Teledyne 460L User Manual

Page of 92
 
TELEDYNE INSTRUMENTS
 
460L Instruction Manual 
Theory of Operation 
05228 Rev B 
53 
DCN 5164 
PRINTED DOCUMENTS ARE UNCONTROLLED 
beam is only required to make pass through the Absorption Tube.  Therefore no complex mirror 
system is needed to lengthen the effective path by bouncing the beam back and forth. 
Finally, the UV then passes through a similar window at the other end of the Absorption Tube and 
is detected by a specially designed vacuum diode that only detects radiation at or very near a 
wavelength of 254nm.  The specificity of the detector is high enough that no extra optical filtering 
of the UV light is needed.   
The detector reacts to the UV light  and outputs a voltage that varies in direct relationship with 
the light’s intensity.  This voltage is digitized and sent to the instrument’s CPU to be used in 
computing the concentration of O
3
 in the absorption tube. 
 
UV 
Source 
ABSORPTION TUBE 
UV Detector 
Sample Gas IN 
Sample Gas OUT 
Window 
Window 
Absorption Path Length = 16 cm 
 
Figure 10-1  O
3
 Absorption Path 
 
10.1.3. The Reference / Measurement Cycle 
In order to solve the Beer-Lambert equation it is necessary to know the intensity of the light 
passing through the absorption path both when O
3
 is present and when it is not.  The Model 460L 
accomplishes this by alternately passing the sample gas through a chemical scrubber that 
removes any O
3
 present and sending it directly to the absorption tube.  
                      
ABSORPTION TUBE 
Particulate 
Filter 
From Sample 
Port 
PUMP 
O
3
  
Scrubber 
Reference/ 
Measure 
Valve 
To Exhaust 
Port 
Valve switches 
every 3 seconds 
Measure Path 
(I
Reference Path
  
(I
0
 
 Figure 10-2 Reference / Measurement Gas Cycle