Ash-Monitor

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RGI software

Regardless of whether for the configuration of measurement systems or for the evaluation of measurement data or for the maintenance of components: the software from RGI is designed directly for the respective application.

Product specification

Software for the continuous determination of ash content in coal

Description

This software is part of a complete measuring system for determining and calculating the ash content in coal consisting of two measuring lines, each with a radiation source, the associated detectors and an industrial PC with the ASH-MONITOR software



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Meeasuring principle

Electromagnetic  waves such as X-rays or gamma rays are absorbed in the material in different ways.

Therefore  it depends on the energy of the radiation and the material itself how it is absorbed.

High  energy waves and low atomic numbers are absorbed according to the density (or bulk density) of the material.

Of  course, the absorption also depends on the layer thickness, which means that the absorption depends on the weight of the material through which the radiation has passed (the weight increases as the path becomes longer or as the density increases).

RGI

Measuring principle

Density  and thickness can be measured using radiation: if one is constant, the other can be calculated.

Lower  energy radiation and higher atomic numbers are absorbed in the same way, but additionally according to the atomic weight: the higher the atomic weight and the lower the energy, the higher the absorption.

For  analysis purposes, a weak energy is required to determine the atomic composition.

But  since the weight also influences the damping. Higher-energy radiation must also be applied in order to obtain a signal that is only influenced by the weight, but not by the atomic composition.

Both  signals can be used mathematically to determine the composition.

Usage

A  cesium-137 radiation source is a relatively high energy emitter that is high enough to be independent of the composition and low enough to handle it safely.

It  makes it possible to determine the weight of the material that it has passed through with great precision, as is the case, for example, with radiometric belt scales.

Another  radiation-emitting material with lower energy is Americium-241: even a steel sheet with a thickness of just 0.8 mm weakens the intensity in half.

In  coal, the part called ash absorbs the radiation of the Am-241 much more than the carbon.

A  higher ash content therefore leads to a relatively strong increase in absorption.

Unfortunately, i n practice there is no way that this absorption is not influenced by the density or layer thickness, e.g. B. by loading a conveyor belt.

Both  signals are therefore required together to mathematically calculate the ash content.

Technique

To  measure the radiation, it has to be absorbed, wher the denser the absorber material is, the higher is the absorption.

Gas  filled ionization chambers or Geiger tubes are available as well known detectors, but the most sensitive is a NaJ crystal with a density of 3.7 g / cm3, which produces small flashes of light when exposed to radiation that must be detected by a light amplifier called a photomultiplier.

The  entire sensor must be installed in a mechanical protective and light-tight housing and stabilized against interference.

Both  radiation sources must be shielded in lead containers so that the rays cannot travel in all directions, so a thin channel ensures that the working jet can only exit in one direction.

The source and the detector build together the measurement path, where two measurement paths are required to determine the ash content, for what it would be possible to use only one detector for both radiations, but since each radiation physically influences the other in the detector, it is more reliable to use separate ones.

Either  the source or the detector can be installed above or below the belt, while the measuring paths should be at least 1 m apart and a solid mechanical frame is required to prevent changes in the distance between the source and detector: it must be absolutely constant to avoid measurement errors.

Evaluation

A program that uses only advanced math does not help the user: it must be applicable.

The  ash analyzer must be able to be calibrated without an extended mathematical background.

For  this purpose, a table is saved in the evaluation unit, in which laboratory values ​​can be stored and used as a comparison.

An  automatic routine for determining the calibration curve determines the coefficients and immediately shows how good the adjustment was.

It  is not only important to simply display the measurement results. The table already mentioned can be used as a data store. All measured values ​​are displayed over a period of 1 hour, 1 shift and 1 day back for 30 days.

In  the service menu, the software can change the assignment of the wiring terminals so that a relay or an analog output can be switched from one terminal to another.

Therefore,  the evaluation unit is not only an indicator for ash, but also fits into the process and can help with the control.

Accuracy

Some  influences are responsible for possible errors and good or bad accuracy.

Extracted hard coal or brown coal can usually be determined with an accuracy of better than ± 0.5% standard error for about 10% ash.

For  ash contents below 10%, even better results are achieved, while with higher ash contents - however not because of the principle but because of the higher error of the laboratories - the error is higher.

The  system must be calibrated with a laboratory error of 0.3% and is therefore of limited accuracy.

The  most important possible error is caused by the coal itself: while the measuring principle is based on the distinction between two components, in reality there are about ten, i.e. any change in the composition of the ash causes a minor error.

Since  the two main components have almost the same absorption coefficient, this ratio does not lead to a false indication, which is why attention must be paid to such changes as the iron content.

The  theoretical error can be very large, but is not very important in practice. Nevertheless, it must be observed, where another mistake can be caused by the moisture content.

Only  if the ash content is approx. 5 - 10% will no error be caused since water is measured as coal, but higher content can lead to an error, which, fortunately, can be compensated for with an RGI microwave moisture meter. 

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