Teledyne Computer Monitor 651 ユーザーズマニュアル

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07506C DCN6727 
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C H A P T E R   6
 
T e c h n i c a l   D e s c r i p t i o n  
The Model 651 is a continuous-flow, water-based, condensation 
particle counter that detects particles down to <7 nm at a sample 
flow rate of 0.12 L/min. This section describes the function of the 
particle counter, its subsystems and its components. A discussion 
of operation theory is given first. 
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 (self-nucleation), 
supersaturation is so high that condensation can take place even if 
no particles are present because molecules of the vapor form 
clusters (nucleation sites) due to the natural motion of the gas and 
attractive van der Waals forces. The Model 651 operates below the 
supersaturation ratio to avoid homogeneous nucleation. 
 
The degree of supersaturation is measured as a saturation ratio 
(P/P
s
), which is defined as the actual vapor partial-pressure divided 
by the saturation vapor pressure for a given temperature: 
 
 
P 
supersaturation =__ 
 
P
s
 
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  
(4
 M
saturation ratio =__ = exp _____ 
 
P
s
  
RTd