Page 474 - Tandem Techniques
        P. 474
     Page 459
            a part of the plate where no sample has passed (the channel between the spots). For this reason, single
            beam and double beam instruments are available, both of which are diagrammatically depicted in
            Figure 12.1. The double beam instrument is to be preferred, and in this configuration, one sensor
            monitors the sample lane (the strip of plate along which the separation has been developed), and the
            other monitors a blank region between the lanes. The difference signal is taken as that responding solely
            to the sample. In most instruments the incident light can be chosen to have wavelengths ranging
            between 200 and 700 nm. Halogen or tungsten lamps can be used to provide light at the higher
            wavelengths, whereas for light between 200 and 400 nm, a deuterium lamp is to be preferred.
            In order to induce fluorescence, lamps with higher energy outputs are sometimes necessary, such as the
            mercury lamp, which generates most of its emission at 254 nm, and the xenon arc lamp, which
            generates light over a broader range of wavelengths, in a similar manner to the deuterium lamp, but at
            much higher intensities. Some samples may be measured with greater sensitivity by using light having a
            narrow band of wavelengths, in which case, a monochromator is introduced between the light source
            and the plate to select the appropriate wavelength. If a monochromator is employed, then either the
            tungsten or deuterium lamp are normally used as the light source.
            The sensitivity of a scanning densitometer depends on a number of factors, including the basic
            instrument design and, in particular, the quality of the optics. The plate surface is viewed by the scanner
            through a slit and the major factor affecting the overall sensitivity is the slit height to spot diameter
            ratio. Although the slit dimensions are usually selectable, as the spots along the plate will be of different
            size it is not possible to adjust the slit to an optimum size for scanning the whole of the plate.
            When measuring either the adsorbed light or the fluorescent light, the sensitivity is inversely related to
            the scan rate. It follows that the slower the scan, the greater the signal. However, carried to the extreme,
            this approach can extend the analysis time considerably. The relationship between the adsorbed light
            and the concentration of solute in the spot is
     	
