An-Kang Gao
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
An-Kang Gao has a total of 57 co-authors. Here are the top co-authors by number of shared publications:
- Xi-Yun Lu
University of Science and Technology of China
12 shared publications - Luoqin Liu
University of Science and Technology of China
4 shared publications - Nan-Sheng Liu
University of Science and Technology of China
3 shared publications - Shaohua Chen
Beijing Institute of Technology
3 shared publications Yipeng Shi
State Key Laboratory for Turbulence and Complex Systems, Peking University, 100871 Beijing, People’s Republic of China
3 shared publications- Chenyue Xie
University of Science and Technology of China
2 shared publications
Latest Publications
- 29 October 2026
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1046, A21
Bifurcation of laterally unconstrained flexible filaments in an inclined flow
The dynamics of laterally unconstrained flexible filaments in an inclined uniform flow is investigated numerically, inspired by the self-propelled behaviour of droplets and filaments in a crosswind. It is found that in addition to conventional downwind drifting, the filament can also undergo counterintuitive upwind motion, arising from a supercritical pitchfork bifurcation. Depending on the Reynolds number, bending stiffness and inflow inclination angle, the filament exhibits multiple wake and motion states, including static, quasi-static, vibrational and translational modes. In the reference frame translating laterally with the incoming flow, the upwind and downwind drifting states induced by different initial perturbations form a pair of dynamically equivalent, symmetry-related branches. Force decomposition shows that both the streamwise drag and lateral thrust predominantly originate from the normal force, and the corresponding scaling relations are identified. Stability analysis further reveals that the hydrodynamic forces near the equilibrium states behave as restoring forces. The resulting stable equilibria can be characterised by a generalised hydrodynamic potential, whose potential wells correspond to the stable states of the system. These findings provide insight into the dynamics of flexible structures in uniform flow.
- 29 October 2026
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1046, A21
Bifurcation of laterally unconstrained flexible filaments in an inclined flow
The dynamics of laterally unconstrained flexible filaments in an inclined uniform flow is investigated numerically, inspired by the self-propelled behaviour of droplets and filaments in a crosswind. It is found that in addition to conventional downwind drifting, the filament can also undergo counterintuitive upwind motion, arising from a supercritical pitchfork bifurcation. Depending on the Reynolds number, bending stiffness and inflow inclination angle, the filament exhibits multiple wake and motion states, including static, quasi-static, vibrational and translational modes. In the reference frame translating laterally with the incoming flow, the upwind and downwind drifting states induced by different initial perturbations form a pair of dynamically equivalent, symmetry-related branches. Force decomposition shows that both the streamwise drag and lateral thrust predominantly originate from the normal force, and the corresponding scaling relations are identified. Stability analysis further reveals that the hydrodynamic forces near the equilibrium states behave as restoring forces. The resulting stable equilibria can be characterised by a generalised hydrodynamic potential, whose potential wells correspond to the stable states of the system. These findings provide insight into the dynamics of flexible structures in uniform flow.
- Open Access
- 12 August 2026
- Published by Walter de Gruyter GmbH in Transport Phenomena
- Vol. 1 (3)
A perspective on unsteady aerodynamic force theories: from the diagnostics of global loads to that of local stress distributions
This paper reviews field-based diagnostic theories of unsteady aerodynamic forces, ranging from formulations for total force and moment to recent developments in the diagnosis of local stress distributions. We first revisit the vorticity-moment theory (Wu, AIAA J, vol. 19, 1981, 432–441) as a starting point for field-based force analysis, with emphasis on far-field decay requirements and subsequent extensions to finite domains and compressible flows. We then consider the vortex-force theory and force-element theory, which provide more physically interpretable connections between the flow field and aerodynamic loads. Subsequently, we discuss decompositions of the pressure field based on its governing equation and boundary conditions. Finally, we examine the transition from total force and moment analysis to the diagnosis of local surface loading through weighted-integral methods. Overall, unsteady aerodynamic force theories have evolved from asking how the total load can be calculated from the surrounding flow field to asking how individual flow structures and physical processes determine the distribution of stress over the body surface.
- 12 August 2026
- Published by Walter de Gruyter GmbH in Transport Phenomena
- Vol. 1 (3)
Open AccessA perspective on unsteady aerodynamic force theories: from the diagnostics of global loads to that of local stress distributions
This paper reviews field-based diagnostic theories of unsteady aerodynamic forces, ranging from formulations for total force and moment to recent developments in the diagnosis of local stress distributions. We first revisit the vorticity-moment theory (Wu, AIAA J, vol. 19, 1981, 432–441) as a starting point for field-based force analysis, with emphasis on far-field decay requirements and subsequent extensions to finite domains and compressible flows. We then consider the vortex-force theory and force-element theory, which provide more physically interpretable connections between the flow field and aerodynamic loads. Subsequently, we discuss decompositions of the pressure field based on its governing equation and boundary conditions. Finally, we examine the transition from total force and moment analysis to the diagnosis of local surface loading through weighted-integral methods. Overall, unsteady aerodynamic force theories have evolved from asking how the total load can be calculated from the surrounding flow field to asking how individual flow structures and physical processes determine the distribution of stress over the body surface.
- Open Access
- 18 June 2026
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1037, A39
Dynamic interactions between a self-propelled flexible plate and multiple wall-mounted compliant blades
A numerical study is conducted on a self-propelled flexible plate moving above an array of wall-mounted compliant blades at Reynolds numbers of order 100, designed to mimic flatfish-like locomotion near the vegetation-covered seabed. Compared with a flat rigid wall located at the same vertical distance from the plate, the blade-covered wall enhances the propulsive performance of the plate, yielding a higher propulsive velocity and lower energy consumption per transport distance. This enhancement intensifies as the blade spacing and vertical distance between the plate and the bottom wall decrease, but diminishes when the flapping frequency approaches the natural frequency of the blades due to resonance. By accounting for the asymmetric motion of the plate during the upper and lower half-periods, a universal scaling law italic Re Subscript c Baseline tilde left parenthesis italic Re Subscript f comma delta Baseline right parenthesis Superscript 3 divided by 2 ${\textit{Re}}_c\sim ({\textit{Re}}_{f,\delta })^{3/2}$ is identified between the propulsive Reynolds number italic Re Subscript c ${\textit{Re}}_c$ and the corrected flapping Reynolds number italic Re Subscript f comma delta ${\textit{Re}}_{f,\delta }$ . Under the excitation of the flapping plate, two distinct vibration patterns are identified for the blade array. The first is the flapping-driven mode, which propagates synchronously with the plate’s motion. The second exhibits forward-propagating travelling waves, which are generated by the cooperative underdamped vibrations of downstream blades, and have a phase velocity much faster than the propulsive velocity of the plate. This study may shed light on the design of bio-inspired underwater vehicles and flow sensing techniques.- 18 June 2026
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1037, A39
Open AccessDynamic interactions between a self-propelled flexible plate and multiple wall-mounted compliant blades
A numerical study is conducted on a self-propelled flexible plate moving above an array of wall-mounted compliant blades at Reynolds numbers of order 100, designed to mimic flatfish-like locomotion near the vegetation-covered seabed. Compared with a flat rigid wall located at the same vertical distance from the plate, the blade-covered wall enhances the propulsive performance of the plate, yielding a higher propulsive velocity and lower energy consumption per transport distance. This enhancement intensifies as the blade spacing and vertical distance between the plate and the bottom wall decrease, but diminishes when the flapping frequency approaches the natural frequency of the blades due to resonance. By accounting for the asymmetric motion of the plate during the upper and lower half-periods, a universal scaling law italic Re Subscript c Baseline tilde left parenthesis italic Re Subscript f comma delta Baseline right parenthesis Superscript 3 divided by 2 ${\textit{Re}}_c\sim ({\textit{Re}}_{f,\delta })^{3/2}$ is identified between the propulsive Reynolds number italic Re Subscript c ${\textit{Re}}_c$ and the corrected flapping Reynolds number italic Re Subscript f comma delta ${\textit{Re}}_{f,\delta }$ . Under the excitation of the flapping plate, two distinct vibration patterns are identified for the blade array. The first is the flapping-driven mode, which propagates synchronously with the plate’s motion. The second exhibits forward-propagating travelling waves, which are generated by the cooperative underdamped vibrations of downstream blades, and have a phase velocity much faster than the propulsive velocity of the plate. This study may shed light on the design of bio-inspired underwater vehicles and flow sensing techniques. - 18 May 2026
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 11 (5)
Fluid transport by flexible blades performing impulsive metachronal rowing
- 18 May 2026
- Published by American Physical Society (APS) in Physical Review Fluids
- Vol. 11 (5)
Fluid transport by flexible blades performing impulsive metachronal rowing
- Open Access
- 27 April 2026
- Published by Elsevier in SSRN Electronic Journal
A stabilized velocity-correction scheme for fluid-rigid-body interaction in incompressible flows via pressure decomposition
In the velocity-correction scheme (VCS) for incompressible fluid–rigid-body interaction, numerical instability often arises from the explicit treatment of the Neumann pressure boundary condition on the body surface, where the wall acceleration at the new time step is approximated from velocity fields at previous time steps through a finite-difference method. To address this issue, we propose a stabilized VCS based on a decomposition of the pressure field into velocity-induced and acceleration-induced components, referred to as the pressure-decomposed velocity-correction scheme (PD-VCS). In the proposed method, only the velocity-induced pressure needs to be calculated from the pressure Poisson equation. The acceleration-induced component is implicitly included in the rigid-body equations of motion. This treatment eliminates the dependence of the numerical pressure boundary condition on the rigid-body acceleration and augments the effective inertia of the body, without introducing additional free parameters or coupling iterations. Numerical results demonstrate that the proposed method is stable and accurate over a wide range of density ratios, including the zero-mass limit of the rigid body.
- 27 April 2026
- Published by Elsevier in SSRN Electronic Journal
Open AccessA stabilized velocity-correction scheme for fluid-rigid-body interaction in incompressible flows via pressure decomposition
In the velocity-correction scheme (VCS) for incompressible fluid–rigid-body interaction, numerical instability often arises from the explicit treatment of the Neumann pressure boundary condition on the body surface, where the wall acceleration at the new time step is approximated from velocity fields at previous time steps through a finite-difference method. To address this issue, we propose a stabilized VCS based on a decomposition of the pressure field into velocity-induced and acceleration-induced components, referred to as the pressure-decomposed velocity-correction scheme (PD-VCS). In the proposed method, only the velocity-induced pressure needs to be calculated from the pressure Poisson equation. The acceleration-induced component is implicitly included in the rigid-body equations of motion. This treatment eliminates the dependence of the numerical pressure boundary condition on the rigid-body acceleration and augments the effective inertia of the body, without introducing additional free parameters or coupling iterations. Numerical results demonstrate that the proposed method is stable and accurate over a wide range of density ratios, including the zero-mass limit of the rigid body.
- 1 April 2026
- Published by AIP Publishing in Physics of Fluids
- Vol. 38 (4)
Drag reduction of SUBOFF model with deep-learning-optimized distributed partial-slip boundaries
Partial-slip boundaries have been demonstrated to be effective at drag reduction of underwater vehicles. However, in practical applications, covering the entire body surface with slip materials is cost-inefficient. To address this issue, a deep learning-based approach is developed to optimize the spatial distribution of slip boundaries on the SUBOFF bare-hull model under prescribed engineering constraints. First, a convolutional neural network surrogate model is trained to predict drag efficiently, enabling rapid evaluation of different slip-boundary configurations. The optimal distribution is then determined through systematic exploration of the parameter space. Numerical simulations of the optimized configurations reveal two key findings: (1) slip boundaries significantly influence the skin-friction drag, whereas their effect on pressure drag remains negligible and (2) a well-designed distributed partial-slip boundary can effectively regulate the development of near-wall turbulence, leading to enhanced the overall drag reduction performance. This study provides a promising framework for the intelligent design of drag-reducing surfaces for underwater vehicles.
- 1 April 2026
- Published by AIP Publishing in Physics of Fluids
- Vol. 38 (4)
Drag reduction of SUBOFF model with deep-learning-optimized distributed partial-slip boundaries
Partial-slip boundaries have been demonstrated to be effective at drag reduction of underwater vehicles. However, in practical applications, covering the entire body surface with slip materials is cost-inefficient. To address this issue, a deep learning-based approach is developed to optimize the spatial distribution of slip boundaries on the SUBOFF bare-hull model under prescribed engineering constraints. First, a convolutional neural network surrogate model is trained to predict drag efficiently, enabling rapid evaluation of different slip-boundary configurations. The optimal distribution is then determined through systematic exploration of the parameter space. Numerical simulations of the optimized configurations reveal two key findings: (1) slip boundaries significantly influence the skin-friction drag, whereas their effect on pressure drag remains negligible and (2) a well-designed distributed partial-slip boundary can effectively regulate the development of near-wall turbulence, leading to enhanced the overall drag reduction performance. This study provides a promising framework for the intelligent design of drag-reducing surfaces for underwater vehicles.
- Open Access
- 19 January 2026
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1027
Flapping dynamics of a compliant membrane in a uniform incoming flow
Recent theoretical and experimental investigations have revealed that flapping compliant membrane wings can significantly enhance propulsive performance (e.g. Tzezana & Breuer J. Fluid Mech. , 2019, vol. 862, pp. 871–888) and energy harvesting efficiency (e.g. Mathai et al. J. Fluid Mech. , 2022, vol. 942, p. R4) compared with rigid foils. Here, we numerically investigate the effects of the in-plane stretching stiffness (or aeroelastic number), $K_{\!S}$ , the flapping frequency, ${\textit{St}}_c$ , and the pitching amplitude, $\theta _0$ , on the propulsive performance of a compliant membrane undergoing combined heaving and pitching in uniform flow. Distinct optimal values of $K_{\!S}$ are identified that respectively maximise thrust and efficiency: thrust can be increased by 200 %, and efficiency by 100 %, compared with the rigid case. Interestingly, these optima do not occur at resonance but at frequency ratios (flapping to natural) below unity, and this ratio increases with flapping frequency. Using a force decomposition based on the second invariant of the velocity gradient tensor $Q$ , which measures the relative strength between the rotation and deformation of fluid elements, we show that thrust primarily arises from $Q$ -induced and body-acceleration forces. The concave membrane surface can trap the leading-edge vortex (LEV) generated during the previous half-stroke, generating detrimental $Q$ -induced drag. However, moderate concave membrane deformation weakens this LEV and enhances body-acceleration-induced thrust. Thus, the optimal $K_{\!S}$ for maximum thrust occurs below resonance, balancing beneficial deformation against excessive drag. Furthermore, by introducing the membrane’s deformation into a tangential angle at the leading edge and substituting it into an existing scaling law developed for rigid plates, we obtain predictive estimates for the thrust and power coefficients of the membrane. The good agreement confirms the validity of this approach and offers insights for performance prediction.- 19 January 2026
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1027
Open AccessFlapping dynamics of a compliant membrane in a uniform incoming flow
Recent theoretical and experimental investigations have revealed that flapping compliant membrane wings can significantly enhance propulsive performance (e.g. Tzezana & Breuer J. Fluid Mech. , 2019, vol. 862, pp. 871–888) and energy harvesting efficiency (e.g. Mathai et al. J. Fluid Mech. , 2022, vol. 942, p. R4) compared with rigid foils. Here, we numerically investigate the effects of the in-plane stretching stiffness (or aeroelastic number), $K_{\!S}$ , the flapping frequency, ${\textit{St}}_c$ , and the pitching amplitude, $\theta _0$ , on the propulsive performance of a compliant membrane undergoing combined heaving and pitching in uniform flow. Distinct optimal values of $K_{\!S}$ are identified that respectively maximise thrust and efficiency: thrust can be increased by 200 %, and efficiency by 100 %, compared with the rigid case. Interestingly, these optima do not occur at resonance but at frequency ratios (flapping to natural) below unity, and this ratio increases with flapping frequency. Using a force decomposition based on the second invariant of the velocity gradient tensor $Q$ , which measures the relative strength between the rotation and deformation of fluid elements, we show that thrust primarily arises from $Q$ -induced and body-acceleration forces. The concave membrane surface can trap the leading-edge vortex (LEV) generated during the previous half-stroke, generating detrimental $Q$ -induced drag. However, moderate concave membrane deformation weakens this LEV and enhances body-acceleration-induced thrust. Thus, the optimal $K_{\!S}$ for maximum thrust occurs below resonance, balancing beneficial deformation against excessive drag. Furthermore, by introducing the membrane’s deformation into a tangential angle at the leading edge and substituting it into an existing scaling law developed for rigid plates, we obtain predictive estimates for the thrust and power coefficients of the membrane. The good agreement confirms the validity of this approach and offers insights for performance prediction. - Open Access
- 1 January 2026
- Published by Journal of University of Science and Technology of China in JUSTC
- Vol. 55 (4) , 0402
Flow-induced vibration of plate and cylinder under unilateral spring constraint
Schematic diagram of unilateral constraint models and their hydrodynamic characteristics differences with bilateral constraints.
- 1 January 2026
- Published by Journal of University of Science and Technology of China in JUSTC
- Vol. 55 (4) , 0402
Open AccessFlow-induced vibration of plate and cylinder under unilateral spring constraint
Schematic diagram of unilateral constraint models and their hydrodynamic characteristics differences with bilateral constraints.
- 10 December 2025
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1024, A57
Weighted integral methods for fluid force diagnostics in incompressible flows
Whilst surface-stress integration remains the standard approach for fluid force evaluation, control-volume integral methods provide deeper physical insights through functional relationships between the flow field and the resultant force. In this work, by introducing a second-order tensor weight function into the Navier–Stokes equations, we develop a novel weighted-integral framework that offers greater flexibility and enhanced capability for fluid force diagnostics in incompressible flows. Firstly, in addition to the total force and moment, the weighted integral methods establish, for the first time, rigorous quantitative connections between the surface-stress distribution and the flow field, providing potential advantages for flexible body analyses. Secondly, the weighted integral methods offer alternative perspectives on force mechanisms, through vorticity dynamics or pressure view, when the weight function is set as divergence-free or curl-free, respectively. Thirdly, the derivative moment transformation (DMT)-based integral methods (Wu et al., J. Fluid Mech. vol. 576, 2007, 265–286) are generalised to weighted formulations, by which the interconnections among the three DMT methods are clarified. In the canonical problem of uniform flow past a circular cylinder, weighted integral methods demonstrate advantages in yielding new force expressions, improving numerical accuracy over original DMT methods, and enhancing surface-stress analysis. Finally, a force expression is derived that relies solely on velocity and acceleration at discrete points, without spatial derivatives, offering significant value for experimental force estimation. This weighted integral framework holds significant promise for flow diagnostics in fundamentals and applications.
- 10 December 2025
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1024, A57
Weighted integral methods for fluid force diagnostics in incompressible flows
Whilst surface-stress integration remains the standard approach for fluid force evaluation, control-volume integral methods provide deeper physical insights through functional relationships between the flow field and the resultant force. In this work, by introducing a second-order tensor weight function into the Navier–Stokes equations, we develop a novel weighted-integral framework that offers greater flexibility and enhanced capability for fluid force diagnostics in incompressible flows. Firstly, in addition to the total force and moment, the weighted integral methods establish, for the first time, rigorous quantitative connections between the surface-stress distribution and the flow field, providing potential advantages for flexible body analyses. Secondly, the weighted integral methods offer alternative perspectives on force mechanisms, through vorticity dynamics or pressure view, when the weight function is set as divergence-free or curl-free, respectively. Thirdly, the derivative moment transformation (DMT)-based integral methods (Wu et al., J. Fluid Mech. vol. 576, 2007, 265–286) are generalised to weighted formulations, by which the interconnections among the three DMT methods are clarified. In the canonical problem of uniform flow past a circular cylinder, weighted integral methods demonstrate advantages in yielding new force expressions, improving numerical accuracy over original DMT methods, and enhancing surface-stress analysis. Finally, a force expression is derived that relies solely on velocity and acceleration at discrete points, without spatial derivatives, offering significant value for experimental force estimation. This weighted integral framework holds significant promise for flow diagnostics in fundamentals and applications.
- 18 September 2025
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1019, A23
Transition of large-scale circulation in thermal convection driven by heat-releasing particles
Large-scale circulation (LSC) dynamics have been studied in thermal convection driven by heat-releasing particles via the four-way coupled Euler–Lagrange approach. We consider a wide range of Rayleigh–Robert number ( ${\textit{Rr}}=4.97\times 10^{5} - 4.97 \times 10^{8}$ ) and density ratio ( $\hat {\rho }_r=1- 1000$ ) that characterize the thermal buoyancy and the particle inertia, respectively. An intriguing flow transition has been found as $\hat {\rho }_r$ continuously increases, involving in sequence three typical LSC regimes, i.e. the bulk-flow-up regime, the marginal regime and the bulk-flow-down (BFD) regime. The comprehensive influence of the LSC regime transition is demonstrated by examining the key flow statistics. As integral flow responses, the heat transfer efficiency and flow intensity change substantially when the LSC regime transition happens, and the thermal boundary layer thicknesses at the top and bottom walls exhibit similar alterations. Significant local accumulation of particles occurs as $\hat {\rho }_r$ increases to a sufficiently high value, resulting in a great modification in the flow dynamics. Specifically, particles aggregate near the sidewalls and heat the local surrounding fluid to generate rising warmer plumes that drive the LSC regime transition. Of interest, well-patterned cellular structures of particles take place near the top wall and obtain notable deviation from the thermal convection cells for the BFD regimes. A mechanical interpretation is proposed and substantiated based on a conceptual vortex–particle model, namely, the centrifugal motion of heat-releasing particles that is confirmed to play a driving role for the LSC regime transition.- 18 September 2025
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 1019, A23
Transition of large-scale circulation in thermal convection driven by heat-releasing particles
Large-scale circulation (LSC) dynamics have been studied in thermal convection driven by heat-releasing particles via the four-way coupled Euler–Lagrange approach. We consider a wide range of Rayleigh–Robert number ( ${\textit{Rr}}=4.97\times 10^{5} - 4.97 \times 10^{8}$ ) and density ratio ( $\hat {\rho }_r=1- 1000$ ) that characterize the thermal buoyancy and the particle inertia, respectively. An intriguing flow transition has been found as $\hat {\rho }_r$ continuously increases, involving in sequence three typical LSC regimes, i.e. the bulk-flow-up regime, the marginal regime and the bulk-flow-down (BFD) regime. The comprehensive influence of the LSC regime transition is demonstrated by examining the key flow statistics. As integral flow responses, the heat transfer efficiency and flow intensity change substantially when the LSC regime transition happens, and the thermal boundary layer thicknesses at the top and bottom walls exhibit similar alterations. Significant local accumulation of particles occurs as $\hat {\rho }_r$ increases to a sufficiently high value, resulting in a great modification in the flow dynamics. Specifically, particles aggregate near the sidewalls and heat the local surrounding fluid to generate rising warmer plumes that drive the LSC regime transition. Of interest, well-patterned cellular structures of particles take place near the top wall and obtain notable deviation from the thermal convection cells for the BFD regimes. A mechanical interpretation is proposed and substantiated based on a conceptual vortex–particle model, namely, the centrifugal motion of heat-releasing particles that is confirmed to play a driving role for the LSC regime transition.