Baoshou Zhang

Dr. Baoshou Zhang

orcid

Research Focus & Metrics

Academic Career Length

9Years (2018-Present)

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

Representative Publications

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1 February 2023 in Petroleum Science
Verified
Journal Article
Open access
Taohua HeTaohua He
Taohua He
WLWenhao Li
Wenhao Li
SLShuangfang Lu
Shuangfang Lu
EYEr-Qiang Yang
Er-Qiang Yang
TJTao-Tao Jing
Tao-Tao Jing
ZCZhonghong Chen
Zhonghong Chen

4 December 2023 in Energy
Verified
Journal Article
Closed access
BZBaoshou Zhang
Baoshou Zhang
BLBoyang Li
Boyang Li
CLCanpeng Li
Canpeng Li
YZYongbo Zhang
Yongbo Zhang
JLJingze Lv
Jingze Lv
HYHaidong Yu
Haidong Yu

1 January 2018 in Applied Ocean Research
Verified
Journal Article
Closed access
BZBaoshou Zhang
Baoshou Zhang
BSBaowei Song
Baowei Song
ZMZhaoyong Mao
Zhaoyong Mao
Boyang LiBoyang Li
Boyang Li

Verified
Journal Article
Open access
PDF file
JLJian Li
Jian Li
PWPeng Wang
Peng Wang
XAXiaoyi An
Xiaoyi An
DLDa Lyu
Da Lyu
RHRuixuan He
Ruixuan He
BZBaoshou Zhang
Baoshou Zhang
Flapping foils are studied to achieve an efficient propeller. The performance of the flapping foil is influenced by many factors such as oncoming vortices, heaving amplitude, and geometrical parameters. In this paper, investigations are performed on flapping foils to assess its performance in the wake of a D-section cylinder located half a diameter in front of the foil. The effects of heaving amplitude and foil thickness are examined. The results indicate that oncoming vortices facilitate the flapping motion. Although the thrust increases with the increasing heaving amplitude, the propelling efficiency decreases with it. Moreover, increasing thickness results in higher efficiency. The highest propelling efficiency is achieved when the heaving amplitude equals ten percent of the chord length with a symmetric foil type of NACA0050 foil. When the heaving amplitude is small, the influence of the thickness tends to be more remarkable. The propelling efficiency exceeds 100% and the heaving amplitude is 10% of the chord length when the commonly used equation is adopted. This result demonstrates that the flapping motion extracts some energy from the oncoming vortices. Based on the numerical results, a new parameter, the energy transforming ratio (RET), is applied to explicate the energy transforming procedure. The RET represents that the flapping foil is driven by the engine or both the engines and the oncoming vortices with the range of RET being (0, Infini) and (−1, 0), respectively. With what has been discussed in this paper, the oncoming wake of the D-section cylinder benefits the flapping motion which indicates that the macro underwater vehicle performs better following a bluff body.

12 January 2023 in Energy
Verified
Journal Article
Closed access
BLBoyang Li
Boyang Li
CLCanpeng Li
Canpeng Li
BZBaoshou Zhang
Baoshou Zhang
FDFang Deng
Fang Deng
HYHualin Yang
Hualin Yang

1 August 2024 in Physics of Fluids
Verified
Journal Article
Closed access
PDF file
SLShenfang Li
Shenfang Li
Junlei WangJunlei Wang
Junlei Wang
BZBaoshou Zhang
Baoshou Zhang
PHPeng Han
Peng Han
The present work employs the immersed boundary method to perform direct simulations of flow-induced vibrations in a tandem cylinder at laminar flows, where only the upstream cylinder (UC) is allowed to vibrate. The primary focus is to elucidate the vibration response of the UC and the underlying hydrodynamic mechanisms when a fixed downstream cylinder (DC) is introduced. The results indicate that varying spacing ratios (L/D) and reduced velocities (U*) leads to both self-limiting galloping and lock-in instabilities in the UC. The resonance regions for the UC can be categorized into different regimes, such as lock-in, harmonic lock-in (HLN), upper branch, and lower branch regimes, based on various mechanisms. Notably, the vibrations in the HLN regime are distinct from the traditional lock-in observed in a bare cylinder, with the oscillation frequency locking onto the higher-order fluid force frequency and the occurrence of larger amplitudes. Regarding the interference galloping instability, we show that the self-limiting amplitude is related to the vortex shedding points on either side of the DC. The introduction of a fixed DC results in the observation of six vortex shedding modes: C(2S), 2S, P+T, 2T, 2P, and Aperiodic. Among these, weak vortices in the 2P mode are found to suppress the vibration amplitude. The asymmetrical and aperiodic evolution of the wake flow generates even-order fluid forces. Furthermore, an analysis of the energy transfer indicates that the tandem cylinders exhibit high fluid kinetic energy conversion ability over a wide range of U*−L/D.