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.

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Author: RPW Scott Book:Gas Chromatography
Section:GC   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

GC   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

 
 
 

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