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Wärmeübergang beim Sieden reiner Stoffe in erzwungener Strömung

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Wärmeübergang beim Kondensieren und beim Sieden

Part of the book series: Wärme- und Stoffübertragung ((WÄRME))

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Zusammenfassung

Während der Wärmeübergang beim Sieden einer Flüssigkeit in freier Strömung im wesentlichen durch die Differenz zwischen Heizflächen- und Siedetemperatur, die Eigenschaften der Flüssigkeit und die der Heizfläche bestimmt wird, spielen beim Sieden in erzwungener Strömung noch zusätzlich die Strömungsgeschwindigkeiten von dampfförmiger und flüssiger Phase und die Art der Phasenverteilung eine Rolle. Wie bereits in Kap. 9 dargelegt, ist der Wärmeübergangskoeffizient nicht mehr durch einfache empirische Korrelation der Form α = cq n darstellbar, sondern es kommen als weitere Einflußgrößen die Massenstromdichte \( \dot m \) und der Strömungsdampfgehalt x* hinzu, so daß empirische Wärmeübergangsbeziehungen von der Form α = cq n \( \dot m \) s f (x * ) sind. Die Art solcher Beziehung wird wesentlich durch die Strömungsform bestimmt, über die im folgenden Kapitel berichtet wird.

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  1. Institut für Technische Thermodynamik und Thermische Verfahrenstechnik, Universität Stuttgart, Pfaffenwaldring 9, 7000, Stuttgart 80, Deutschland

    Prof. Dr.-Ing. Karl Stephan

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© 1988 Springer-Verlag Berlin Heidelberg

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Stephan, K. (1988). Wärmeübergang beim Sieden reiner Stoffe in erzwungener Strömung. In: Wärmeübergang beim Kondensieren und beim Sieden. Wärme- und Stoffübertragung. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-83159-1_13

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  • DOI: https://doi.org/10.1007/978-3-642-83159-1_13

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  • Online ISBN: 978-3-642-83159-1

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