Donglai Gao

Dr. Donglai Gao

School of Civil Engineering, Harbin Institute of Technology, Harbin 150090, China

Research Focus & Metrics

Academic Career Length

12Years (2015-Present)

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

Representative Publications

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1 August 2021 in Journal of Fluids and Structures
Verified
Journal Article
Closed access
Donglai GaoDonglai Gao
Donglai Gao
ZDZhi Deng
Zhi Deng
WYWenhan Yang
Wenhan Yang
WCWenli Chen
Wenli Chen

1 April 2017 in Experimental Thermal and Fluid Science
Verified
Journal Article
Closed access
Donglai GaoDonglai Gao
Donglai Gao
Wen-Li ChenWen-Li Chen
Wen-Li Chen
HLHui Li
Hui Li
HHHui Hu
Hui Hu

1 July 2022 in Ocean Engineering
Verified
Journal Article
Closed access
Wen-Li ChenWen-Li Chen
Wen-Li Chen
YHYewei Huang
Yewei Huang
CCChanglong Chen
Changlong Chen
HYHaiyang Yu
Haiyang Yu
Donglai GaoDonglai Gao
Donglai Gao

30 October 2015 in Experiments in Fluids
Verified
Journal Article
Closed access
PDF file
Wen-Li ChenWen-Li Chen
Wen-Li Chen
Donglai GaoDonglai Gao
Donglai Gao
WYWen-Yong Yuan
Wen-Yong Yuan
HLHui Li
Hui Li
HHHui Hu
Hui Hu

10 January 2019 in Experiments in Fluids
Verified
Journal Article
Closed access
PDF file
Donglai GaoDonglai Gao
Donglai Gao
GuanBin ChenGuanBin Chen
GuanBin Chen
Wen-Li ChenWen-Li Chen
Wen-Li Chen
YHYewei Huang
Yewei Huang
HLHui Li
Hui Li

1 April 2021 in Physics of Fluids
Verified
Journal Article
Closed access
PDF file
Donglai GaoDonglai Gao
Donglai Gao
HMHao Meng
Hao Meng
YHYewei Huang
Yewei Huang
GuanBin ChenGuanBin Chen
GuanBin Chen
Wen-Li ChenWen-Li Chen
Wen-Li Chen
This study experimentally investigated an active flow control method with combined jets at the front and the rear stagnation points of a square cylinder to suppress the unsteady wake flow. The Reynolds number (Re) was 1.67 × 10 4 , based on the incoming speed of airflow and the diameter of test model. The square cylinder model was manufactured with two narrow slots symmetrically positioned at the centerline of the front and rear surfaces. The strength of the jets is characterized with a dimensionless momentum coefficient C μ . We obtained the dynamic wake flow regimes by employing the particle image velocimetry technique. Then, with the method of proper orthogonal decomposition and linear stability analysis, the time-averaged flow characteristics, e.g., turbulence kinetic energy (TKE) and the Reynolds shear stress (RSS) distributions, and the dynamic wake flow behind the square cylinder were analyzed in detail. Results of flow visualization suggested that at low momentum coefficient C μ the wake flow regime showed no notable modifications to the wake. As C μ increased to 0.0948, the periodic shear layers from the square cylinder were found to be pushed to the farther wake. Meanwhile, the time-averaged wake flow region was found to be greatly modified in the streamwise direction with a notable decrease in TKE and RSS distributions. The experimental results indicated that unsteadiness of vortex shedding in the wake flow experienced notable suppression. For higher C μ up to 0.2133 and 0.3793, unsteady vortex shedding from the square cylinder and the dynamic wake flow were further suppressed in the near wake. A linear stability analysis was also employed to reveal the underlying nature of wake modification by the combined jets.