2003
DOI: 10.1017/s002211200300586x
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Force on a body in a continuously stratified fluid. Part 2. Sphere

Abstract: In this paper the experimental study presented in Part 1 is extended to the three-dimensional case. The in-line force coefficients (added mass and damping) of a sphere oscillating horizontally in a uniformly stratified fluid of limited depth and in a smooth pycnocline are evaluated from Fourier-transforms of the experimental records of impulse response functions. The hydrodynamic loads in the three- and two-dimensional cases are shown to be essentially different, notably in the low-frequency limit, where the d… Show more

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Cited by 17 publications
(22 citation statements)
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References 21 publications
(35 reference statements)
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“…the virtual mass tends to zero m 0 ≈ 0. This agrees qualitatively with the results [16] for a sphere with a forced oscillation frequency close to the buoyancy frequency.…”
Section: Resultssupporting
confidence: 91%
See 1 more Smart Citation
“…the virtual mass tends to zero m 0 ≈ 0. This agrees qualitatively with the results [16] for a sphere with a forced oscillation frequency close to the buoyancy frequency.…”
Section: Resultssupporting
confidence: 91%
“…Although the values of the oscillation period calculated with account for the dependence of the virtual mass on the oscillation frequency in a continuously stratified fluid lie closer to the values observed, the difference is still noticeable [16]. Since in this case the oscillation frequencies are greater than the buoyancy frequency, the virtual mass must be negative.…”
Section: Resultssupporting
confidence: 60%
“…The qualitative conclusions [10] concerning the proportionality of the damping coefficient to the square of the thickness for a relatively thin pycnocline is confirmed for the low-frequency limit of the damping coefficient. This is attributable to the analogy with the blocking effect in the slow horizontal motion of plane bodies.…”
Section: Numerical Resultsmentioning
confidence: 67%
“…Voisin (2007) showed theoretically that, when N is fixed and Ω varies from 0 to its upper bound N, the power of the waves radiated by an oscillating sphere is maximum for Ω/N ≃ 0.84 (and for ≃ 0.82 for an oscillating cylinder). These results have been verified experimentally (Ermanyuk & Gavrilov (2003)). Interestingly, when a mixed region is released at its equilibrium level (Wu (1969)) or above it (Cerasoli (1978)), in a constant N stratified fluid, the power spectrum of the radiated waves is peaked at a frequency Ω such that Ω/N ≃ 0.8 as well.…”
Section: Introductionmentioning
confidence: 53%