NUCLEATION LABORATORY
TWO-DIMENSIONAL
TRANSPORT AND WALL EFFECTS
IN
THE THERMAL DIFFUSION CLOUD CHAMBER
PART II: STABILITY OF OPERATION
J.
Chem. Phys. 106 , 624 (1997)
Anne
Bertelsmann and Richard H. Heist
RESEARCH
SUMMARY
As a result of this investigation, we are now able to address the operational
stability of the vapor-gas mixture in a diffusion cloud chamber with respect to
density profile extrema and the accompanying possibility of buoyancy-driven
convective flow disturbances. We
have determined conditions for stable operation (no convective flow
disturbances) in the central portion of the cloud chamber, as well as conditions
necessary for stable operation in the vicinity of the cloud chamber wall.
We found that the total density profile in the central portion of the cloud
chamber can pass through a density minimum event though the density at the upper
plate surface is less than the density at the lower plate surface.
These local density profile inversions can result in unstable
(convective) behavior that propagates through the cloud chamber.
Furthermore, we found that local extrema in the total density profile
near the chamber wall can lead to subtle, convective flows that are difficult to
detect yet can exert a profound influence on nucleation in the central portion
of the cloud chamber.
As a further result of this study, we developed a simple method to estimate the
limiting total pressure in a cloud chamber that will support stable operation.
From results of our investigations based upon this method, it appears
that the TDCC is best suited for experiments at higher temperatures where the
accessible total pressure range is largest.
The equation that defines the upper limit for the total pressure for
which the density gradient will be stable throughout the chamber can be written
as:
All
of the terminology is defined in the original paper (cited above).
Finally, we found that results of our investigation into the effects of total pressure and kind of background gas on nucleation in diffusion cloud chambers involving the low molecular weight alcohols and hydrogen and helium background gases cannot be explained on the basis of these kind of density disturbances occurring within the diffusion cloud chamber. Also, for (relatively) low vapor pressure materials, such as 1-pentanol or other high molecular weight alcohols and alkanes, stability limitations may preclude nucleation measurements at low temperatures using a diffusion cloud chamber altogether.
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