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May 17, 2026Physics of Fluids0 citations

Stern and wake flows over submarine models based on constrained large-eddy simulation

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HDHaoxiang DongZXZuoli Xiao

Key Points

  • This research aims to examine the boundary-layer and near-wake flows over submarine models using constrained large-eddy simulations.
  • Utilized constrained large-eddy simulations (CLES) with Spalart–Allmaras and WALE models at Reynolds numbers of 1.1−1.2×10^6.
  • Performed comparisons of surface pressure, skin-friction coefficients, and boundary-layer thickness with SUBOFF measurements.
  • Analyzed the effects of submarine appendages on wake behavior.
  • CLES method outperformed WALE model on low-resolution grid for boundary-layer characteristics.
  • Stern boundary layer showed a double-peak structure in turbulent kinetic energy and enhanced turbulence due to fins.
  • AFF-1 demonstrated self-similar behavior in velocity deficit while AFF-8's self-similarity was delayed but approached a quasi-stable state downstream.

Abstract

The boundary-layer and near-wake flows of the Submarine Off-body Flow (SUBOFF) bare hull (AFF-1) and fully appended configuration (AFF-8), developed by the Defense Advanced Research Projects Agency (DARPA), are numerically investigated using constrained large-eddy simulations (CLES) method at length-based Reynolds numbers of 1.1−1.2×106. In the CLES method, a Spalart–Allmaras type model is employed to constrain the near-wall mean subgrid-scale (SGS) stresses, while a wall-adapting local eddy-viscosity (WALE) model is selected as the baseline closure to mimic the SGS stresses. Comparisons are made for surface pressure, skin-friction coefficients and boundary-layer thicknesses with SUBOFF measurements and high-resolution simulations. Generally, the CLES method outperforms the WALE model on the same low-resolution grid. The present results manifest that a weakly favorable-pressure-gradient zone upstream of the stern is followed by a strong adverse-pressure-gradient region, in which the boundary layer thickens rapidly while remaining attached, and the stern boundary layer develops an inner-outer double-peak structure in turbulent kinetic energy (TKE). The existence of fins enhances outer-layer turbulence and introduces strong three-dimensionality, providing an upstream origin for the bimodal distribution of TKE observed in the appended wake. In the wake of AFF-1, the velocity deficit exhibits classical self-similar behavior. For AFF-8, the appendages mainly broaden the wake and redistribute outer-layer momentum, so that the decay of centerline velocity deficit remains broadly comparable to that of AFF-1, whereas the establishment of self-similarity is clearly delayed. Further analysis shows that the second-order wake statistics of AFF-8 gradually approach a quasi-stable self-similar state farther downstream.

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Cite This Study

Dong et al. (2026) studied this question.

synapsesocial.com/papers/6a095b3f7880e6d24efe109chttps://doi.org/10.1063/5.0328076
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