Abhishek Lakshman Pillai
Abhishek Lakshman Pillai has a total of 39 co-authors. Here are the top co-authors by number of shared publications:
- Ryoichi Kurose
Kyoto University
15 shared publications Ryoichi Kurose
9 shared publicationsJiangkuan Xing
5 shared publications- Umair Ahmed
School of Engineering, Newcastle University, Newcastle upon Tyne NE1 7RU, UK
5 shared publications - Jun Nagao
Faculty of Humanities, Gifu Shotoku Gakuen University, Gifu 501-6194, Japan
4 shared publications - Takeshi Shoji
Japan Aerospace Exploration Agency
4 shared publications
Latest Publications
- Open Access
- 6 November 2026
- Published by Elsevier in Proceedings of the Combustion Institute
- Vol. 42
Enstrophy evolution in a laboratory-scale lean-premixed lifted hydrogen swirling flame
- 6 November 2026
- Published by Elsevier in Proceedings of the Combustion Institute
- Vol. 42
Open AccessEnstrophy evolution in a laboratory-scale lean-premixed lifted hydrogen swirling flame
- Open Access
- 19 January 2026
- Published by Elsevier in Combustion and Flame
- Vol. 286
Experimental and numerical investigation on flashback of low-swirling hydrogen–air jet flames
- 19 January 2026
- Published by Elsevier in Combustion and Flame
- Vol. 286
Open AccessExperimental and numerical investigation on flashback of low-swirling hydrogen–air jet flames
- 1 November 2024
- Published by AIP Publishing in Physics of Fluids
- Vol. 36 (11)
Pressure-equilibrium semi-implicit solver for real fluids
In this study, a semi-implicit pressure-based scheme which can suppress the spurious pressure oscillations is developed for real fluid flows. Conservation properties relevant to the proposed scheme are investigated through one-dimensional numerical simulations of the nitrogen interface advection. The efficiency and validity of this scheme are carefully examined with two- and three-dimensional numerical simulations of cryogenic nitrogen jets. From the one-dimensional simulation results, the conservation properties are well conserved as the past studies. The two-dimensional simulation results show that the developed scheme can reduce the computational cost by more than 92% (13–14 times faster) compared with the conventional density-based explicit solver employing the double flux model. It is also found that, through the three-dimensional simulation results, the developed scheme can predict the structure of the nitrogen jet under both transcritical and supercritical conditions, while taking into account the effects of real fluid properties on the mixing and spatiotemporal evolution of this jet, with excellent accuracy.
- 1 November 2024
- Published by AIP Publishing in Physics of Fluids
- Vol. 36 (11)
Pressure-equilibrium semi-implicit solver for real fluids
In this study, a semi-implicit pressure-based scheme which can suppress the spurious pressure oscillations is developed for real fluid flows. Conservation properties relevant to the proposed scheme are investigated through one-dimensional numerical simulations of the nitrogen interface advection. The efficiency and validity of this scheme are carefully examined with two- and three-dimensional numerical simulations of cryogenic nitrogen jets. From the one-dimensional simulation results, the conservation properties are well conserved as the past studies. The two-dimensional simulation results show that the developed scheme can reduce the computational cost by more than 92% (13–14 times faster) compared with the conventional density-based explicit solver employing the double flux model. It is also found that, through the three-dimensional simulation results, the developed scheme can predict the structure of the nitrogen jet under both transcritical and supercritical conditions, while taking into account the effects of real fluid properties on the mixing and spatiotemporal evolution of this jet, with excellent accuracy.
- 1 April 2024
- Published by AIP Publishing in Physics of Fluids
- Vol. 36 (4)
Effect of temporal increase in equivalence ratio on combustion instability of a lean-premixed swirling hydrogen flame
The effect of temporal increase in the equivalence ratio on the combustion instability of a lean-premixed low-swirl hydrogen jet flame in a low-swirl combustor (LSC) is investigated in detail using a high-fidelity Large-Eddy Simulation (LES). The equivalence ratio is linearly increased from 0.3 to 0.5 over a duration of 0.4 s. The results show that the pressure oscillation amplitude in the combustor increases significantly when the equivalence ratio at the combustor inlet (ERCI) exceeds 0.42, and the maximum pressure amplitude and the combustion instability mode exhibit trends consistent with those in a previous experiment and numerical simulation conducted with the same LSC setup at a fixed equivalence ratio of 0.39. Temporal variations in the equivalence ratio and consequently the temperature inside the combustor cause the drastic amplification of pressure oscillation (when the ERCI exceeds 0.42) whose amplitude is larger than that at the fixed equivalence ratio (= 0.39). Prior to the onset of this exceptionally strong combustion instability, a transient irregular oscillation phenomenon comprising instantaneous changes in the pressure oscillation frequency is observed. While the pressure oscillations in the combustor and in the injector channel are in phase after the onset of strong combustion instability, they are in opposite phases during the occurrence of the irregular oscillation phenomenon prior to the onset of strong combustion instability. This irregular oscillation phenomenon predicted by the LES may play a crucial role in the mechanism of transition from stable combustion to combustion instability.
- 1 April 2024
- Published by AIP Publishing in Physics of Fluids
- Vol. 36 (4)
Effect of temporal increase in equivalence ratio on combustion instability of a lean-premixed swirling hydrogen flame
The effect of temporal increase in the equivalence ratio on the combustion instability of a lean-premixed low-swirl hydrogen jet flame in a low-swirl combustor (LSC) is investigated in detail using a high-fidelity Large-Eddy Simulation (LES). The equivalence ratio is linearly increased from 0.3 to 0.5 over a duration of 0.4 s. The results show that the pressure oscillation amplitude in the combustor increases significantly when the equivalence ratio at the combustor inlet (ERCI) exceeds 0.42, and the maximum pressure amplitude and the combustion instability mode exhibit trends consistent with those in a previous experiment and numerical simulation conducted with the same LSC setup at a fixed equivalence ratio of 0.39. Temporal variations in the equivalence ratio and consequently the temperature inside the combustor cause the drastic amplification of pressure oscillation (when the ERCI exceeds 0.42) whose amplitude is larger than that at the fixed equivalence ratio (= 0.39). Prior to the onset of this exceptionally strong combustion instability, a transient irregular oscillation phenomenon comprising instantaneous changes in the pressure oscillation frequency is observed. While the pressure oscillations in the combustor and in the injector channel are in phase after the onset of strong combustion instability, they are in opposite phases during the occurrence of the irregular oscillation phenomenon prior to the onset of strong combustion instability. This irregular oscillation phenomenon predicted by the LES may play a crucial role in the mechanism of transition from stable combustion to combustion instability.
- 29 January 2024
- Published by Elsevier in Aerospace Science and Technology
- Vol. 146
Large-eddy simulation of blade-turbulence interaction in a cyclorotor system
- 29 January 2024
- Published by Elsevier in Aerospace Science and Technology
- Vol. 146
Large-eddy simulation of blade-turbulence interaction in a cyclorotor system
- Open Access
- 1 October 2023
- Published by AIP Publishing in Physics of Fluids
- Vol. 35 (10)
Large-eddy simulation of a lean-premixed hydrogen flame in a low-swirl combustor under combustion instability
Large-eddy simulation (LES) of a lean-premixed hydrogen turbulent jet flame with combustion instability (CI) in a low-swirl combustor (LSC) is performed by employing a dynamically thickened flame model with a detailed chemical reaction model with 9 chemical species and 20 reactions, and the LES validity and the CI characteristics are investigated in detail. The results show that the present LES can accurately reproduce the experimentally observed characteristics of the CI such as intensity, frequency, sporadic decay of pressure oscillations, and a flame–flow interaction inducing the periodic transitions of an inverted conical flame structure and a flat flame structure in the LSC. The sporadic decay of pressure oscillations and the flame–flow interaction are caused by the temporal decoupling of pressure and heat release rate and the periodic outward and inward deflections of the inflow, which is associated with the flow behavior in the upstream injector channel, respectively.
- 1 October 2023
- Published by AIP Publishing in Physics of Fluids
- Vol. 35 (10)
Open AccessLarge-eddy simulation of a lean-premixed hydrogen flame in a low-swirl combustor under combustion instability
Large-eddy simulation (LES) of a lean-premixed hydrogen turbulent jet flame with combustion instability (CI) in a low-swirl combustor (LSC) is performed by employing a dynamically thickened flame model with a detailed chemical reaction model with 9 chemical species and 20 reactions, and the LES validity and the CI characteristics are investigated in detail. The results show that the present LES can accurately reproduce the experimentally observed characteristics of the CI such as intensity, frequency, sporadic decay of pressure oscillations, and a flame–flow interaction inducing the periodic transitions of an inverted conical flame structure and a flat flame structure in the LSC. The sporadic decay of pressure oscillations and the flame–flow interaction are caused by the temporal decoupling of pressure and heat release rate and the periodic outward and inward deflections of the inflow, which is associated with the flow behavior in the upstream injector channel, respectively.