1971
DOI: 10.1175/1520-0469(1971)028<0604:tcombi>2.0.co;2
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The Coupling of Momentum Between Internal Gravity Waves and Mean Flow: A Numerical Study

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Cited by 42 publications
(16 citation statements)
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“…The dynamical consequences of wave-mean flow interactions have long been studied by atmospheric fluid dynamicists, for example, in the context of gravity-wave forcing of zonal winds in the equatorial stratosphere (e.g., Lindzen & Holton 1968;Jones & Houghton 1971;Holton & Lindzen 1972;Grimshaw 1975;Plumb 1977;Savaranan 1990). The results of numerous such investigations contradict the previously noted expectation that angular momentum transport by internal waves can eradicate nonuniform rotation in the radiative interior of the Sun.…”
Section: Introductionmentioning
confidence: 99%
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“…The dynamical consequences of wave-mean flow interactions have long been studied by atmospheric fluid dynamicists, for example, in the context of gravity-wave forcing of zonal winds in the equatorial stratosphere (e.g., Lindzen & Holton 1968;Jones & Houghton 1971;Holton & Lindzen 1972;Grimshaw 1975;Plumb 1977;Savaranan 1990). The results of numerous such investigations contradict the previously noted expectation that angular momentum transport by internal waves can eradicate nonuniform rotation in the radiative interior of the Sun.…”
Section: Introductionmentioning
confidence: 99%
“…We remark that one of the main differences between the present paper (and also Paper I) and most of the earlier works in atmospheric sciences (e.g., Lindzen & Holton 1968;Jones & Houghton 1971;Holton & Lindzen 1972;Plumb 1977;Savaranan 1990) is that the momentum transport arises from the radiative damping in the diffusive limit. For instance, Lindzen & Holton (1968) invoked critical layers for wave absorption, and Plumb (1977) used Newtonian radiative cooling (which is valid in an optically thin medium).…”
Section: Introductionmentioning
confidence: 99%
“…Breeding [1971] performed nonlinear simulations that predicted larger reflection and smaller transmission coefficients than expected on the basis of linear theory, particularly at small (stable) values of the minimum mean Richardson number. The coupling between an incident gravity wave and the mean flow was considered in more detail by Jones and Houghton [1971]. For a maintained incident wave forcing, Tanaka [1975] and Fritts [1978] found the criticallevel interaction and the induced unstable layers to be displaced toward the wave source with time, a consequence of the mean flow accelerations induced by the vertical divergence of the incident wave Reynolds stress near the critical level.…”
Section: Introductionmentioning
confidence: 99%
“…The waves are dissipated when they approach critical levels [Bretherton, 1966] or when they induce convective instability [Hodges, 1967], and their associated momentum is deposited into the flow [Jones and Houghton, 1971]. In the mean, this gravity wave drag forces flow into a region away from the breaking waves where it subsequently descends and warms adiabatically.…”
mentioning
confidence: 99%