CFD Based Performance Prediction Model
for Paddle Wheel Aerator
Priyambodo Nur Ardi Nugroho
1a
, Muhammad Anis Mustaghfirin
1b
,
Dwi Sasmita Aji Pambudi
1c
, Eky Novianarenti
1d
, Dyah Arum Wulandari
2e
and Shuichi Torii
3f
1
Shipbuilding Engineering Department, Politeknik Perkapalan Negeri Surabaya, Indonesia
2
Department of Mechanical Engineering, Universitas Negeri Jakarta, Indonesia
3
Department of Advanced Mechanical System Engineering, Kumamoto University, Japan
dyaharum@unj.ac.id, torii@mech.kumamoto-u.ac.jp
Keywords: Paddlewheel Aerator, Performance Prediction Model, Computational Fluid Dynamics (CFD), Water Quality,
Aeration Process.
Abstract: The intensive aquaculture industry is mainly affected by the ability to maintain water quality, and low
dissolved oxygen could be improved through the aeration process. The paddlewheel aerator is one of the
supporting devices required for the intensive aquaculture pond system. The paddlewheel aerator still has a
low aeration performance, resulting in higher operational costs. This paper presents an analytical model to
predict the optimal performance of a paddle wheel aerator. The model considers the most influential factors
affecting the performance of the paddlewheel aerator. Then, Computational Fluid Dynamics (CFD) is
employed to simulate and validate the developed analytical model. The simulation results demonstrate that
the model is accurate enough to estimate the paddlewheel aerator's optimal operational condition.
1 INTRODUCTION
Aquaculture has become an important global source
of food and commercial products. According to a
technical report by Gillet (2008) for the Food and
Agriculture Organization of the United Nations, the
annual worldwide production of shrimp, both farmed
and caught, is approximately 6 million tonnes, with
more than 40% coming from farming. Aquaculture is
generally divided into marine and inland categories.
Unlike marine aquaculture, which takes place in finite
spaces surrounded by an open environment such as a
river or sea, inland aquaculture occurs in isolated
coastal vessels or ponds with little connection to the
external environment. In these isolated spaces,
biological conditions can deviate from the natural
environment, leading to technical problems such as
a
https://orcid.org/0000-0001-7111-5866
b
https://orcid.org/0000-0002-9669-1015
c
https://orcid.org/0000-0002-4869-4326
d
https://orcid.org/0009-0002-7869-1692
e
https://orcid.org/0000-0001-5803-0227
f
https://orcid.org/0000-0001-9327-741X
low dissolved oxygen (DO) levels in the water, which
can pose a challenge for aquatic organisms in shrimp
culture (Itano, 2018).
Aeration is the mechanism by which a certain
amount of oxygen is added to the water to provide
sufficient oxygen. Aeration is achieved by increasing
the contact of water and air using an aerator. One type
of aerator widely used in pond culture is the paddle
wheel aerator (Laksitanonta, 2003). The paddlewheel
aerator is the most suitable due to its aeration
mechanism and the sizeable drive power (Romaire,
2007). Several parameters affect the aeration rate,
including water and air surface contact, differential
oxygen concentration, membrane surface coefficient,
and turbulence (Boyd, 1988). A single paddle wheel
aerator's performance in shrimp ponds has been
examined (Ong, 2005). On the other hand, a
comprehensive review of the state-of-the-art
Nugroho, P., Mustaghfirin, M., Pambudi, D., Novianarenti, E., Wulandari, D. and Torii, S.
CFD Based Performance Prediction Model for Paddle Wheel Aerator.
DOI: 10.5220/0012114600003680
In Proceedings of the 4th International Conference on Advanced Engineering and Technology (ICATECH 2023), pages 103-106
ISBN: 978-989-758-663-7; ISSN: 2975-948X
Copyright
c
2023 by SCITEPRESS – Science and Technology Publications, Lda. Under CC license (CC BY-NC-ND 4.0)
103
paddlewheel aerators in aquaculture is also available
(Saucedo-Teran, 2019).
Some researchers have examined the aeration
efficiency of a single paddle wheel aerator in
aquaculture (Duan, 2015). The paddle wheel's shape,
size, and speed can impact aeration efficiency
(Moulick, 2002). Low aeration efficiency can result
in the need for higher drive horsepower due to higher
drag, which can lead to increased operating costs,
including electricity and fuel consumption. Various
models of paddle wheel aerators are available in the
market, with Taiwan-designed aerators being widely
used due to their affordability and lightweight design,
as depicted in Figure 1 (Wyban, 1989). However,
their efficiency is relatively low, with the paddle
wheel aerator having a Standard Aeration Efficiency
(SAE) value of 1.063 kg O
2
kW h
-1
, which is lower
than other designs (Peterson, 2002).
Previous research has used computational fluid
dynamics (CFD) modelling to examine the
performance of paddle wheel aerators in aquaculture,
providing insights into the aerator's flow pattern and
oxygen transfer efficiency (Akintoye, 2018). Other
studies have also employed CFD simulations to
analyze the flow pattern of a paddle wheel aerator
tank (Kiatkittipong, 2007) and to investigate flow and
mixing patterns in an aerated paddlewheel tank
(Prasertsri, 2009). The current study aimed to predict
the optimal performance of a paddle wheel aerator
based on numerical analysis of the current model
design, serving as a baseline for future improvement.
Figure 1: Paddle Wheel Aerator based on Taiwan design.
2 MATERIALS AND METHODS
A hydrodynamic model was performed using the
continuity and momentum equations for Newtonian
incompressible fluids to represent the flow structure
through a paddlewheel aerator. This study refers to
previous studies about the hydrodynamic
characteristics of a paddle wheel aerator using CFD
simulation (Yu, 2021). Recently, a numerical study
based on CFD simulation to investigate the
hydrodynamic characteristics of the impeller of a
paddle wheel aerator have been conducted (Miao,
2018). Reynolds terms were resolved to fluctuate
time-averaged values and averaged in the
longitudinal direction to yield the depth-integrated
three-dimensional Reynolds equation (Schlichting,
1979). The paddlewheel aerator's thrust effects are
considered a mass force to produce the acceleration
and are included in the Reynolds equation (Peterson,
2002). The governing equations can be deduced in the
x, y, and z directions to give the following equations
(Chen, 1994).
𝜕𝜂
𝜕𝑡
+
𝜕𝐻𝑈
𝜕𝑥
+
𝜕𝐻𝑉
𝜕𝑦
+
𝜕𝐻𝑊
𝜕𝑧
=0
(1)


+


+


+


=𝐻𝐹

𝑔𝐻



+𝜀
̅
𝐻

+

+

(2)


+


+


+


=𝐻𝐹

𝑔𝐻



+𝜀
̅
𝐻

+

+

(3)


+


+


+


=𝐻𝐹

𝑔𝐻



+𝜀
̅
𝐻

+

+

(4)
Where η is water surface elevation; t is time; x,
y, and z are Cartesian coordinates; U, V, and W are
depth-averaged velocity components in the x-, y-, and
z- directions; and H is total depth. The paddlewheel
aerator pushes the water mass forward, creating
horizontal circulation. On the other hand, it splashes
water particles vertically. Figure 2 shows the
operation of the paddlewheel aerator in a fish pond.
Water particles are projected and dispersed in an area
of constant height and width at the front of the
impeller. The blades of the paddlewheel aerator have
some holes in the body to improve reaeration.
However, the swept mass of the blades may not be
equal to the mass pushed forward by the paddlewheel
aerator, resulting in a mass imbalance. To correct this,
a simple mass correction factor can be used.
ICATECH 2023 - International Conference on Advanced Engineering and Technology
104
Figure 2. Pushing and splashing of water particles by
paddlewheel operating in the pond.
Figure 3 shows the computational domain after
running approximately 10,000 iterations. This study
aimed to create a relationship between laboratory data
and a computational fluid dynamics model. The
Ansys Fluent software was used to perform a series
of simulation experiments on the developed model.
The Reynolds-averaged Navier-Stokes equations
were applied to the stable, incompressible, three-
dimensional flow of the pond. The transport
equations of the Standard k ε turbulence model were
utilized to calculate the turbulence kinetic energy k
and its dissipation rate ε.
Figure 3. Computational Domain.
3 RESULTS AND DISCUSSION
Figure 4 provides a visualization of the velocity
vector changes in the computational domain,
observed from the x-y side view. The highest
recorded velocity vector was found to be 5 m/s, while
the average velocity, based on the velocity volume
represented in Figure 5, was approximately 2 m/s.
The results were confirmed through experimental
analysis. It is important to note that various factors,
such as wind, pond shape, floor topography, turbulent
diffusivity, and paddlewheel aerator arrangement,
influence the pond's flow characteristics.
Figure 4: Velocity Vector.
A physical experimental analysis is necessary to
separate the individual effects of wind, pond shape,
floor topography, turbulent diffusivity, and the
arrangement of paddlewheel aerators on the flow
characteristics in the pond. However, controlling and
quantifying all these effects simultaneously is not
easy. Therefore, laboratory experiments using
proportional models are needed to control the
parameters and obtain data for analysis. It is
suggested that further research should be conducted
to verify the model prediction and clarify the flow
characteristics of paddle wheel aerators using fluid
dynamics experiments in a controlled laboratory, as
previously recommended (Kang, 2004).
Figure 5: Velocity Volume.
4 CONCLUSIONS
In conclusion, optimizing various factors affecting
aeration can lead to improved efficiency, ultimately
reducing operating costs and improving overall
aquaculture productivity. Computational fluid
dynamics models have proven to be useful tools in
CFD Based Performance Prediction Model for Paddle Wheel Aerator
105
predicting the performance of paddle wheel aerators
and can aid in the development of more efficient
designs. However, laboratory experiments using
proportional models are still necessary to fully
understand the flow characteristics and optimize the
design of paddle wheel aerators. Future research
should focus on combining both computational and
experimental approaches to improve the
understanding and optimization of aeration in
aquaculture.
ACKNOWLEDGEMENTS
This research was supported by the Ministry of
Research, Technology and Higher Education
Indonesia and The Indonesia Endowment Funds for
Education (LPDP) through an applied scientific
research funding program. Such funding is crucial in
advancing research and promoting innovation, and it
is a positive step toward promoting sustainable
aquaculture practices. The results of this study can
provide valuable insights into the aquaculture
industry, which can help them optimize their
production processes and increase their productivity
while minimizing their environmental impact.
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