Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 9 min ago
PreprintarXiv licencearXiv

Preferential concentration in a periodically forced particle-laden turbulent planar jet

Abstract

Periodic forcing is common in particle-laden jets, yet its influence on turbulence and inertial-particle clustering remains poorly understood. We investigate a turbulent planar jet at two Reynolds numbers, approximately 4950 and 9900 based on nozzle height, subjected to sinusoidal forcing at a frequency three orders of magnitude below the preferred jet instability. Hot-wire anemometry and high-speed particle imaging characterise the carrier turbulence, while Voronoi tessellations quantify preferential concentration of dilute inertial droplets. Despite its low frequency and moderate amplitude, forcing substantially modifies turbulence while leaving the mean-flow development nearly unchanged. The integral scale decreases by up to 40%, while forced and unforced jets retain the same time-averaged relationship between the dimensionless dissipation coefficient and Taylor-scale Reynolds number. Within the forcing cycle, velocity fluctuations and the Taylor microscale vary approximately in opposite phase, keeping the Taylor-scale Reynolds number within ±10% of its cycle mean despite substantial variations in dissipation and Kolmogorov time scale. Particle clustering is even more sensitive, with forcing increasing mean preferential concentration and producing phase-dependent variations of $21−−49\%$ of the cycle mean. Clustering peaks when the Kolmogorov time scale is largest, corresponding to the smallest particle Stokes number. Thus, markedly different clustering states occur at similar instantaneous Taylor-scale Reynolds numbers. These findings demonstrate that weak temporal modulation can control particle organisation without substantially altering the mean transporting flow.

Related

  1. Seven Limit Cycles in a Periodically Forced Three-Zone Equation
    Chaoyu Hu, Jizheng Chen
    arXivPreprintarXiv licenceFull textAnalysis & PDEsDynamical systemsarXiv
  2. Conversions between kinetic and surface energy in periodically forced multiphase turbulence
    Jonathan Vahé, Fabien Thiesset
    Physical Review FluidsPeer-reviewedCC BY 4.0Full textFluid dynamicsHAL
  3. Modelling friction and heat transfer in turbulent forced convection over porous lattices
    Aneek Chakraborty, Stefan Hickel, Davide Modesti
    arXivPreprintCC BY 4.0Full textFluid dynamicsarXiv
  4. Preferential concentration of cloud droplets: Coupled effects of phase change and gravitational settling
    Zi-Mo Liao
    arXivPreprintarXiv licenceFull textAtmospheric science & meteorologyFluid dynamicsarXiv
  5. Concentration of Stationary Measures onto Large Scales in the Fast-Advection Limit of the Stochastically Forced Two-Dimensional Navier-Stokes Equations
    Tobias Rohner
    arXivPreprintCC BY-NC-SA 4.0Full textMathematical physicsNumerical analysis & scientific computingarXiv
BibTeX
@misc{ahmad2026preferential,
  title = {{Preferential concentration in a periodically forced particle-laden turbulent planar jet}},
  author = {Mohammad Ahmad and Pierre Bragança and Christophe Cuvier and Martin Obligado},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.17353},
  eprint = {2610.17353},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.17353},
}
RIS
TY  - UNPB
TI  - Preferential concentration in a periodically forced particle-laden turbulent planar jet
AU  - Mohammad Ahmad
AU  - Pierre Bragança
AU  - Christophe Cuvier
AU  - Martin Obligado
PY  - 2026
DA  - 2026/10/12
PB  - arXiv
DO  - 10.48550/arxiv.2610.17353
UR  - https://arxiv.org/abs/2610.17353
AB  - Periodic forcing is common in particle-laden jets, yet its influence on turbulence and inertial-particle clustering remains poorly understood. We investigate a turbulent planar jet at two Reynolds numbers, approximately 4950 and 9900 based on nozzle height, subjected to sinusoidal forcing at a frequency three orders of magnitude below the preferred jet instability. Hot-wire anemometry and high-speed particle imaging characterise the carrier turbulence, while Voronoi tessellations quantify preferential concentration of dilute inertial droplets. Despite its low frequency and moderate amplitude, forcing substantially modifies turbulence while leaving the mean-flow development nearly unchanged. The integral scale decreases by up to 40%, while forced and unforced jets retain the same time-averaged relationship between the dimensionless dissipation coefficient and Taylor-scale Reynolds number. Within the forcing cycle, velocity fluctuations and the Taylor microscale vary approximately in opposite phase, keeping the Taylor-scale Reynolds number within ±10% of its cycle mean despite substantial variations in dissipation and Kolmogorov time scale. Particle clustering is even more sensitive, with forcing increasing mean preferential concentration and producing phase-dependent variations of $21−−49\%$ of the cycle mean. Clustering peaks when the Kolmogorov time scale is largest, corresponding to the smallest particle Stokes number. Thus, markedly different clustering states occur at similar instantaneous Taylor-scale Reynolds numbers. These findings demonstrate that weak temporal modulation can control particle organisation without substantially altering the mean transporting flow.
ER  -