Hostname: page-component-848d4c4894-x5gtn Total loading time: 0 Render date: 2024-04-30T13:34:20.458Z Has data issue: false hasContentIssue false

Natural ventilation in interconnected chambers

Published online by Cambridge University Press:  15 September 2006

M. R. FLYNN
Affiliation:
Department of Mechanical and Aerospace Engineering, Jacobs School of Engineering, University of California, San Diego, 9500 Gilman Drive, La Jolla, CA 92093-0411, USA
C. P. CAULFIELD
Affiliation:
BP Institute, University of Cambridge, Madingley Rise, Madingley Road, Cambridge, CB3 0EZ, UK Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, UK

Abstract

Ventilation of adjacent, connected chambers, forced in one chamber by an isolated point source of buoyancy is investigated. There are floor- and ceiling-level external openings in the forced and unforced chambers, respectively, while the partition between the chambers has both a floor- and ceiling-level opening. The flow evolves on the time scale over which the volume flux associated with the plume at the ceiling would fill both chambers. The steady state in the forced chamber is analogous to the single chamber flow described by Linden, Lane-Serff & Smeed (J. Fluid Mech., vol. 212, 1990, p. 309), with a well-mixed buoyant upper layer which is deeper than in the single chamber flow due to the extra pressure drop at the upper interior opening. The steady state in the unforced chamber inevitably exhibits vertical stratification, and depends on the transient flow, all the opening areas, and the relative plan area of the two chambers, as is verified by laboratory experiments. When the upper interior opening is relatively large, the buoyant layer in the unforced chamber is deeper than the buoyant layer in the forced chamber, which contradicts model predictions based on the assumption that the layers are always well-mixed.

Type
Papers
Copyright
© 2006 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)