DOI: 10.1017/jfm.2026.11896 ISSN: 0022-1120
Energy dissipation mechanisms in an acoustically driven slit
Haocheng Yu, Tianyi Chu, Spencer H. Bryngelson
We quantify the conversion of incident acoustic energy into vortical motion and viscous dissipation for a plane wave passing through large-aspect-ratio slit geometries. We perform direct numerical simulations over a broad imposed parameter space in incident sound pressure level (ISPL), Strouhal number (
italic St
St
$\textit{St}$
) and Reynolds number (
italic Re
Re
$\textit{Re}$
). Spectral proper orthogonal decomposition yields energy-ranked coherent structures at each frequency, from which we construct mode-by-mode fields for spectral kinetic energy (KE) and viscous loss (VL) to examine the acoustic absorption mechanisms. At
italic ISPL equals 150 dB
ISPL
=
150
dB
$\textit{ISPL} = {150}\,\textrm{dB}$
, the acoustic–hydrodynamic energy conversion is highest when
italic St less than or equals 4 italic St Subscript 0 Baseline
St
≤
4
St
0
$\textit{St} \le 4\textit{St}_0$
, corresponding to an effective Keulegan–Carpenter number (
upper K Subscript c
K
c
${K_c}$
) larger than 40. In this regime, three-dimensional simulations show that the dominant flow response is two-dimensional, with the oscillatory shear layer near the slit corners rolling up into shedding vortices. The VL accounts for 20 %–60 % of the KE contribution. For larger
italic St
St
$\textit{St}$
, the Stokes-layer confinement produces X-shaped near-slit modes, reducing the energy input by approximately 50 %. The influence of
italic Re
Re
$\textit{Re}$
depends on amplitude. Larger
italic Re
Re
$\textit{Re}$
corresponds to suppressed broadband fluctuations and sharpened harmonic peaks at
150 dB
150
dB
${150}\,\textrm{dB}$
. At
italic ISPL equals 120 dB
ISPL
=
120
dB
$\textit{ISPL} = {120}\,\textrm{dB}$
, the boundary layers remain attached, vortex shedding is weak, absorption monotonically scales with viscosity and the
italic Re
Re
$\textit{Re}$
- and
italic St
St
$\textit{St}$
-dependencies become comparable. Across all conditions, more than 99 % of the VL is confined to a compact region surrounding the slit mouth. The KE–VL spectra identify regimes that enhance or suppress acoustic damping in slit geometries, providing a physically interpretable basis for acoustic-based design.