1951
DOI: 10.1007/bf02246793
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Grundlagen einer Theorie der tropischen Zyklonen

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Cited by 107 publications
(55 citation statements)
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“…As proposed by Kleinschmidt (1951) and Riehl (1954), latent and sensible heat fluxes from the sea surface are crucial to TC genesis and intensification. Decades of numerical simulations have verified the fundamental role of surface fluxes (Ooyama, 1969;Rotunno and Emanuel, 1987; Nguyen et al, 2008).…”
Section: Theorymentioning
confidence: 92%
“…As proposed by Kleinschmidt (1951) and Riehl (1954), latent and sensible heat fluxes from the sea surface are crucial to TC genesis and intensification. Decades of numerical simulations have verified the fundamental role of surface fluxes (Ooyama, 1969;Rotunno and Emanuel, 1987; Nguyen et al, 2008).…”
Section: Theorymentioning
confidence: 92%
“…Although the evaporation of water from the underlying ocean has been long recognised as the ultimate energy source for tropical cyclones (Kleinschmidt 1951;Riehl 1954;Malkus and Riehl 1960;Ooyama 1969), 15 Emanuel's contributions with colleagues re-focused attention on the airsea interaction aspects of the intensification process. Rather than viewing latent heat release in deep convective towers as the 'driving mechanism' for vortex amplification, this body of work showed that certain aspects of these storms could be understood in terms of a simple time-dependent model in which the latent heat release was implicit.…”
Section: A Steady-state Hurricane Modelmentioning
confidence: 99%
“…To the best of this author's knowledge, this is the first paper in which it is explicitly recognized that the energy source of hurricanes arises from the in situ evaporation of ocean water 1 . By the next year, another German scientist, Ernst Kleinschmidt, could take it for granted that "the heat removed from the sea by the storm is the basic energy source of the typhoon" (Kleinschmidt, 1951). Kleinschmidt also showed that thermal wind balance in a hurricane-like vortex, coupled with assumed moist adiabatic lapse rates on angular momentum surfaces, implies a particular shape of such surfaces.…”
Section: Energeticsmentioning
confidence: 99%
“…The expression (16) was derived on quite different grounds by Kleinschmidt (1951) and later by Emanuel (1986). They assumed hydrostatic and gradient wind balance from the start, and simply integrated the thermal wind equation upward along angular momentum surfaces assuming that the saturation entropy, * s , is constant on angular momentum surfaces.…”
Section: Energeticsmentioning
confidence: 99%