1977
DOI: 10.1175/1520-0493(1977)105<0334:teoawd>2.0.co;2
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The Energetics of African Wave Disturbances as observed During Phase III of GATE

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Cited by 166 publications
(134 citation statements)
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“…Because AEWs north of the AEJ derive the majority of their energy from baroclinic processes associated with the interaction of the low-level meridional temperature gradients in the Sahel−Sahara region and the potential vorticity gradients in the AEJ core, the energetics of AEWs should in part reflect the local changes to surface air temperature that occur in response to enhanced radiative forcing. Stronger gradients in potential temperature result in greater zonal available potential energy for AEW growth (17,24,30). AEWs access this source of zonal available potential energy by fluxing temperature down the meridional temperature gradient, creating eddy available potential energy.…”
Section: Resultsmentioning
confidence: 99%
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“…Because AEWs north of the AEJ derive the majority of their energy from baroclinic processes associated with the interaction of the low-level meridional temperature gradients in the Sahel−Sahara region and the potential vorticity gradients in the AEJ core, the energetics of AEWs should in part reflect the local changes to surface air temperature that occur in response to enhanced radiative forcing. Stronger gradients in potential temperature result in greater zonal available potential energy for AEW growth (17,24,30). AEWs access this source of zonal available potential energy by fluxing temperature down the meridional temperature gradient, creating eddy available potential energy.…”
Section: Resultsmentioning
confidence: 99%
“…AEWs then grow by converting the eddy available potential energy to eddy kinetic energy through baroclinic overturning. To enable sustained AEW growth, the eddy available potential energy must be replenished by the zonal available potential energy (17,30).…”
Section: Resultsmentioning
confidence: 99%
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“…The fluxes double in magnitude in association with the considerably stronger mid-tropospheric meridional PV gradient as a result of moist convection (Figure 11). The spatial distribution of the vertical heat fluxes below the moist AEJ (not shown) exhibits a minimum located towards 17 • N and an additional maximum compared with the dry life cycle which is located around 10 • N. This is associated with a negative baroclinic conversion probably linked to the overturning associated with evaporative cooling in convective downdraughts, as hypothesized by Norquist et al (1977) in their energetics analysis of GATE data, as observed between 800 and 600 mb by Diedhiou et al (2002), and in a regional modelling study by Hseih and Cook (2007). The minimum at 17 • N is in the right sense for baroclinic growth, and the weak low-level amplitudes in the moist model were closely correlated to increases in this minimum.…”
Section: The Moist Life Cyclementioning
confidence: 90%
“…These conversion terms represent the diabatic conversion of latent heat energy and the baroclinic conversion of mean state available potential energy (APE), respectively, to eddy APE. The terms are defined by the following formulas (Norquist et al 1977): …”
Section: E Energy Conversion Calculationsmentioning
confidence: 99%