(32) Sound-hard boundary conditions thus correspond to imposing homogeneous Neumann boundary con- ditions on S(⃗ x) and ∂⃗ ν∆S(⃗ x) = − u2 u1 ∂⃗ ν ⃗ n· HS⃗ n

Sound-hard boundary conditions also change since the normal component of the fluid velocity⃗ ν· ⃗ vnow satisfies the equation −iωρ0(⃗ v· ⃗ ν) = c2 0∂⃗ νS(⃗ x) − ρ2 0u1∂⃗ ν∆S(⃗ x) (

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it

browse 1 citing papers

representative citing papers

Time-harmonic waves in Korteweg and nematic-Korteweg fluids

math-ph · 2024-11-20 · reject · novelty 5.0

The authors derive Helmholtz-Korteweg and nematic Helmholtz-Korteweg equations and study plane waves, evanescent waves, reflection, and scattering, but the penetration depth formula is wrong.

citing papers explorer

Showing 1 of 1 citing paper.

Time-harmonic waves in Korteweg and nematic-Korteweg fluids math-ph · 2024-11-20 · reject · none · ref 6
The authors derive Helmholtz-Korteweg and nematic Helmholtz-Korteweg equations and study plane waves, evanescent waves, reflection, and scattering, but the penetration depth formula is wrong.

(32) Sound-hard boundary conditions thus correspond to imposing homogeneous Neumann boundary con- ditions on S(⃗ x) and ∂⃗ ν∆S(⃗ x) = − u2 u1 ∂⃗ ν ⃗ n· HS⃗ n

fields

years

verdicts

representative citing papers

citing papers explorer