560 INSTRUMENTATION: WATER AND WASTEWATER ANALYSIS
relaxation emit fluorescence emission. The wavelengths in the
fluorescence emission are unique for different elements. This
information may be delineated by wavelength or energy dis-
persion instruments (see Figure 4C). Wavelength dispersion
is carried out with a crystal as a diffraction grating with sub-
sequent detection by a gasfilled detector (see Figure 5), while
energy dispersion may be accomplished by a lithium-drifted
silicon detector and energy-discriminative electronic circuits
(see Figure 16). Non-dispersive instruments use filters.
Elements with atomic numbers greater than 7
(oxygen 8) fluoresce on irradiation with x-rays. Useful
irradiating wavelengths extend from 0.5 to 2.5 Å. Due to
the large absorption of wavelengths greater than 2.5 Å by
air and spectrometer windows, elements of atomic numbers
below 22 (titanium) cannot be detected. Elements with lower
atomic numbers can be detected with a change of atmo-
sphere; down to aluminium (atomic no. 13) in helium and
to boron (atomic no. 5) in a vacuum.
(9) Nephelometric & turbidimetric devices^36
The presence of turbidity, suspended matter and col-
loids, in liquid results in the scattering of a beam of incident
light passing through the liquid. The scattering process is
elastic; the wavelength of incident and scattered light is the
same. Particle shape and size distribution, size relative to the
wavelength of the incident light, concentration of particles,
and molecular absorption effect the angular distribution of
scattered light intensity. Since the scattering phenomenon is
so complicated analytical results are empirical depending on
the use of standards. However, differences in the design of
instruments leads to different values for the same standard.
Turbidimetry refers to the measure of the decrease in the
intensity of a beam of light undergoing scatter by suspended
or colloidal particles in a liquid. If the transmittance is less
than 90%, this method is effective. A filter photometer illus-
trated in Figure 9 is a suitable instrument.
If the intensity of the scattered beam is measured at
an angle to the transmitted beam, then the phenomenon is
known as nephelometry. Right angle scatter is commonly
used for a number of readings, although forward scatter
is more sensitive to large particles. Stray light caused by
scratches, dirt or condensation on cell walls leads to a positive
error. Figure 14, a simple fluorometer, measuring scattered
light at 90 can be employed for nephelometric measure-
ments. A surface scatter instrument shown in Figure 17 is
used to eliminate stray light. No cell is employed since the
flowing water sample surface is directly illuminated with the
light beam. Figure 18 illustrates a low range turbidimeter.
Electron
column
Si(Li)
detector
Electrons
Sample
X-rays
Preamp
Pulse
processor
Energy-to-
digital
converter
Video
Keyboard
Multi-
channel
analyzer
Disk
storage
system
Mini-
computer
FIGURE 16 Components of a typical energy-dispersive microanalysis system. The Si(Li) detector is cooled in
a liquid nitrogen cryostat. The charge pulse from the Si(Li) detector is converted in the preamp to a step on a volt-
age ramp. The pulse processor converts the signal to a well-shaped voltage pulse with an amplitude proportional
to the energy of the x-ray. (Courtesy of the Kevex Instruments, Inc.)
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