-
cell, v-cell and w-cell. For unsteady flow ap0 in (15)
is added to the central coefficients of the above
three equations.

󰇛󰇜
2.6 Error Analysis
There are two kinds of errors made by the computer
during each iteration. Which are the discretization
error (DE) and round off error(R)
De = A – S; R = N – S (16)
Where ‘A’ is the analytical solution of the partial
differential equation. ‘S’ is the exact solution of the
difference equation. ‘N’ is the Numerical solution
from a real computer with finite accuracy.
Discretization involves approximating continuous
mathematical models with discrete counterparts.
The error arises due to the finite representation of
continuous quantities in the discrete domain.
Round-off errors occur due to limitations in
computer precision. Computers represent numbers
with a finite number of digits, leading to small
errors in calculations, especially with repeated
operations.
The solution is unstable if the Ris grow bigger
during the progression of the solution from nth step
to (n+1)th step. The stable solution is obtained if

(17)
Stability is crucial for the reliability of numerical
solutions. If the Ri’s (round-off errors) grow larger
during iterations, it indicates instability in the
solution. The stability criterion (Equation 17)
ensures that the errors do not accumulate rapidly,
preventing numerical instability.
In summary, discretization errors result from the
process of approximating continuous problems with
discrete methods, while round-off errors stem from
the finite precision of computer arithmetic. Ensuring
stability through the defined criterion helps maintain
the reliability of numerical solutions in the iterative
process.
3 Results and Discussion
The velocity profile of both steady and unsteady air
flow is analyzed and interpreted the graph at
different positions y=0.25m, z=0.25m,
y=0.75m&z=0.75m are visualized in Figure 6,
Figure 7, Figure 8 and Figure 9 respectively. Both
steady and unsteady flow shows a similar pattern
and velocity contours, which are visualized in these
figures.
The maximum flow velocity is 86 m/s (red color
contour) and the minimum velocity is 0 m/s
(stagnation area) as shown in all these figures
(Figure 6, Figure 7, Figure 8 and Figure 9). The
individual roots are located in some position and jet
flow occurs around these roots, which causes the
flow velocity to increase in certain locations. The
velocity of the flow decreased to 0m/s when the
flow traveled around the Rhizophora Mangrove
roots and tree. The light blue color region is
represented by a velocity of 21.5 m/s, the dark green
colorcolor region is represented by a velocity of
43.0 m/s, the light green color region represented by
51.3 m/s, and some places in the main trunk
represented by 77.4 m/s.
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Fig. 6: Velocity at y=0.25m
Fig. 7: Velocity at z=0.25m
Fig. 8: Velocity at y=0.75
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Fig. 9: Velocity at z=0.75m
The pressure distribution of both steady and
unsteady wind flow is also analyzed and interpreted
in the graph at different positions y=0.25m,
z=0.25m, y=0.75m&z=0.75m are shown in Figure
10, Figure 11, Figure 12 and Figure 13 respectively.
The highest pressure observed as 1679 Pa (red color
contour).
The pressure decreased to -116 Pa (light
blue color contour) after the flow passed through the
mangroves. The green color contour is represented
by the pressure of 140Pa and the yellow color
contour indicates the pressure is 815 Pa.
Fig. 10: Pressure at y=0.25m
Fig. 11: Pressure at z=0.25m
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Fig. 12: Pressure at y=0.75m
Fig. 13: Pressure at z=0.75m
Figure 14, demonstrates the drag coefficients
and drag force on the model's wall tree. For air
velocity of 50 m/s, the highest coefficient of drag is
20687.047 and the drag force is 12670.816. Figure
15, illustrates how the solution converges onto three
decimal places when the fluid flow velocity is 50m/s
in both steady and unsteady models. The
convergence plot and a previous study from the
literature survey, [25], [26], [27], [28], [31], [32],
[34], are used to validate the outcome.
Fig. 14: Drag coefficient and drag force acting on wall tree
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Fig. 15: Convergence plot
4 Conclusion
The CFD simulations of the steady and unsteady
wind flow around a three dimensional Rhizophora
mangrove tree model (using the data from the
Pichavaram mangrove forest) with flow velocity of
50m/s were simulated and analyzed the velocity
profile, pressure distribution, drag coefficient, and
drag force. The ANSYS-18.1 Fluent with the k-
epsilon, steady, and unsteady turbulent models are
used for the simulations. This study reveals that the
Rhizophora mangroves can decrease the velocity of
the wind and be able to protect the coast. The
Rhizophora mangrove trees in the Pichavaram can
significantly reduce the flow velocity of the wind
and will be able to safeguard the coast and
communities nearby from natural disasters such as
cyclones, mudslides, and tsunamis. The future scope
of this research refers to the wave simulation around
multiple mangrove trees, multiphase flow, and
different arrangements of mangrove trees. This
study advises each human to plant new mangrove
trees and protect old ones because they are
extremely valuable.
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Contribution of Individual Authors to the
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The authors equally contributed to the present
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problem to the final findings and solution.
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Scientific Article or Scientific Article Itself
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Conflict of Interest
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WSEAS TRANSACTIONS on FLUID MECHANICS
DOI: 10.37394/232013.2023.18.27
Sini Rahuman, Mohamed Ismail,
Shyla Manavalan Varghese, Binson V. A.
E-ISSN: 2224-347X
294
Volume 18, 2023