Recorder
A recorder (originally a recording milli-ammeter), now more precisely termed a potentiometric recorder, is a device that draws the chromatogram that results from a chromatographic process onto chart paper and provides a visual representation of the separation that has been achieved. The device can have a ‘full scale deflection’ (FSD) voltage that commonly ranges from 1 mv to 10 v and which can be selected to suit the output of the detector electronics. The time scale of the chart movement normally ranges from about 1 cm per second to 1 cm per hour which can also be selected to suit the separation that is being carried out. Most modern chromatographs no longer employ recorders to present the chromatogram and the results are automatically processed by a computer and presented on the computer monitor or printed out as required.
Author: RPW Scott
Book:Gas Chromatography
Section:YES Data Scaling-Ampifier
Data Acquisition and Processing
Originally,
analytical results were calculated from measurements made directly on the
chromatogram provided by the chart recorder. This is still true for many
chromatographs in use today, but analyses obtained from contemporary instruments commonly process the results using a computer. The output
from the detector (which is only rarely the direct output from the detector
sensor) is usually in millivolts and is suitable for direct connection to a
potentiometric recorder. This output represents a voltage that is linearly
related to solute concentration being measured by the detector sensor and as
the sensor
YES Data Scaling-Ampifier
Author: RPW Scott
Book:Gas Chromatography Detectors
Section:GC-Detectors Noise Measurement
nbsp;
A combination of all three sources of noise
is shown by the trace at the bottom of figure 4. The sensitivity of the
detector should never be set above the level where the combined noise exceeds
2% of the F.S.D. (full scale deflection)
of the recorder (if one is used), or appears as morethan2%F.S.D.
of the computer simulation of the chromatogram.
Measurement of Detector Noise
Detector noise is defined as the maximum
amplitude of the combined short– and long-term noise measured over a period of
10 minutes (the E19 committee recommends a period of 15 minutes). The detector
is connected to a column and mobile phase must be passed through it during
measurement. The detector noise is obtained by constructing parallel lines embracing
GC-Detectors Noise Measurement
Author: RPW Scott
Book:Principles and Practice of Chromatography
Section:Principles Basic-Chromatograph Output
changes or variations in solvent
composition. A combination of all three sources of noise is shown by the trace
at the bottom of figure 26.
The detector
noise is defined as the maximum amplitude of the combined short– and long-term
noise measured over a period of 15 minutes. The detector must be connected to a
column and mobile phase passed through it during measurement. The detector
noise (ND) is obtained by constructing parallel lines embracing the
maximum excursions of the recorder trace over the defined time period as shown
in figure 27
Principles Basic-Chromatograph Output
Author: RPW Scott
Book:Principles and Practice of Chromatography
Section:Principles TLC
Data Acquisition and Processing System
A diagram of e
chromatographic data acquisition and processing system is shown in figure 29.
Figure 28
The Data Acquisition and Processing System
The actual
format of the data system can vary widely from manufacturer to manufacturer.
Most systems have a means for real time monitoring the detector output either
by using an ancillary recorder or by computer software, the chromatogram being
drawn by the computer on the printer. The signal from the detector is first
scaled, usually to a range from 0 to 5 volt by a suitable amplifier and the
scaled signal is then digitized by means of an A/D converter. The data is then
regularly read by the computer and stored on disk. The data may be partially
processed 'on the fly' or processed at the completion of the analysis.
Thin Layer Chromatography Apparatus
Thin layer
Principles TLC
Author: RPW Scott
Book:Extra Column Dispersion
Section:EC-Dispersion Low-Dispersion-Connecting-Tubes Serpentine-Type
found to be sufficient to achieve
complete thermal equilibrium between the column and the mobile phase.
The different
forms of dispersion profiles that are obtained from various types of connecting
tubes used in LC are shown in figure 14. The peaks shown were obtained using a
low dispersion UV detector (cell volume, 1.4 ml) in conjunction with a sample valve witha 1 mlinternal loop. The tubes had the
same length and the flow rate was 2 ml/min.; the peaks were recorded on a high
speed recorder. The serpentine tubing is seen to produce symmetrical peaks
which had the smallest width. The peak from the coiled tube, albeit quite
symmetrical, is the widest of all four peaks at the points of inflexion.
Ref (P) J. Chromatogr. 268(1978)681
Figure 14. Dispersion Profiles
from Different Types of Tube
EC-Dispersion Low-Dispersion-Connecting-Tubes Serpentine-Type
Author: RPW Scott
Book:Extra Column Dispersion
Section:EC-Dispersion Response-Time
nbsp;
The curve
shows very significant a.c. noise, which was smoothed by a 5-point smoothing
routine available in the recorder software and the smoothed curve is included
in figure 22. The smoothed curve is also shown expanded to full scale together
with the logarithm of the expanded curve. From the slope of the linear portion
of the logarithmic curve the time constant of the sensor could be calculated
and was found to be about 2.5 s. A time constant of this magnitude is
completely unacceptable for high speed liquid chromatography as a complete
separation can be achieved in a period commensurate with the time
EC-Dispersion Response-Time