
C H A P T E R 6
Technical Description
The Model 651 is a
T h e o r y
The Model 651 acts very much like an optical particle counter. However, the particles are first enlarged by a condensing vapor to form easily detectable droplets. Portions of the following discussion (focusing on how to condense the vapor onto the particles) are taken from a paper by Keady, et al. [1986].
In heterogeneous condensation, the vapor surrounding particles reaches a certain degree of supersaturation and begins to condense onto the particles. In homogeneous nucleation
The degree of supersaturation is measured as a saturation ratio
(P/Ps), which is defined as the actual vapor
P supersaturation =__ Ps
For a given saturation ratio, the vapor can condense onto particles only if they are large enough. The minimum particle size capable of acting as a condensation nucleus is called the Kelvin diameter and is evaluated from the following relationship:
P | (4γ M) |
saturation ratio =__ = exp _____ | |
Ps | ρRTd |
07506C DCN6727 | 53 |