552 INSTRUMENTATION: WATER AND WASTEWATER ANALYSIS
across the electrodes, the radiant energy or photons cause
emission of photoelectrons. The photoelectrons are collected
at the anode giving rise to a photocurrent. The photocurrent is
proportional to the power or radiant energy of the light beam
and is independent of the applied potential (see Figure 6).
The eleven chemical compositions of various photoemissive
cathode coatings determine the wavelength range and sen-
sitivity varying from the uv to the near ir spectral regions.
The window in the tube must be transparent to wavelength
of interest. The dark current is a small current flowing when
no light falls on the cathode and is due to thermal energy and
electron emission from potassium-40,^40 K, in the glass tube.
It limits the sensitivity of the detector. Although this detector
has about one tenth the sensitivity of the photovoltaic cell,
its signal may be amplified because of its large internal elec-
trical resistance compared to the photovoltaic detector. The
photoemissive detector is used for higher intensity radiation
and lower wavelength scanning rates than used with other
detectors.
(iii) Photomultiplier tubes^20
A photomultiplier tube contains a photoemissive cathode
followed by a sequential, electron multiplying assemblage
of about nine dynodes (electrodes) as illustrated in Figure 7.
The voltage of each succeeded dynode increases by 75 to
100 volts. Photoelectrons from the photoemissive cathode are
accelerated by the voltage increase of the first dynode caus-
ing the release of several electrons for each impinging pho-
toelectron. This multiplier effect continues as the electrons
Sample
changer Samplespinner Rotation
of detector
Collimators
Detector
Diffracting
crystal
Goniometer
Phototube
Rotation
of crystal
100 kV
power supply
X-Ray tube
Phase
detector
Balance
indicator
Calibrated
attenuator
60-Hz
power
input Cooling water
30-Hz
generator
60-Hz
X-ray
unit
Synchronous
motor
Chopper
Cell
Fluorescent screen
Light collector
Dial
1800
rpm
75°
150°
0°
φ
φ
2
xs
θ 2
θ
(a)
(b)
θ
θ
Amplifier
FIGURE 5 (a) Geometry of a plane-crystal x-ray fluorescence spectrometer.
Note that the angle of the detector with respect to the beam, 2θ, is twice that of
the detector to the crystal face, θ. (Courtesy of Philips Electronic Instruments.)
(b) Nondispersive x-ray absorptiometer. (Courtesy of General Electric Co.)
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