The performance of an analytical instrument is determined
by parameters like repeatability, reproducibility, stability
and accuracy. These parameters describe the instrument
behavior in certain situations. |
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Repeatability is the probability that an analytical result
remains the same for repeated measurements in a short
period of time. If measured for a long period of time, this
property is called stability. Reproducibility is the capability to
repeatedly deliver the same result for the same measuring
conditions but for different users. Finally, accuracy is the
ability to obtain the correct result. |
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For this lab report, various measurements were performed
to determine the repeatability and stability in dependence of
different measurement parameters. |
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Instrumentation |
| Excitation |
W-tube (max. 40 kV, 40 W)
glass side window |
| Detection |
prop-counter with 1100 mm2 sensitive area
900 eV energy resolution (Mn Ka)
30,000 cps maximum count rate |
| Dimensions |
size (DxWxH): 600x450x400, 30 kg |
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Analysis |
Since one of the main applications of the M1 spectrometer
is the analysis of jewelry alloys, the measurements were
performed on a series of gold alloys. |
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Working principle |
When excited by the radiation of an X-ray tube, the sample
emits characteristic radiation. This radiation is detected
by an energy-dispersive detector that delivers energyproportional
signals. For this analysis, a proportional
counter was used. The energy distribution of the detected
radiation is determined by a pulse height analysis. Special
quantification models are necessary to calculate the
concentration of different elements in the sample. The
complete instrument is controlled by a special software
package on a laptop computer that is connected to the
device via USB. |
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Results |
Stability |
The stability of the instrument was determined by repeated
measurements of pure Au over a long period of time.
variation of intensity over a period of more than 40 hours
(more than 2400 single measurements of 60 seconds
was 0.168 %. The theoretically expected value calculated
statistics is 0.164 %, i.e. only insignificantly lower. |
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Temperature dependence |
The temperature dependence of intensity over a large
temperature range is shown in Figure 1. The room
temperature changed from 23° to 35° C. The instrument
temperature, displayed on the diagram, changed from 29° to
43° C. The instrument temperature is only 8 degrees higher
than the room temperature. This shows the very low power
consumption of the device. |
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The temperature dependence of peak position is irrelevant.
Changes are smaller than 0.1 % for this wide temperature
range. However, the detector’s energy resolution is
influenced by temperature. The FWHM slightly increases
with temperature, but also only less than 0.1 % per degree. |
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Diagram showing the temperature dependence of intensity
over a large temperature range |
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Repeatability of quantification |
In order to determine repeatability, four samples were
measured 10 times for 60 seconds each. Since the
measurement results are influenced by the element
concentration, the measurements were carried out on
samples with different compositions. The delivered results
regarding repeatability are shown in Table 1. |
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Repeatability analysis results |
| Gold content |
Standard deviation for 10 measurements for |
|
Au (Wt-%) |
Au statistic error (%) |
Ag (Wt-%) |
Cu (Wt-%) |
22 karat (91.6 %) |
0.09 |
0.30 |
0.05 |
0.07 |
18 karat (75 %) |
0.05 |
0.33 |
0.08 |
0.07 |
14 karat (58.5 %) |
0.11 |
0.37 |
0.33 |
0.06 |
10 karat (41.7 %) |
0.09 |
0.50 |
0.11 |
0.10 |
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Tolerance against fluctuations in excitation intensity |
The quantification procedure also shows high tolerance
against changes in excitation conditions. In order to illustrate
this feature, the same sample was measured with the same
tube voltage but different tube currents. For every excitation
parameter, measurements were repeated five times. The
results are presented Table 2. |
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Tolerance analysis results |
| Tube current |
Average concentrations with standard
deviation |
|
Au |
Ag |
Cu |
| Given |
64.5 |
14.9 |
15.1 |
| 800 µA |
64.54 ± 0.122 |
14.94 ± 0.080 |
15.18 ± 0.040 |
| 780 µA |
64.53 ± 0.103 |
14.93 ± 0.046 |
15.19 ± 0.072 |
| 650 µA |
64.50 ± 0.078 |
15.00 ± 0.089 |
15.15 ± 0.129 |
| 500 µA |
64.64 ± 0.104 |
14.99 ± 0.127 |
15.01 ± 0.090 |
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Conclusion |
Changes in temperature, excitation intensity or other factors
have only very little influence on the repeatability and
stability of the instrument. They are lower than statistical |
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