English

Transitional and Near-Wall Turbulence Dynamics over Rib-Roughened Surfaces

Fluid Dynamics 2026-01-26 v2

Abstract

This study utilizes Large Eddy Simulation (LES) to investigate the impact of longitudinal triangular riblets on the laminar-to-turbulent transition in boundary layer flow. Five cases are examined: one involving a flat plate and four with ribbed plates. Among the ribbed cases, three use a riblet aspect ratio of two, whereas one has an aspect ratio of one. Arrays of longitudinal triangular riblets are positioned on a flat plate, and the transition to turbulence is initiated by controlled excitation of a Tollmien-Schlichting (TS) wave imposed on a Blasius velocity profile in a stable region. The longitudinal triangular riblets attenuate the TS wave, leading to a lower growth rate of turbulence. For higher riblet height (hh) and width (ww), with inner-scaled dimensions h+=25h^+ = 25, w+=S+=50w^+ = S^+ = 50 (where SS is the spacing between two riblets), an early transition is triggered by high-frequency disturbances generated at the leading edge of the roughness elements. However, increasing riblet spacing to S+=75S^+ = 75 delays the transition by 17.5 percent. Both cases exhibited increased drag compared to the flat plate. For h+=12.5h^+ = 12.5 and w+=S+=25w^+ = S^+ = 25, transition was delayed by 37 percent, with a modest overall drag reduction of 8.8 percent. The most significant result from the considered cases, h+=w+=S+=12.5h^+ = w^+ = S^+ = 12.5, showed a 47 percent delay in transition and a 13.69 percent reduction in overall drag. Smaller riblets cause minimal disturbance at the leading edge of roughness, resulting in a transition mechanism similar to a flat plate, while also reducing pressure loss, secondary flows, and velocity fluctuations.

Keywords

Cite

@article{arxiv.2505.12818,
  title  = {Transitional and Near-Wall Turbulence Dynamics over Rib-Roughened Surfaces},
  author = {Ranjan Kushwaha and S. Sarkar and Gautam Biswas},
  journal= {arXiv preprint arXiv:2505.12818},
  year   = {2026}
}