1992
DOI: 10.1575/1912/5484
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Observations of turbulence, internal waves and background flows : an inquiry into the relationships between scales of motion

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Cited by 11 publications
(3 citation statements)
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References 102 publications
(255 reference statements)
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“…Estimates of oceanic velocity, temperature, salinity, and turbulent kinetic energy (e) and thermal (X) dissipation rates are generally available. Detailed descriptions of the HRP and data processing are given by Schmitt et al [1988] and Polzin [1992, Appendix 1]. EPSONDE [Oakey, 1988] is a loosely tethered profiler used to obtain estimates of temperature, e, and X.…”
Section: Fine-scale Sampling and Backgroundmentioning
confidence: 99%
“…Estimates of oceanic velocity, temperature, salinity, and turbulent kinetic energy (e) and thermal (X) dissipation rates are generally available. Detailed descriptions of the HRP and data processing are given by Schmitt et al [1988] and Polzin [1992, Appendix 1]. EPSONDE [Oakey, 1988] is a loosely tethered profiler used to obtain estimates of temperature, e, and X.…”
Section: Fine-scale Sampling and Backgroundmentioning
confidence: 99%
“…This simple idea, however, has not stood in the light of recent micro-3 structure data. Polzin (1992) demonstrates that equally important in the scaling of K from internal wave dissipation, are the energy levels and frequency content of the internal wave field. Through out most of the ocean's volume these are well described by the Garrett and Munk model (Garrett and Munk, 1975), and the resulting diffusivities are small (-0. lcm 2 s' 1 ), in agreement with the values found away from the bottom in the present model.…”
mentioning
confidence: 96%
“…The empirical CDFtrue(Ri1true) are shown in Figure , where they are in excellent agreement with the following CDF of simple exponential distribution: CDFtrue(x,μtrue)=1ex/μ, x0, where x=Ri1, μ is the mean, and μ2 is the variance. The parameter μ is μ(4075)=0.67±0.03 for Ri1 in the depth range Dz = 40–75 and μ(75150)=1.16±0.035 for Ri1 in the range Dz = 75–150 m. The exponential distribution of Ri1 has been already utilized by Anderson [] and Polzin [] (unpublished manuscripts referred to by Pinkel and Anderson []). The behavior of (3) is similar to a probability distribution for Ri1 suggested by Pinkel and Anderson [].…”
Section: Internal Wavesmentioning
confidence: 99%