北英 刘

Dr. 北英 刘

orcid

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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12 December 2014 in Tumor Biology
Verified
Journal Article
Closed access
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FMFang Mei
Fang Mei
JYJiangfeng You
Jiangfeng You
北刘北英 刘
北英 刘
MZMengxue Zhang
Mengxue Zhang
JLJiangying Liu
Jiangying Liu
FPFei Pei
Fei Pei

9 April 2025 in Polymers
Verified
Journal Article
Open access
PDF file
SQSheng Qu
Sheng Qu
QZQi Zhang
Qi Zhang
北刘北英 刘
北英 刘
Wei LiWei Li
Wei Li
YWYesong Wang
Yesong Wang
JLjisheng liu
jisheng liu
Successful continuous fiber-reinforced composite filament 3D printing hinges on the synergistic relationship between the printing nozzle and precisely controlled process parameters. This research uses a simulation model to investigate how printing temperature, printing speed, and nozzle length affect the prepreg filament’s molten state during 3D printing. We employed the Box–Behnken response surface methodology to optimize these key parameters. Using continuous fiber-reinforced composite filament polylactic acid (CFRCF/PLA) as an example, and a printing nozzle with a 1 mm diameter and an 8 mm length of heating zone were designed. The optimal printing parameters were determined to be as follows: printing temperature of 220 °C, printing speed of 300 mm/min, and printing layer height of 0.2 mm. Experimental validation using the optimized nozzle and parameters demonstrated enhanced stability in continuous fiber prepreg filament printing.

17 February 2022 in Journal of Fluids Engineering
Verified
Journal Article
Closed access
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WYWenming Yang
Wenming Yang
BFBoshi Fang
Boshi Fang
北刘北英 刘
北英 刘
Backward-facing step (BFS) flow is a benchmark case study in fluid mechanics. Its control by means of electromagnetic actuation has attracted great interest in recent years. This paper focuses on the effects of a uniform stationary magnetic field on the laminar ferrofluid BFS flows for the Reynolds number range 0.1≤Re≤400 and different expansion ratios. The coupled ferrohydrodynamic equations, including the microscopically derived magnetization equation, for a two-dimensional domain are solved numerically by an openfoam solver after validation and a test of accuracy. The application of a magnetic field causes the corner vortices in the concave corner behind the step to be retracted compared with their positions in the absence of a magnetic field. The maximum percentage of the normalized decrease in length of these eddies reaches 41.23% in our simulations. For small Reynolds numbers (<10), the flow separation points on the convex corner are lowered in the presence of a magnetic field. Furthermore, the dimensionless total pressure drop between the channel inlet and outlet decreases almost linearly with Reynolds number Re⁠, but the drop is greater when a magnetic field is applied. On the whole, the normalized recirculation length of the corner vortex increases nonlinearly with increasing magnetic Reynolds number Rem and Brownian Péclet number Pe⁠, but it tends to constant values in the limits Rem≪1 and Rem≫1⁠.

30 November 2023 in Materials
Verified
Journal Article
Open access
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CCChen Cheng
Chen Cheng
北刘北英 刘
北英 刘
JCJinxin Cheng
Jinxin Cheng
XXXIAO XIONG
XIAO XIONG
Accurate prediction of Electro-Discharge Machining (EDM) results is crucial for industrial applications, aiming to achieve high-performance and cost-efficient machining. However, both the current physical model and the standard Artificial Neural Network (ANN) model exhibit inherent limitations, failing to fully meet the accurate requirements for predicting EDM machining results. In addition, Micro-EDM Drilling can lead to the distortion of the macroscopic shape of machining pits under different input conditions, rendering the use of only the volume of machining pits as the evaluation index insufficient to express the complete morphological information. In this study, we propose a novel hybrid prediction model that combines the strengths of both physical and data-driven models to simultaneously predict Material Removal Rate (MRR) and shape parameters. Our experiment demonstrates that the hybrid model achieves a maximum prediction error of 4.92% for MRR and 5.28% for shape parameters, showcasing excellent prediction accuracy and stability compared to the physical model and the standard ANN model.

6 August 2018 in IEEE Transactions on Plasma Science
Verified
Journal Article
Closed access
WYWenming Yang
Wenming Yang
RZRong Zhu
Rong Zhu
CZChao Zhang
Chao Zhang
北刘北英 刘
北英 刘
It is necessary to recognize the spatial distribution of ion density and temperature in some practical applications. While numerical modeling is a useful method to fulfill this task, a self-consistent numerical model based on the first few moments of the Boltzmann transport equation coupled to Poisson's equation was built using COMSOL Multiphysics to simulate the dc discharge of a needle-to-plane geometry in atmospheric pressure. Simulation of the discharge was carried out for an actual geometry in aerosol sensors when only the main compositions of air and the main collisional populating and depopulating processes were considered. The simulation results demonstrated that the space occupied by the positive ions with a density of sufficiently charging aerosol particles was very limited. In the meanwhile, the electron temperature in the vicinity of the entire plane electrode was higher than the melting point of most metals. Experiments of measuring the current inducted by charged particles with a diameter of 95 nm using devices with narrowed channels showed that the specific current increased to nearly five times when the width of the channel in the charging stage decreases from 5 to 2 mm. Furthermore, the ablation of the plane electrode used in the experiments occurred on almost the entire surface, which was agreed with the prediction by simulation.

1 November 2018 in Pathology - Research and Practice
Verified
Journal Article
Closed access
XLXinying Liu
Xinying Liu
DLDan Liu
Dan Liu
XWXiaoqiang Wang
Xiaoqiang Wang
RWRui Wu
Rui Wu
ZKzhang kuangen
zhang kuangen
FPFei Pei
Fei Pei