2.5. Included Examples¶
2.5.1. List of example projects¶
In most cases the associated literature for an example project is cited within the projects; see TAB “Procedure” after loading a project. See also Help topic “Used literature”.
All example project files can be considered as being evaluated, because they originate from associated publications, or they were confirmed by colleagues through independent intercomparison calculations.
Note
In 2023 and in 2024, all projects were checked with respect to the correct use of physical units. Only very few errors were found and corrected.
All example project files indicated by the \(\surd\) symbol in the left column can be considered as being evaluated, because they originate from associated publications, or they were confirmed by colleagues through independent intercomparison calculations.
2.5.1.1. Examples with 1 output quantity¶
without linear unfolding
ISO-Example-1a_EN.txp
|
Alpha activity concentration in liquid material: measurement with an Alpha detector; corresponds to example 1a, section D.2.1, ISO 11929:2010 |
ISO-Example-1b_EN.txp
|
Alpha activity concentration in liquid material: measurement with a rate meter; corresponds to Example 1b, Section D.2.2, ISO 11929:2010 |
ISO-Example-2a_EN.txp |
Sr-90 in soil, several determinations; corresponds to Example 2, Section D.3.1, ISO 11929:2010; DL 5 % too small |
|
simplified version of ISO-Example-2a_EN.txp |
ISO-Example-2b_EN.txp
|
Sr-90 in soil, several determinations; corresponds to Example 2, Section D.3.2, ISO 11929:2010; |
|
simplified version of ISO-Example-2b_EN.txp |
ISO-Example-3a_EN.txp
|
I-131 accumulation on air filter; corresponds to Example 3(a) section D.4, ISO 11929:2010 |
ISO-Example-3b_EN.txp
|
I-131 accumulation on air filter; corresponds to Example 3(b) section D.4, ISO 11929:2010 |
ISO-Example-4_EN.txp
|
Activity concentration with peak evaluation (Ge-Detector); corresponds to Example 4, Section D.5.1, ISO 11929:2010 |
ISO-Example-5_EN.txp
|
Peak net counting rate (NaI(Tl)-Detector); corresponds to Example 5 Section D.5.2, ISO 11929:2010 |
|
I-129 determination in soil by AMS (one value changed) |
Sterlinski-2008-NAA_EN.txp
|
Cs determination in tobacco by neutron activation analysis (en) (new example) |
ISO-Neutron-Dose_EN.txp
|
Measuring neutron dose in a mixed radiation field; replaces AKS-Neutron-Dose_EN.txp |
ISO-Photon-Dose_EN.txp
|
Measuring neutron dose in a mixed radiation field; replaces AKS-Photon-Dose_EN.txp |
Moreno-Sr90_IAEA-135_V4_EN.txp
\(\surd\)
|
Sr-90 determination by LSC in a
IAEA-135 sample
|
Alpha-IAEA-1401-Kanisch_V2_EN.txp
\(\surd\)
|
Alpha-spectrometry of Pu-238 in fish
|
vTI-Alpha-Americium_EN.txp
\(\surd\)
|
Alpha-spectrometry of Americium-241 in
fish; rather complex due to two
interferences: a) in-growing Am-241
from a Pu-241 impurity of the Pu‑242
tracer and b) Am-241 as impurity of the
solution confirmed the results
|
Gamma spectrometric determination of
\(\surd\)
|
Ra-226 (186 keV line) with subtraction
of a U-235 contribution (interference);
a corresponding Excel solution
confirmed the results
|
DWD_AB-Gesamt-Aeros-Alpha1_EN.txp
|
Monitoring artificial-alpha activity
concentration in air, version 1
|
DWD_AB-Gesamt-Aeros-Alpha3_EN.txp
Gesamt-Aeros-Alpha3_EN.txp
|
Monitoring artificial-alpha activity
concentration in air, version 3
|
DWD_AB-Gesamt-Aeros-Beta1_EN.txp
|
Monitoring artificial-beta activity
concentration in air, version 1
|
DWD_AB-Gesamt-Aeros-Beta3_EN.txp
|
Monitoring artificial-beta activity
concentration in air, version 3
|
Gamma-Dist_EN.txp
|
Application of the (N+1) rule for the
case of very low count numbers of gross
and background counting rates
|
Lira-GammaDist_EN.txp
|
Application of the (N+1) rule for the
case of very low count numbers of gross
and background counting rates;
example from Lira & Grientschnig,
2010
|
Fe-55-with-LSC-and-standard-addition_EN.TXP
\(\surd\)
|
LSC measurement of Fe-55 using the
method of standard addition
The gross count rate symbol is
occurring twice in the calculation
equation, in the nominator and in the
denominator of that expression. See the
description given in the project file.
(Independently confirmed by D.
Schrammel (KIT) and Prof. Michel )
|
NLWKN_Fe-55_with_KALFIT_EN.txp
|
Fe-55 beta measurement evaluation
including a full calibration curve for
the counting efficiency
|
Example_8_with_KALFIT_EN.txp
\(\surd\)
|
Example 8 of the new (German)
Supplement 1 to DIN ISO 11929 (2014).
|
Mean-theta_EN.txp
|
Sr-90-Measurement with several
individual measurements of a reference
sample and input of its data set to the
project, which allows deriving a
parameter theta, by which mean und
uncertainty can be calculated.
|
TemperaturCurve_KALFIT_V2_EN.txp
\(\surd\)
|
Interpolation of a linear temperature
calibration curve, example from JCGM
100:2008: b(t) = y1 +y2*(t - t0)
|
BSH_total-Gamma_var1_DE.txp
|
total Gamma measurement in seawater,
version 1
|
BSH_total-Gamma_var2_DE.txp
|
total Gamma measurement in seawater,
version 2
|
Ac228_binomial_V2_EN.txp
|
Measuring a short-lived radionuclide
with long counting: binomial
distributed sample contribution to the
gross counts
|
Ra226_U235-at-186keV_EN_long.txp
\(\surd\)
|
Same as the one show above, but with
longer symbol names
|
sumEval_sum_V3_EN.txp
|
Combining 4 measurements by summation
for determining one output quantity
|
sumEval_mean_V3_EN.txp
|
Combining 4 measurements by averaging
for determining one output quantity
|
PresetCounts_EN.txp
|
Simple single channel measurement for
demonstrating the case of measurement
with pre-set counts (number of counts n
are fixed; counting duration t is
variable)
|
A set of projects
i
so11929-4_Example-6_EN.txp
through
is
o11929-4_Example-17_EN.txp
\(\surd\)
|
Projects prepared for the examples
considered in the standard ISO
11929-4:2022
|
with linear unfolding
vTI-Y90-16330_Blw_V2_EN.txp
contribution (fish sample)
|
|
vTI-Y90-16671_Blw_V2_EN.txp
|
Y-90 decay curve, including blank
contribution (fish sample)
|
vTI-Y90-16748_Blw_V2_EN.txp
|
Y-90 decay curve, including blank
contribution (fish sample)
|
Several-peaks-
nuclide-activity-V3_EN.txp
|
Activity, determined by weighted mean
from several γ-peaks of a radionuclide
|
La140_REMSPEC-4Lines-V3_DE.txp
|
Activity, determined by weighted mean
from 4 γ-lines of the radionuclide
La-140
|
Ratel_Annex1_Beispiel_EN.txp
|
Measurement of the decay curve of
Fluor-18 (half-live of 1.829 h);
example from Ratel et al., Metrologia, 2015
|
2.5.1.2. Example with more than 1 output quantity¶
without linear unfolding
Janszen-Sr-89-Sr-90_V4_EN.txp
\(\surd\)
|
Sr-89/Sr-90 determination in
soil/sediment IAEA-1401
|
J-ALUFT-Sr-89-Sr-90_V2_EN.txp
\(\surd\)
|
Sr-89/Sr-90 determination in exhaust
air
|
Galpha_beta_Rusconi_2006_V2_EN.txp
\(\surd\)
|
Total alpha- and total-beta
determination in water by LSC
measurements in two windows, with
alpha/beta discrimination
|
dwd_sr89_sr
90_TDCR_procedureV2_EN.txp
|
Determination of Beta emitters Sr-89
und Sr-90 by a TDCR-procedure, as
realised with a HIDEX LSC Counter
|
with linear unfolding
Sr89-Sr90_Schrammel_EN.txp
\(\surd\)
|
Sr-89/Sr-90 determination by LSC, with
1 energy window; simple
|
DWD-LSC-3Kanal-V2_EN.txp
\(\surd\)
|
Sr-89/Sr-90 determination by LSC, with
3 energy windows; complex
|
DWD-LSC-3Kanal-V2-fd_EN.txp
\(\surd\)
|
Sr-89/Sr-90 determination by LSC, with
3 energy windows; complex; with using
the (decay) function fd()
|
J-ALUFT_Sr-89_Sr-90_Linf_EN.txp
\(\surd\)
|
Sr-89/Sr-90 determination in exhaust
air (compare with
J-ALUFT-Sr-89-Sr-90_V2_EN.txp)
|
LUBW_Sr-89_Sr-90_with-Sr-85-fixed_V2_EN.txp
|
Sr-89/Sr-90 determination with Sr-85
tracer added, where the tracer count
rate contribution is NOT subject to
fitting
|
Sr89-Sr90_IAEA_AQ-27_2013_V2_EN.txp
|
Sr-89/Sr-90 determination by LSC;
energy window and counting efficiencies
vary between 1st and 2nd measurement
|
Sr89_Sr90_LSC-without-Sr85_EN.txp
|
Sr-89/Sr-90 determination by LSC, with
3 energy windows; without Sr-85-tracer;
with covariances between window
efficiencies
|
Tritium_4Bubbler_used_1-3_DE.txp
|
Measurement of HT and HTO in air with
applying a 4-fold-Bubbler (according to
J.-M. Duda, JER 189 (2018) 235-249),
application of linear unfolding;
bubblers 1,2 and 3 were evaluated
|
Tritium_4Bubbler_used_2-3_DE.txp
|
Measurement of HT and HTO in air with
applying a 4-fold-Bubbler (according to
J.-M. Duda, JER 189 (2018) 235-249),
application of linear unfolding;
bubblers 2 and 3 were evaluated
|
Pb210_Bi210_Po210_series_backwards_EN.txp
|
Examples of using the UR function
SDECAY for a 3-member radioactive
decay chain
|
2.5.1.3. Other examples from the literature, evaluated, without detection limits¶
Neutron-Dose-Cox-2006_V2_EN.txp
\(\surd\)
|
Determination of neutron dose
equivalent
|
Calibration-of-weight-Cox-2001_V2_EN.txp
\(\surd\)
|
calibration of a weight
|
Kessel-1-2006_EN.txp
\(\surd\)
|
calibration of a mass of nominally 10
kg
|
Kessel-2a-2006_EN.txp
\(\surd\)
|
Pb mol mass determination, with several
correlations
|
Kessel-2b-2006_EN.txp
\(\surd\)
|
alternative Pb mol mass determination,
with several correlations
|
Wuebbeler-Ex1_EN.txp
\(\surd\)
|
MC example for non-gaussian
distribution
|
Wuebbeler-Ex2_EN.txp
\(\surd\)
|
MC example for non-gaussian
distribution
|
Pear
sonYork_with_KALFIT_EN.txp
\(\surd\)
|
Application of weighted total LS (WTLS)
to the data Pearson & York data set
|
2.5.1.4. Example for a “negative” linear Model¶
Rn-222-Emanation_EN.txp |
Detection limit calculation for a Rn-222 emanation coefficient |
2.5.1.5. Revision of physical units in the examples¶
With version 2.4.13 of UncertRadio an option was introduced for deriving the physical units of dependent quantities by calculations; see chapters 2.27, 2.26 and Section 5.21. In the context of applying this option, the units used in the example projects of section Section 2.5.1 were tested for correctness. Several modifications were found to be necessary. They mean, that not all units introduced earlier by the author of this program were correct or functional.
In some cases notes about the modifications were documented within the project file, TAB “Procedure”. In most of the cases, it was necessary to change the existing unit “1” (or “ “) for detection probability variables (often called eps…) to “1/Bq/s”. This helps the output variable to receive the unit part “Bq” instead of “1/s”. These latter changes were only seldom documented within the project files. In the example J-ALUFT-Sr-89-Sr-90_V2_EN.txp, two parameters, a and b, used for calculating eps2, got the new units “1/Bq/s/mg” and “1/Bq/s”, respectively.
In another case, Ra226_U235-at-186keV_EN.txp, the equation RRa = RS – RU5 resulted in a difference of the units “1/s” and “Bq”; in this case, in the program the first one was then applied as the unit name for RRa.
In the case of Ac228_binomial_V2_EN.txp, the detection probability epsD is used two times, as part of the parameter p, which should be dimensionless as a parameter of the binomial distribution, and as a part of the calibration factor. This dilemma was solved such that the epsD which is used within the expression for p, receives the unit “1” (or ” “), while a second variable epsD_U was introduced, which as part of the calibration factor got the unit “1/Bq/h”, but the measurement value was set equal to one (without uncertainty).
In such examples explicitly containing scaling factors of 60 for the unit “min” or 1/1000 for the unit “g”, two special switching variables (or Trigger variables) were attributed to these factors; see section Using switching variables in equations.
For a group of projects their version number (_Vx_) in the file name was increased:
Ac228_binomial_V2_EN.txpDWD_sr89_sr90_TDCR_procedure_V2_EN.txpGalpha_beta_Rusconi_2006_V2_EN.txpJ-ALUFT-Sr89-Sr-90_V2_EN.txpJanszen-Sr-89-Sr-90_V3_EN.txpMoreno-Sr90_IAEA-135_V2_EN.txpsumEval_sum_V2_EN.txpsumEval_mean_V2_EN.txpvTI-Y90-16330_Blw_V2_EN.txpvTI-Y90-16671_Blw_V2_EN.txpvTI-Y90-16748_Blw_V2_EN.txp
A consequence of calculating units of dependent variables (withing the menu item “test physical units”) is the transformation to basic units. In some cases, the associated scaling factors change the output quantity value powers of 10:
Galpha_beta_Rusconi_2006_V2_EN.txp: factor 1000 (1/g 1/kg) (permanently
changed)
Sterlinski-2008-NAA_EN.txp: factor 1.0E-9 (due to a unit “ng/g”)
sumEval_summe_V2_DE.txp: factor 1.0E+4 (1/cm2 1/m2)
sumEval_mitteln_V2_DE.txp: factor 1.0E+4 (1/cm2 1/m2)
The last three changes do not apply if the test of physical units is not used, i.e., if the program is used in the normal mode!
A new version was prepared for the file with reference values of the example projects:
BatListRef_v06.txt
