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Frans_M_Everaerts_Isotachophoresis_378342.pdf

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W ABSORPTION METER<br />

230 240 2% m zm 280 EC GO 30 m 330<br />

wovelength (nm)<br />

Fig.6.27. Optical filters used for the UV absorption measurements on the various zones. A combina-<br />

tion of an interference filter and an end filter (coloured glass filter) was always used. From this figure,<br />

an estimation of the band width can be made for the experiments included in this book.<br />

impedance, the circuit must be surrounded with a metal frame in order to prevent<br />

disturbances. Special care must be taken in selecting the 104-Ma resistor, which is<br />

basically responsible for a bad signal-to-noise ratio and drift.<br />

In the PTFE narrow-bore tube (I.D. 0.45 mm, O.D. 0.75 mm), in combination with<br />

a slit width of 0.3 mm*, the difference in signal (uv) between dark and light is approxi-<br />

mately 100 mV, which is the normal value if a non-absorbing component is inside the<br />

narrow-bore tube with water as the solvent and the combination of interference filter<br />

and coloured glass filter (end filter) is chosen, as shown in Fig.6.27. This value of 100 mV<br />

is chosen arbitrarily and depends mainly on the sensitivity of the potential recorders<br />

available.<br />

6.5.4. UV detector in combination with a modulated UV source<br />

In the UV detector, the alternating current, due to the alternating influx of W<br />

quanta, in the phototube is changed to an alternating voltage, which is then detected<br />

synchronously.<br />

*Later experiments learn that with a slit of 0.1 mm and a narrow-bore tube (I.D. 0.2 mm, O.D.<br />

0.4 mm), sharper boundaries could be detected between the various zones.<br />

161

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