Yongdong Cui

Yongdong Cui

orcid

Research Focus & Metrics

Academic Career Length

22Years (2005-Present)

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

Representative Publications

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1 November 2015 in Ocean Engineering
Verified
Journal Article
Closed access
ZWZhaoyu Wei
Zhaoyu Wei
Tze How NewTze How New
Tze How New
YCYongdong Cui
Yongdong Cui

1 April 2017 in Extreme Mechanics Letters
Verified
Journal Article
Open access
XYXiang Yu
Xiang Yu
Zhenbo LuZhenbo Lu
Zhenbo Lu
Fangsen CuiFangsen Cui
Fangsen Cui
LCLi Cheng
Li Cheng
YCYongdong Cui
Yongdong Cui
Acoustic metamaterial comprising an array of resonators being attached to the side wall of a rigid duct is investigated in this study. We propose a resonator design by employing a pre-stretched dielectric elastomer (DE) membrane to tune the acoustic property of each resonator. Both numerical and experimental techniques are developed to characterize the acoustic behavior of the proposed device in terms of transmission loss (TL). By connecting multiple resonators, we show that a broadband TL can be achieved which combines the multiple attenuation bands provided by each resonator unit. The resulted attenuation band can be tuned by varying the applied voltage to the DE membranes, showing promising potentials such as adaptive sound control devices for ventilation systems and other engineering applications

1 February 2022 in Aerospace Science and Technology
Verified
Journal Article
Closed access
Jichao LiJichao Li
Jichao Li
MZMengqi Zhang
Mengqi Zhang
CTChien Ming Jonathan Tay
Chien Ming Jonathan Tay
NLNingyu Liu
Ningyu Liu
YCYongdong Cui
Yongdong Cui
BKBoo Cheong Khoo
Boo Cheong Khoo

1 May 2015 in AIAA Journal
Verified
Journal Article
Closed access
ZZZijie Zhao
Zijie Zhao
JLJiun-Ming Li
Jiun-Ming Li
JZJianguo Zheng
Jianguo Zheng
YCYongdong Cui
Yongdong Cui
BKB. C. Khoo
B. C. Khoo
The shock wave behavior generated from a single shot of pulsed nanosecond dielectric-barrier-discharge plasma actuator with varying pulse voltages in quiescent air was studied by experiments and numerical simulations. The experiments included using the schlieren technique, a fast response pressure transducer, and a two-velocity-component particle image velocimetry system to measure the propagation of the shock wave, the shock overpressure, and the shock induced flow, respectively. For the numerical simulation, a simple “phenomenological approach” was employed by modeling the plasma region over the encapsulated electrode as a jump-heated and pressurized gas layer. The present investigation revealed that the behaviors of the shock wave generated by the nanosecond pulsed plasma were fundamentally a microblast wave, and their speed and strength were found to increase with higher input voltages. The blast wave occured about 1 to 3 μs after the discharge of the nanosecond pulse, which was dependent on the inpu...

1 March 2014 in Physics of Fluids
Verified
Journal Article
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PDF file
JZJ. G. Zheng
J. G. Zheng
ZZZ. J. Zhao
Z. J. Zhao
JLJ. Li
J. Li
YCYongdong Cui
Yongdong Cui
BKBoo Cheong Khoo
Boo Cheong Khoo
We present a numerical study of nanosecond pulsed dielectric barrier discharge (DBD) actuator operating in quiescent air at atmospheric condition. Our study concentrates on plasma discharge induced fluid dynamics and on exploration of parametric space of interest for voltage pulse in an attempt to shed some light into elucidation of the mechanisms whereby the generated shock wave propagates through and affects the external flow. Specifically, a one-dimensional, self-similar, local ionization kinetic model recently developed to predict key parameters of nanosecond pulsed plasma discharge is coupled with the compressible Navier-Stokes equations possibly for the first time. Within the considered range of parameters of the plasma model which is justified for the modeling of surface nanosecond pulsed discharge at atmospheric pressure, our coupled method is able to provide satisfactory prediction of the shock structure generated by the actuator for comparison with experiment, not only in the qualitative shock wave shape but also in quantitative shock front displacement. We provide a comprehensive analysis of the gas heating, shock wave initiation and evolution processes. For example, the characteristic time of the rapid localized heating responsible for shock wave generation, which is yet to be quantified experimentally, is found to be ∼350 ns. We conduct a parametric investigation by varying the peak voltage from 10 kV to 50 kV and rise time from 5 ns to 150 ns. The pressure wave whose behavior is found to be dominated by input voltage amplitude, introduces highly transient, localized disturbance to the quiescent air. In addition, the vortex induced by the shock passage is relatively weak. The interplay of the induced flows by a few successive plasma discharges operating at continuous mode does not appear to be significant, especially at low voltage amplitude.

1 October 2019 in Physics of Fluids
Verified
Journal Article
Open access
PDF file
Hao DongHao Dong
Hao Dong
TXTianyu Xia
Tianyu Xia
LCLin Chen
Lin Chen
SLShicheng Liu
Shicheng Liu
YCYongdong Cui
Yongdong Cui
AZAihong Zhao
Aihong Zhao
As typical flow characteristics in a low Reynolds number, laminar separation bubbles (LSBs) and transition to turbulence over airfoils have been extensively studied in recent years. In order to analyze their flow mechanism, numerical investigation using the finite volume method to solve the Reynolds averaged Navier-Stokes equations with a transition Shear Stress Transport (SST) four-equation transition model is performed in this work, combined with the experimental study facilitated by the oil film interferometry technique. Specifically, the transition SST four-equation transition model is solved to simulate the separation location and LSB structure at low Reynolds numbers on a Wortmann FX63-137 airfoil. Good agreement is obtained between the numerical simulation and experimental measurements regarding the separation, transition and reattachment location, aerodynamic coefficients, and overall flow structures. At higher Reynolds numbers of 200 000 and 300 000, similar bubble structures on the airfoil surface are observed, and the location of the bubble moves toward the leading edge of the airfoil by increasing the angle of attack. However, in Reynolds numbers ranging from 300 000 to 500 000, significant changes of the laminar flow separation structures emerge. The flow structure changes from the classical laminar separation bubble to the nonclassical separation flow structure that is composed of a major vortex 1(V1) and a minor vortex 2(V2). Due to the small distance between V1 and V2, it is difficult to distinguish the delicate structure of the two separation bubbles from the classical laminar separation bubble by the experimental method.