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Nitesh Kumar Sahu

Publications and source records attributed to Nitesh Kumar Sahu.

4 recordsLinked to original sources

Sensitivity of Isothermal Swirl Combustor Flow to Inlet Reynolds Number

Numerical simulations were conducted to investigate the influence of inlet Reynolds number on the isothermal flow field in a lab-scale swirl combustor while keeping a fixed inlet swirl number of 0.67. The combustor geometry and baseline conditions were adopted from Taamallah et al. [1]. Unlike the experimental setup, which used axial vane swirlers to generate rotation, this study imposed a velocity profile at the inlet to introduce swirl. The simulations employed the Reynolds averaged Navier Stokes (RANS) approach with the shear stress transport k omega turbulence model, using ANSYS Fluent 2024R2. A grid independence study was performed using meshes of approximately 0.4, 0.5, and 0.6 million elements. The turbulent kinetic energy varied by less than 2 percent between the 0.5M and 0.6M grids, confirming adequate mesh resolution. The solver was validated against experimental data from Taamallah et al. [1], showing good agreement in axial velocity distribution. The validated model was then used to simulate a higher Reynolds number of about 30000. Contours and centerline profiles of axial velocity were analyzed. An inner recirculation zone (IRZ), identified by negative axial velocity in the core, formed in both cases and plays a key role in flame stabilization. An outer recirculation zone (ORZ) was observed near the expansion plane. Increasing Reynolds number raised the peak forward axial velocity by about 46 percent and intensified reverse velocity at x = 0.10 m by nearly 68 percent, indicating stronger recirculation. However, the axial location of the IRZ remained nearly unchanged. These results suggest robust flame anchoring under varying inertial conditions. Reacting flow simulations are planned as future work.

physics.flu-dyn

Vortex breakdown and its topologies in turbulent flows within a typical swirl combustor geometry

We investigate vortex breakdown (VB) and its dominant topologies in turbulent, non-reacting flows within a canonical swirl combustor using large-eddy simulations (LES). A baseline configuration and operating conditions are first used to validate the LES solver, then five additional cases differing only by swirler vane-angle are simulated. The onset of VB is quantified using the generic swirl-number formulation, SNg, by detecting an internal recirculation zone (IRZ) in the mean flow, excluding highly-intermittent VB cases. Analysis of the mean flow shows that SNg measured within 40 mm downstream of swirler best represents the flow's swirl-strength compared with commonly used alternatives. A stable-VB first appears in the flow with 25° vane-angle, SNg=0.35. Q-criterion iso-surfaces and velocity time-series at VC footprints show a single-helix VC to prevail across all investigated vane-angles; up to 60°, SNg=0.98. Weaker double-helix signatures also appear, resulting from quadratic self-interaction of single-helix tone for vane-angles <= 50°. They are quadratically independent in 60° case, indicating association with a distinct helical hydrodynamic mode. Axisymmetric IRZ oscillations interact with helical-VC dynamics in 25° and 60° cases. VC precesses as stable limit-cycle oscillation via a marginally stable mode in 40° to 50° cases, while it waxes and wanes strongly in 25° and 60° cases driven by stochastic forcing of a slightly stable mode. Alongside the coherent VC-strand, a weakly-coherent strand originates from swirler. Its precession frequency matches with the lowest coherent precession frequency, corroborating its precession-based origin. Overall, we establish critical-values, evaluation locations and a topology-map for predicting and interpreting VB-states in isothermal swirl combustor flows.

physics.flu-dyn

Effect of particle-momentum on an isothermal flow-field inside a swirl combustor

This paper investigates the impact of particles on isothermal flow inside a lab-scale swirl combustor for a fixed inlet swirl number of 0.67 using steady-state CFD simulations. The combustor geometry and baseline conditions, with no particles, are taken from Taamallah et al. [1], but with a simplification. In the present work, we provide rotation to the flow using velocity boundary condition, whereas in [1], a swirler is built into the geometry to achieve the same effect. Shear stress transport (SST) k-omega model, an eddy-viscosity based Reynolds averaged Navier-Stokes equation approach, is used for modelling turbulence. The comprehensive model is validated against the experimental axial-velocity data in [1]. Two simulations, one with 75 and another with 100 micron particles using Discrete particle model (DPM) were conducted to isolate the effect of particle motion on swirl-combustor flow without combustion. Their analysis shows significant downstream shift of central recirculation zone (CRZ). An effect that can significantly impact the stabilization of coal flame in pulverized particle reactors.

physics.flu-dyn

Influence of Centre Body on the Dynamics of Isothermal Flow Swirl Combustor

This study examines the effect of centre-body geometry on the dynamics of an isothermal, non-reacting swirl combustor through computational fluid dynamics (CFD) simulations. Two different central body shapes were considered in a lab-scale combustor configuration, modelled as transient, incompressible flow using the SST k-omega turbulence model. The numerical model was validated against experimental velocity data from literature to ensure accuracy. Cross-spectral analysis techniques were employed to characterise the coherent dynamics of the flow, providing insight into the influence of geometry on unsteady swirl dynamics.

physics.flu-dyn