NUCLEATION LABORATORY

 

 

 

THE IMPACT OF CONVECTIVE FLOW ON THERMAL DIFFUSION CLOUD CHAMBER OPERATION

 

accepted for publication in J. Phys. Chem. 2001

F.T. Ferguson and R.H. Heist

 

RESEARCH SUMMARY

     We report in this paper new results that further elucidate the role of buoyancy-driven convective flows in determining the distribution of vapor mole fraction and temperature in the thermal diffusion cloud chamber.  A two-dimensional model describing both diffusion and convection in the presence of chamber sidewalls is presented.  The model equations are use to analyze 1-butanol and 1-pentanol nucleation data obtained earlier.  The results of the investigation are summarized in the figures shown below.  These results show that convective flow is nearly always present and, in the cases considered here, result in a reduction in the value of the calculated critical supersaturation (as compared to the one-dimensional case).  The dependence of critical supersaturation with total pressure reported earlier is smaller but is not eliminated.

 

Variation of critical supersaturation of 1-pentanol in helium with total pressure for the 1-D analysis (solid symbols) and the 2-D analysis (open symbols).  The solid lines are regression fits to the linear portions of the data sets and are included to emphasize trends in the data.  Nucleation temperatures:  diamonds - 356K; squares - 366K; triangles - 377K.  Variation of critical supersaturation of 1-butanol in helium with total pressure for the 1-D analysis (solid symbols) and the 2-D analysis (open symbols).  The solid lines are regression fits to the linear portions of the data sets and are included to emphasize trends in the data.  Nucleation temperatures:  diamonds - 334K; squares - 348K; triangles - 363K.

 

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