
Device description and operating principle
Operating principle
Light sources The light sources used are a halogen lamp for the VIS and infrared
region and a deuterium lamp for the UV region.
The lamp-selector slider serves to couple the light of either the
halogen or the deuterium lamp, or the light of both lamps
simultaneously into the optical path.
In measurement breaks, lamp radiation is shut off by shutters. That
way, it is possible to perform dark-current measurements and
protect the sample from unnecessary radiation exposure.
Sample
compartment
The optical setup with polychromator allows an open sample
compartment. The bundle of rays is restricted by optical slits to the
lamp compartment and the polychromator side each. The
accessory units are clamped to the carrier rails of the sample
compartment.
Polychromator The polychromator used is the patented MCS module (Multi
Channel System) from Carl Zeiss. The entrance slit, the imaging
holographic grating and the detector are embedded in a ceramic
housing.
4.2 Operating principle
The undispersed light of the halogen and/or the deuterium lamp transmits the sample
and is partly absorbed by the sample. The thus altered light is spectrally dispersed in the
polychromator by the holographic grating. The produced spectrum is imaged onto the
diode array. The measured values of the individual photodiodes thus represent the value
of intensity Iover a small spectral region. As this is done in a very fast process, this type
of measurement is called simultaneous.
However, reading the individual photodiodes takes a certain time (integration time). This
integration time can be varied within predefined limits. The shortest integration time
possible depends, inter alia, on the number of photodiodes per line. A compromise has
to be made in selecting the most favorable integration time. A smaller integration time
means, that there is less time for the photodiode to capture the light to be measured. The
level of the measured signal will be lower and thus the signal-to-noise ratio deteriorate.
On the other hand, a too high integration time may result in an intensity that exceeds the
level the photodiode can receive (degree of saturation). The corresponding sections of
the diode array are overdriven and the found transmission or absorbance values are
wrong. However, a high integration time may be quite desirable if measurements shall be
taken in low-energy regions of the spectrum (e.g. 900 – 1020 nm) and the overdriven
areas are deliberately eliminated for the analysis. The system provides software-
supported automatic search of integration times suitable for the analytical measuring
range.
In absorption measurements, the incident intensity IR (reference value) and the intensity
ISattenuated by the sample is measured at every wavelength of interest. Measurement
is in arbitrary units, as only the ratio of both values is of importance. Quantitatively, the
absorption behavior is expressed in transmission T[%] or absorption A:
However, also the dark current must be considered for result generation. The dark
current is the intensity IDof the ambient light that may enter the polychromator through
the open sample compartment including the currents on the diode array caused by
electronics. The intensity of the dark current must be subtracted from the intensities of
sample and reference. The dark current can be measured automatically or – in very
time-critical measurements – started manually. The corresponding options are to be
selected along with other measurement parameters in WinASPECT®software.
12 Issue 02/2008 SPECORD®S600
Analytik Jena AG