Ari Hamdani

Dr. Ari Hamdani

Japan Atomic Energy Agency
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Research Focus & Metrics

Academic Career Length

13Years (2014-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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24 December 2018 in Applied Sciences
Verified
Journal Article
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WWWongsakorn Wongsaroj
Wongsakorn Wongsaroj
Ari HamdaniAri Hamdani
Ari Hamdani
NTNatee Thong-un
Natee Thong-un
HTHideharu Takahashi
Hideharu Takahashi
HKHiroshige Kikura
Hiroshige Kikura
This study introduces a measurement technique for simultaneous phase-separated velocity in two-phase bubbly flow. The non-invasive technique, based on an Ultrasonic Velocity Profiler (UVP), is used in order to obtain an instantaneous, separate velocity profile for both liquid and bubble. The aim of this paper is to measure each phase velocity at the same time and position it using only a single resonant frequency. To achieve this aim, extended signal processing of the Short-Time Fourier Transform (STFT) is proposed, combining with amplitude classification to analyze Doppler signal influenced from the bubbly flow. The use of developed algorithms allows the instantaneous separation of liquid and bubble velocity profiles. In this work, the developed technique is used to measure the velocity profile of bubbly flow in the vertical pipe, demonstrating the classification of liquid and bubble velocity. To confirm the accuracy of each velocity profile phase, the Particle Image Velocimetry (PIV) method is used for comparison. The results clarify that the proposed method is in good agreement with the PIV measurement. Finally, the effect of void fraction against velocity measurement of both phases was demonstrated.

1 February 2022 in Annals of Nuclear Energy
Verified
Journal Article
Open access
SASatoshi Abe
Satoshi Abe
Ari HamdaniAri Hamdani
Ari Hamdani
MIMasahiro Ishigaki
Masahiro Ishigaki
YSYasuteru Sibamoto
Yasuteru Sibamoto

2 October 2022 in Progress in Nuclear Energy
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Journal Article
Open access
Ari HamdaniAri Hamdani
Ari Hamdani
SASatoshi Abe
Satoshi Abe
MIMasahiro Ishigaki
Masahiro Ishigaki
YSYasuteru Sibamoto
Yasuteru Sibamoto
TYTaisuke Yonomoto
Taisuke Yonomoto

22 September 2016 in Journal of Mechanical Science and Technology
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Journal Article
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Ari HamdaniAri Hamdani
Ari Hamdani
TITomonori Ihara
Tomonori Ihara
NTNobuyoshi Tsuzuki
Nobuyoshi Tsuzuki
HKHiroshige Kikura
Hiroshige Kikura

1 November 2017 in Theoretical and Applied Mechanics Letters
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Journal Article
Open access
MBMunkhbat Batsaikhan
Munkhbat Batsaikhan
Ari HamdaniAri Hamdani
Ari Hamdani
HKHiroshige Kikura
Hiroshige Kikura

15 July 2020 in Energies
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Ari HamdaniAri Hamdani
Ari Hamdani
SASatoshi Abe
Satoshi Abe
MIMasashiro Ishigaki
Masashiro Ishigaki
YSYasuteru Sibamoto
Yasuteru Sibamoto
TYTaisuke YONOMOTO
Taisuke YONOMOTO
In the case of a severe accident, natural convection plays an important role in the atmosphere mixing of nuclear reactor containments. In this case, the natural convection might not in the steady-state condition. Hence, instead of steady-state simulation, the transient simulation should be performed to understand natural convection in the accident scenario within a nuclear reactor containment. The present study, therefore, was aimed at the transient 3-D numerical simulations of natural convection of air around a cylindrical containment with unsteady thermal boundary conditions (BCs) at the vessel wall. For this purpose, the experiment series was done in the CIGMA facility at Japan Atomic Energy Agency (JAEA). The upper vessel or both the upper vessel and the middle jacket was cooled by subcooled water, while the lower vessel was thermally insulated. A 3-D model was simulated with OpenFOAM®, applying the unsteady Reynolds-averaged Navier–Stokes equations (URANS) model. Different turbulence models were studied, such as the standard k-ε, standard k-ω, k-ω shear stress transport (SST), and low-Reynolds-k-ε Launder–Sharma. The results of the four turbulence models were compared versus the results of experimental data. The k-ω SST showed a better prediction compared to other turbulence models. Additionally, the accuracy of the predicted temperature and pressure were improved when the heat conduction on the internal structure, i.e., flat bar, was considered in the simulation. Otherwise, the predictions on both temperature and pressure were underestimated compared with the experimental results. Hence, the conjugate heat transfer in the internal structure inside the containment vessel must be modeled accurately.