Dose distributions in the
ICRU sphere for monoenergetic
photons and electrons
and for ca. 800 radionuclides
N. Petoussi, M. Zankl,
G. Fehrenbacher, G. Drexler
Institut für Strahlenschutz
GSF-Bericht 7/93
GSF- Forschungszentrum
fü r Umwelt und Gesundheit
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GSF • Forschungszentrum für
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© GSF - Forschungszentrum,
2.
Überarbeitete Auflage
April
1993
1993
Dose distributions in the ICRU sphere for
monoenergetic photons and electrons and for
ca. 800 radionuclides
N. Petoussi, M. Zank!, G. Fehrenbacher, G. Drexler
GSF - Bericht
March
7/93
1993
This work was financially supported by the
Bundesamt für Gesundheitswesen,
Abteilung Strahlenschutz, Bern, Switzerland
under the contract number FE
316-92-353
Contents
1
Calculation of dose distribution for monoenergetic sources
3
1.1
1.2
3
4
Calculation of H'(O.Oi) for monoenergetic point sources
Calculation of H'(IO) for monoenergetic point sources .
2
Calculation of H'(0.07) and H'(lO) for radionuclides
4
3
Comparison with results of other authors
5
4
Dose factors from contamination of the skin
6
5
Conclusions
7
Acknowledgements
7
References
18
Appendix
20.
2
Abstract
Dose distributions for distant point sources in air of monoenergetic photons and electrons
incident on the ICRU sphere have been calculated with the Monte Carlo codes EGS4
and SPHERE. Of particular interest were the <loses at 0.07 and 10 mm depths, which
are for the directional dose equivalent operational quantities H'(0.07) and H'(lO), the rec­
ommended depths to represent the dose equivalents. Similar quantities were previously
calculated by simulating an infinite slab instead of a sphere or broad parallel beams in­
stead of point sources. In our study, the presence of the air is taken into account. The
results were summed over the discrete photon and electron energies and beta spectra to
derive distributions for ca. 800 radionuclides.
Dose rates from skin contamination, beta and gamma, are presented, derived by using
existing data.
3
1
Calculation of dose distribution for monoenergetic
sources
The absorbed dose distributions from incident monoenergetic electrons and photons were
EGS4, and for some photon exposures, additionally
SPHERE. EGS4 is an elcctron-photon transport code used
extensively, mainly for electron beam calculations /1/. At the version used for the present
work the PRESTA algorithm was implemented /2/. SPHERE is a photon transport code
developed at the GSF and employed to estimate dose distributions in the ICRU sphere
/3/. Details of the codes can be found elsewhere. The energy at which the particle history
was terminated was 1 % of the incident energy except for energies below 200 keV where 2
calculated with the Monte Carlo code
with the Monte Carlo code
·.
keV were used.
The medium considered was the ICRU sphere which is a sphere of
sisting of tissue equivalent material
air at
100
and
10
/4/.
30
cm diameter con­
The simulated sources were point sources in
cm distance from the sphere, positioned on the principal axis.
dose distributions were calculated at various depths inside the sphere (from
0.007
-
The
to
15
cm) and were obtained as dose per entrance ßuence or dose per particle. (The entrance
ßuence is derived purely geometrically from the number of particles emitted from the
source and the field size at the entrance point. For this quantity, the presence of the air
is not considered). Of particular importance were the depths at
H'(0.07)
are the directional dose equivalents
by ICR U
/5/.
and
H'{lO)
0.07
and
10
mm which
defined for operational purposes
The <loses were derived from the calculated energy deposited at collecting
volumes surrounding the points of interest modeled as cylinders with a center at those
points. For example, to estimate the dose at
a cylinder with height from
0.05
to
0.09
0.07
mm depth, the collecting volume was
mm on the principal axis and radius
1
cm. At
bigger depths the collecting volumes were !arger to improve statistical accuracy. (At
mm depth, the collecting cylinder had
5
mm height and
1
10
cm radius).
The absorbed <loses are numerically equal to the dose equivalent, since the quality factor
for photons and electrons is unity.
1.1
Calculation of H '(0.07) for monoenergetic point sources
In order to calculate the
H'(0.07)
the dose equivalent at
sphere has to be evaluated, for sources at
Figures
1
and
2
10
0.07
mm depth of the ICRU
cm distance from the surface of the sphere.
show the dose equivalent per ßuence at
0.07
mm depth, as a function
of energy emitted, for photons and electrons respectively; also shown are the standard
deviations due to Monte Carlo calculations. On the original data cubic spline functions
were fitted, shown also on the figures. Table
1
gives the data in a tabular form.
4
1.2
Calculation of H '(10) for monoenergetic point sources
In order to estimate the
H'(lO),
the <lose equivalent at
has to be evaluated, for sources at
Figures
3
and
4
100
10
mm depth of the ICRU sphere
cm distance from the surface of the sphere.
show the <lose per ßuence at
10
mm depth, as a function of energy
emitted, for photons and electrons respectively, together with their standard deviations
and the fitted spline functions. Table
2
Calculation of H
2
gives the data in·a tabular form.
'(0.07)
and H
'(10)
for radionu­
clides
Using the results for monoenergetic sources and nuclear data for ca. 800 radionuclides,
the
H'(0.07)
and
H'(lO)
for radionuclides were derived. The data for the radioactive decay
of the radionuclides were taken from Brenk
the ICRP data on nuclear transformations
/6/.
/7/.
These data are identical to the data of
Data for the emitted gamma rays are
included, together with the beta spectra and the discrete Auger and conversion electrons.
The beta spectra were calculated according to Dillrnan /8/.
The energy distribution for a given beta transition ranges from zero energy to the max­
imum endpoint energy. We define
nurnber per decay,
E;,
f;.
as the intensity of the ith discrete electron (e) in
as· the energy of the ith discrete electron in MeV,
sity of the jth continuous beta transition (ß) in number per decay,
energy in MeV for the jth beta transition, and
Eiß""'
f;fJ
as the inten­
as the endpoint
N;fJ(E) as the energy distribution function
for the jth beta transition. The energy distribution function is assumed to be normalised
so that
E""•s
f0 j#
N;fJ(E)dE
=
1.
Then, for a given electron spectrum, the dose equivalent rate factor due to beta radiation
and electrons is given by
.
H.
=
L; f;,
.
·
Ems�
H,(E;,) + L; f;p f0
;#
.
N;fJ(E) H,(E)dE
·
where tbe summations over i and j include all discrete and continuous electron radiations.
The dose equivalent rate factor. due to gamma and x-rays is given by
where /i.-, is the intensity of the kth photon in nurnber per decay and
of the kth photon in MeV.
Ei.-,
is the energy
5
Both fl. and fl„ were estimated by logarithmic interpolation using the spline functions
fitted on the data of tables l and 2, derived from the Monte Carlo calculations.
To obtain the <lose rates for a source of a unit activity, one has to take into account
the geometry simulated, i.e. point source at a distance of 10 or 100 cm from the surface of
the sphere, and multiply by a "geometry factor" which a:.llows for the ratio of the particles
emitted to those reaching the surface of the sphere.
Tables Al and A2 of the Appendix give the H'(0.07) and H'(lO) in mSv h-1 GBq-1•
The separate contribution to the <lose equivalent due to gamma and electron radiation
can be also seen.
·
•
The <lose equivalent quantities H'(0.07) and H'( 10) (in mSv) can be calculated for a specific
case from the tabulated values of <lose quivalent rates per activity (in mSv h-1 GBq-1)
by multiplying with the actual source activity (in GBq) and the time of exposure (in h).
·
3
•
Comparison with results of other authors
Various authors, for example, /9-13/, have calculated dose distributions for electrons and
photons on water, but there are no results which are directly comparable with the present
ones due to differences on the irradiation geometries. In most cases, parallel beams were
considered incident normally oit infinite water slabs, whereas the presence of air was not
taken into account. Table 3 shows the present results for electrons at 0.07 mm depth,
compared with results taken from Bielajew and Rogers /2/ and Cross et al /12/. Table
4 shows the present results at l cm depth, compared with results taken from the ICRP
Publication 51 /ll/ and Cross et al /12/. lt could be seen that by ignoring the presence
of the air, one overestimates largely the dose for· electron energies lower than 200 keV
for point sources 10 cm distant from the sphere and 0.07 mm depth; for electron point
sources 100 cm distant and 10 mm depth, the absence of air results to overestimation for
all energies.
6
4
Dose factors from contamination of the skin
The <lose equivalent in tissue at a depth of 0.007 cm is widely used as a quantification
of the hazard from beta radiation. This is practically the same as the directional <lose
equivalent H'(0.07) defined by the ICRU /5/, since the radius of the ICRU sphere is !arge
compared with the ranges of most beta rays in tissue and its surface, near the point of
interest, is therefore close to a plane. Furthermore, the ICRP has recommended /14/
that for evaluating deterministic effects from localised skin exposures, <loses should be
averaged over areas of no more than 1 cm2.
Various authors have presented dose-factors for contamination of the skin, due to beta
radiation. For the present work, the recent data of Cross et al. ../15/ were taken, who
calculated with Monte Carlo methods <lose distributions from beta contamination on an
air-water interface for monoenergetic electrons from 0.025 to 4 MeV. Figure 5 shows the
<lose rate at 0.007 cm depth in water, on the axis of 1 Bq· cm-2 isotropic sources of
monoenergetic electrons distributed uniformly over a 1 cm2 circular area, on an air-water
boundary.
The <lose factors shown in figure 5 were used, together with the nuclide data of Brenk /6/,
to calculate the <lose distribution due to beta emission, conversion and Auger electrons
as described above.
Although the beta component of H'(0.07) from skin contamination generally exceeds by
far the gamma component, there are cases when the latter plays an equal role as shown
by Henrichs et al /16/. For this reason, estimates of the <lose factors due to gamma skin
contamination are also included.
To obtain those, Specific Absorbed Fractions (SAF) were taken from Snyder et al /17/,
for monoenergetic photon sources in the energy range 0.010 - 4 MeV, shown in figure 6.
Dose equivalent coefficients for radionuclides were obtained by summing up the SAF
for the various photon energies E;� emitted, weighted by their relative frequencies fh:
D(skin)
=
1.6 · 10-1o 'L,J;� E;� SAF;�
·
·
·
D(skin) gives the <lose to the skin per single decay, or equivalently, the <lose rate in Sv/s
for an activity of 1 Bq on the body surface. The total <lose may be derived by multiplying
with the number of decays.
The specific absorbed fractions, SAF;� in g-1 were derived by logaritmically interpo­
lating the values shown in figure 6.
The skin <lose rates in terms of Sv/s per Bq·cm-2 can be obtained from the above formula
by multiplying with the total surface of the body i.e. skin, which is 17 000 cm2•
·
7
Table A3 of the Appendix shows the H'(0.07) from skin contamination due to gamma
and beta radiation in mSv h-1 kBq-1• cm2•
·
5
•
Conclusions
Photon and beta ray <lose rates have been calculated inside the ICRU sphere for monoen­
ergetic point sources in air at a distance of 100 and 10 cm from the surface of the sphere.
The calculations were performed using the Monte Carlo codes EGS4 and SPHERE. Using
these data, the H'(0.07) and H'(lO) for ca. 800 radionuclides were derived for 10 and 100
cm distant sources respectively.
,.
Tables Al and A2 of the Appendix give the H'(0.07) and H'(lO) in mSv h-1 GBq-1 for
�
nume ous radionuclides.
·
•
Comparing the above results to <lose rates from parallel beams incident normally on
infinite water slabs, it was found that by ignoring the presence of the air, one overesti­
mates largely the <lose for electron energies lower than 200 keV for point sources 10 cm
distant from the sphere and 0.07 mm depth; for electron point sources 100 cm distant and
10 mm depth, the absence of air results to overestimation for all energies.
Furthermore, <lose rates from skin contamination, beta and gamma, are presented, de­
rived by using data of Cross et al /15/ and Snyder et al /17 /. Table A3 gives the H'(0.07)
from skin contamination in mSv h-1 kBq-1 cm2 for radionuclides.
·
•
•
The tables are arranged in order of increasing atomic number. Within a given atomic
number, the radionuclides appear in order of decreasing mass number.
Acknow ledgements
This project was financially supported by the Bundesamt für Gesundheitswesen Abteilung
Strahlenschutz, Bern, Switzerland under the contract number FE 316-92-353. We wish
to express our thanks for many useful discussions and advice to Drs. W. Zeller and M.
Jungck of the Bundesamt für Gesundheitswesen, Dr. Ch. Vernli of the Paul Scherrer Insti­
tut, Villigen and Prof. J.-F. Valley of the Institut de Radiophysique Appliquee, Lausanne.
The advice of Dr. Klaus Henrichs of SIEMENS AG, Germany, is gratefully acknowl­
edged.
8
Table 1: Dose equivalent at 0.007 cm depth at the main axis of
the ICRU sphere, H'(0.07}, from point sources ofmonoenergetic
photons and electrons at distance of 10 cm from the surface of
the sphere
Energy Dose per
Dose per Dose per
emitted fluence due emitted fluence due
to electrons electron to photons
Sv.cm2
Sv.cm2
MeV
Sv
0.010
0.015
0.020
0.025
0.030
. 0.040
0.050
0.060
0.070
0.080
0.090
0.100
0.125
0.150
0.200
0.300
0.400
0.500
0.600
0.800
1.000
2.000
3.000
4.000
5.000
0.40E-14
0.22E-10
0.19E-09
0.98E-09
0.lOE-08
0.87E-09
0.32E-l7
0.18E-13
0.15E-12
0.78E-12
0.81E-12
0.70E-12
0.47E-09
0.37E-12
0.38E-09
0.35E-09
0.32E-09
0.28E-09
0.28E-09
0.28E-09
0.27E-09
0.30E-12
0.28E-12
0.2.5E-12
0.23E-12
0.22E-12
0.22E-12
0.22E-12
Dose per
emitted
photon
Sv
0.72E-11
0.31E-ll
0.18E-11
0.12E-11
0.84E-12
0.55E-12
0.43E-12
0.39E-12
0.41E-12
0.42E-12
0.57E-14
0.25E-14
0.14E-14
0.92E-15
0.67E-15
0.44E-15
0.34E-15
0.31E-15
0.32E-15
0.33E-15
0.50E-12
0.40E-15
0.76E-12
0.llE-11
0.16E-ll
0.61E-15
0.84E-15
0.13E-14
0.2iE-ll
0.22E-14
0.50E-ll
0.83E-l l
0.40E-14
0.66E-14
0.13E-10
O.lOE-13
Distance source - surface of sphere: 10 cm
Diameter of sphere: 30 cm
F ield size at entrance point: 0.126·103 cm2
Fraction of particles emitted reaching the sphere: 0.100
9
Table 2: Dose equivalent at 1 cm depth at the main axis of
the ICRU sphere, H'(lO), from point sources of monoenergetic
photons and electrons at distance of 100 cm from the surface of
the sphere
Dose per Dose per
Energy Dose per
emitted fluence due emitted fluence due
to electrons electron to photons
Sv.cm2
Sv.cm2
Sv
MeV
0.010
0.015
0.020
0.025
0.030
0.040
0.050
0.060
0.070
0.080
0. 100
0.150
0.200
0.300
0.500
1.000
2.000
2.500
3.000
3.500
4.000
4.500
5.000
0.34E-14
0.31E-ll
0.45E-10
0.14E-09
0.24E-09
0.30E-09
0.34E-09
0.35E-09
0.27E-19
0.25E-16
0.36E-15
0.12E-16
0.19E-f4
0.24E-14
0.27E-14
0.28E-14
Dose per
emitted
photon .
Sv
0.49E-13
0.69E-12
0.96E-12
0.85E-12
0.75E-12
0.59E-12
0.50E-12
0.49E-12
0.48E-12
0.51E-12
0.59E-12
0.83E-12
O.llE-11
0.l7E-ll
0.27E-ll
0.52E-ll
0.84E-ll
0.39E-18
0.55E-17
0.76E-17
0.68E-17
0.60E-17
0.47E-l7
0.40E-17
0.39E-17
0.38E-l7
0.41E-l7
0.46E-17
0.66E-l7
0.85E-17
0.13E-16
0.22E-16
0.41E-16
0.67E-16
0.12E-10
0.96E-16
Distance source - surface of sphere: 100 cm
Diameter of sphere: 30 cm
Field size at entrance point: 0.537·103 cm2
Fraction of particles emitted reaching the sphere: 0.427· 10-2
10
Table 3: H1(0.07) in Sv.cm2 for monoenergetic electrons
from various workers and methods
Energy
Dose per fluence
emitted
Sv.cm 2
MeV
GSF
Bielajew /2/ Cross et al /12/
point source
broad parallel broad parallel
10 cm distance
ICRU sphere
slab/water
slab/water
air
no a1r
no a.ir
0.080 0.40E-14
0.090 0.22E-10
0.100 0.19E-09
0.125 0.98E-09
0.150 0.lOE-08
0.200 0.87E-09
0.400 0.47E-09
0.600 0.38E-09
0.800 0.35E-09
1.000 0.32E-09
2.000 0.28E-09
3.000 0.28E-09
4.000 0.28E-09
0.18E-08
0.18E-08
0.32E-09
0.90E-09
0.90E-09
0.18E-08
O.ISE-08
0.!4E-08
0.90E-09
0.48E-09
0.39E-09
0.35E-09
0.33E-09
0.29E-09
0.30E-09
0.30E-09
11
Table 4: H'(lO) in Sv.cm2 for monoenergetic electrons
from various workers and methods
Dose per fluence
Energy
emitted
Sv.cm 2
MeV
ICRU 51 /11/ Cross et al /12/
GSF
broad parallel broad parallel
point source
100 cm distance
slab/water
slab/water
ICRU sphere
no air
no air
air
1.000
2.000
2.500
3.000
3.500
4.000
4.500
5.000
0.34E-14
0.31E-11
0.45E-10
0.14E-09
0.24E-09
0.30E-09
0.34E-09
0.35E-09
0.23E-11
0.35E-09
0.50E-09
0.32E-09
0.40E-09
12
"'
Q_
"
0
s.
I
1 0-
13
'-'-.......J����L-���L-��_.__J
0.10
1.00
0.01
Photon energy
Fig.
1:
sphere
( MeV)
Dose equivolent per unit fluence ot
(on
0.07
mm depth in the
ICRU
the moin oxis ) produced by monoenergetic photon point
sources in oir
10
cm distont from the surfoce
13
+
0.1
1.0
Electron energy (MeV)
10.0
Fig. 2: Dose equivolent per unit fluence ot 0.07 mm depth in the ICRU
sphere ( on the moin oxis) produced by monoenergetic electron point
sources in oir 10 cm distont from the surfoce
"E
14
11
10-
u
�
>
Q)
u
c
Q)
::i
-12
"' 10
�
0
Q.
0.0 1
1.00
0.10
Photon energy (MeV)
Fig.
3:
sphere
Dose equivolent per unit fluence et
(an
10
mm depth in the
ICRU
the mein oxis) produced by monoenergelic photon point
sources in oir
100
cm distont from the surfoce
Fig. 4: Dose equivolent per unit fluence et
sphere
( on
the moin oxis
sources in oir
100
)
10
mm depth in the
produced by monoenergetic
cm dislont from the surfoce
electron
ICRU
point
16
N
E
�
�
0m
1000
r.
,;._
ü
s
„
"§
„
"'
0
0
100
0
0.1
1.0
Electron energy (MeV)
Fig. 5: Dose rote ot 0.07 mm depth in woter, on the oxis of 1 Bq.cm-'
isotropic sources of monoenergetic electrons distributed uniformly over
1 cm' circulor oreo, an an oir-woter boundory (from Cross et ol, /12/)
17
10-4
�
..:=;
�
<
U1
10-5
0.01
0.10
1.00
Photon energy (MeV)
Fig. 6: Specific obsorbed froction (SAF) of photon energy;
source in skin, torget: skin; (from Snyder et ol, /17 /)
Ref erences
l.
Nelson, W.R.. Hirayama, A. and Rogers, D.W.O. The EGS4 Code
System. Stanford Linear Accelerator Center Report SLAC-265
Stanford, CA 94305, (1985)
2. Bielajew, A.F. and Rogers. D.W.O. PRESTA: the Parameter
Reduced Electron-Step Transport Algorithm for electron Monte
Carlo transport. Nucl. Instr. Methods. Bl8, 165-181 (1987)
3.
Williams. G., swanson, W.P., Kragh, P. and Drexler, G.
Calculation and analysis of photon dose equivalent
distributions in the ICRU sphere. GSF-Bericht S-958.
Gesellschaft für Strahlen- und Umweltforschung mbH, München
(1985)
4.
International Commission on Radiation Units and Measurements:
Radiation Quantities and Units. ICRU Report 33, International
Commission on Radiation Units and Measurements, Bethesda, MD
(1980)
5. International Commission on Radiation Units and Measurernents:
Determination of Dose Equivalents Resulting from External
Radiation Sources. ICRU Report 39, International Commission
on Radiation Units and Measurements, Bethesda, MD (1985)
6.
Brenk, H.D. Dosisfaktoren für ca. 800 Radionuklide zur
Berechnung der externen Strahlenexposition durch Photonen­
und Elektronenstrahlung. Brenk Systemplanung, Aachen (1983)
7.
International Commission on Radiological Protection.
Radionuclide transformations: Energy and Intensity of
Emissions. ICRP Publication 38, Annals of the ICRP 11-13,
Pergamon Press. Oxford, (1983)
8. Dillman, L.T. EDISTER - A computer program to obtain a
nuclear decay data base for radiation dosimetry. Oak Ridge
National Laboratory, Report ORNLTM-6689 (1980)
9. Berger, M.J. Distribution of absorbed dose around a point
source of electrons and beta particles in water and other
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bei äußerer Strahlenexposition durch Photonenstrahlen und
Berechnungsgrundlage für die Ermittlung von Körperdosen bei
äußerer Strahlenexposition durch Elektronen, inbesondere
durch ß-Strahlung. Veröffentlichungen der
Strahlenschutzkommission, Band 3 (1986)
19
11. International Commission on Radiological Protection.
use in Protection Against External Radiation. ICRP
Publication 51, Pergamon Press, Oxford, (1987)
Data for
12.
Cross, W. G., Freedman N.O. and Wong, P. Y. Dose distributions
for electrons and beta rays incident normally on water.
Radiat. Prot. Dos., Vol 35, 2 (1991)
13.
Cross. W.G.. Freedman N. O. and Wong, P.Y. Beta ray dose
distributions from point sources in an infinite water medium.
Health Physics, Vol 63, 2 (1992)
14. International Commission on Radiological Protection.
Recommendations of the International Commissi.on on
Radiological Protection. ICRP Publication 60,, . . Pergamon Press.
Oxford, (1991).
15. Cross. W. G., Freedman N. O. and Wong, P. Y. Beta ray dose
distributions from skin contamination. Radiat. Prot. Dos.
(1992)
16. Henrichs. K. , Eiberweiser, C. and Paretzke, H. G.
Dosisfaktoren für die Kontamination der Haut und der
Kleidung. GSF-Bericht 7/85. Gesellschaft für Strahlen- und
Umweltforschung mbH, München (1985)
17.
snyder, w. s . • Ford M.R . • Warner G. G. and Watson, S.B. A
tabulation of dose equivalent per microcurie-day for source
and target organs of an adult for various radionuclides.
Report No. ORNL-5000, Vol. 1, Oak Ridge National Laboratory,
Oak Ridge (1974)
Appendix
Tables Al and A2 give the H'(0.07) and H'(lO) in mSv h-1 GBq-1•
·
·
Table A3 gives the H'(0.07) from skin contamination in mSv h-1 kBq-1 • cml.
·
•
The tables are arranged in order of increasing atomic number. Within a given atomi
number, the radionuclides appear in order of decreasing mass number.
·
- 21 0
Appendix
Table Al
Dose equivalent at 0.07 mm depth in the ICRU sphere at the main axis,
H'(0.07), for radionuclides emitted from point sources at a distance of
10 cm from the surface of the sphere.
The <lose are given in mSv
·
h-1
·
GBq-1•
- 22 -
Element
Electron
Photon
Contribution
Contribution
Sum
B
3
0.0011:+00
1.4711:-03
l.47&-03
BK
7
9.8511:-05
7.7211:-01
7.7211:-01
BK
10
1.6511:+03
O.OOE+OO
1.6511:+03
c
11
1.4611:+03
1.6011+01
1. '811:+03
•
13
1.3411:+03
1.6811:+01
1.3611:+03
c
u
1.53E+02
0.0011:+00
1.5311:+02
0
15
1.1511:+03
1.7311:+01
1.1711:+03
r
18
1.6611:+03
1.6011:+01
1.6811:+03
NI:
19
1.0511:+03
1.7711:+01
1.0711:+03
22
1.5311:+03
3.1511:+01
1.5711:+03
1.3111:+03
NA
NA
24
1.2611:+03
4.7511:+01
AL
26
1.0611:+03
3.5611:+01
i .0911:+03
AL
28
9.7111:+02
2.1811:+01
9.9311:+02
IG
28
1.4211:+03
2.0211:+01
1.4411:+03
p
30
9.3011:+02
1.601+01
9.46E+02
SI
31
1.2311:+03
1. 2011:-02
1.2311:+03
p
32
1.1711+03
0.0011:+00
1.1711:+03
SI
32
5.0311:+02
O.OOE+OO
5.03E+02
p
33
7. 35E+02
0.0011:+00
7.3511+02
s
35
1.8911:+02
0.001!+00
1.8911:+02
CL
36
1.4511:+03
2.3711:-03
1. 4511:+03
37
0.001!+00
0.001!+00
0.0011:+00
CL
38
1.051!+03
1.77&+01
1.0611:+03
lt
38
9.681!+02
4.091!+01
1.0111:+03
39
1.53E+03
3.48E-01
1.5311:+03
CL
39
1.1211:+03
1.9311:+01
1.UE+03
lt
40
1.09Jr:+03
2.031+00
1. 0911:+03
41
1.3311:+03
1.801+01
1.3511:+03
CA
41
0.0011+00
O.OOE+OO
0.0011:+00
lt
42
9.63E+02
3.541+00
9.6611:+02
lt
43
1.461!+03
1.5011:+01
1.4711:+03
SC
43
1.20E+03
1.721!+01
1.22E+03
1.02E+03
2.7411:+01
1.05B+03
2.29E+02
4.30E+OO
2.3311:+02
1.1911:+03
AR
AR
AR
lt
"
SC
UM
"
"
1.16E+03
3.12E+01
'l.'I
7.8911:-05
2.Ul!+OO
2.UE+OO
CA
45
7.4911!+02
3.4611:-05
7.4911:+02
SC
1
z
lt
45
1.0511:+03
2.3111:+01
1.0711:+03
'l.'I
45
1.21"+03
1.3611:+01
l.22E+03
SC
46
1.191!+03
2.8511:+01
1.2111:+03
CA
47
1.43E+03
1.44E+01
1.4411:+03
SC
47
1.42E+03
1.59E+OO
1.4211:+03
V
47
1.06!+03
1.551!+01
1.08E+03
CR
48
4.18E+01
6.67E+OO
4.851!+01
SC
48
1.49E+03
4.651!+01
1.54E+03
V
48
8.36E+02
4.09E+Ol
8.7711:+02
CA
49
1.09E+03
3.23E+01
1.121!+03
CR
49
1.191;:+03
1.6411:+01
1.2011:+03
SC
49
1.1011!+03
1.2911:-02
1.10E+03
V
49
0.001!+00
0.0011:+00
0.0011:+00
CR
51
2.7011:-01
2.40E+OO
2.6711:+00
51
1.02E+03
1.5511:+01
1.0311:+03
52
9.091!+02
1.UE+Ol
9.2111:+02
MN
n:
- 23
-
MN
52M
9 . ' 9E+02
3 . 40E+01
9 . 8 3E+ 0 2
MN
52
5 . 22&+02
4 . 84E+01
5 . 71E+02
MN
53
O . OOE+OO
1 . 81E+01
1 . 8 1E+Ol
MN
54
2 . 39E-01
1 . 23E+01
1 . 26E+01
CO
55
9 . 7 9E+ 02
2 . 93E+ 0 1
1 . 01E+ 0 3
FE
55
O . OOE+OO
1 . 68E+01
1 . 6 8E+ 0 1
CO
56
2 . 50E+02
4 . 61E+ 0 1
2 . 9 6E+ 0 2
MN
56
1 . 17E+03
2 . 2 5E+ 0 1
1 . 1 9E+ 0 3
NI
56
3 . 79E+01
2 . 53E+ 0 1
6 . 32E+ 0 1
CO
57
8 . 1 4E+Ol
3 . 1 3E+ 0 1
1.131:+ 0 2
NI
57
6 . 42E+02
2 . 58E+Ol
6 . 6 8E+ 0 2
CO
58M
O . OOE+OO
1 . 22E+01
1 . 2211:+ 0 1
CO
58
2 . 74E+02
2 . 2 5E+ 0 1
2 . 9611:+02
n
59
1 . 1011:+ 0 3
1 . 6 311:+ 0 1
1 . 1211:+03
NI
59
0 . 0 0 11:+ 0 0
1 . 46E+01
1 . 4 611:+ 0 1
CO
60M
3 . 0 511:+ 0 0
1 . 38E+01
1 . 6 911:+ 0 1
CO
60
1 . 0111:+03
3 . 38E+01
1 . 04E+03
60
9 . 7 6E+ 02
5 . 1 3E+ 0 1
1.0311:+03
n
60
8 . 6 8E+Ol
0 . 0 0 11:+ 0 0
8 . 6811:+ 0 1
CO
61
1 . 311:+03
2 . 9011:+00
1 . 3111:+ 0 3
61
8 . 39E+02
1 . 2711:+ 0 1
8 . 5211:+ 0 2
62M
1 . 0 4E+ 0 3
3 . 57E+ 0 1
1 . 08E+03
9 . 4511:+02
CU
CU
CO
CU
62
9 . 2911:+ 02
1 . 5711:+ 0 1
ZN
62
1 . 4911:+02
1 . 9 0E+ 0 1
1 . 68E+02
NI
63
O . OOE+OO
0 . 0011:+00
O . OOJ:+OO
ZN
63
9 . 68E+02
1 . 68E+01
9 . 85&+02
64
8 . 50E+02
8 . 4 5E+OO
8 . 58&+ 02
CU
GA
65
1 . 00E+03
1 . 78E+01
1 . 02E+03
NI
65
1 . 23E+03
7 . 3 0E+OO
1 . 23&+03
ZN
65
2 . 51E+ 0 1
1 . 90&+01
4 . 41&+01
66
1 . 021:+03
1 . 2 0&+ 0 0
1 . 02&+ 0 3
GA
66
5 . 35&+02
3 . 03E+ 0 1
5 . 65&+02
GI:
66
3 . 97E+ 02
2 . 0 9E+ 0 1
4 . 1 8E+ 0 2
NI
66
5 . 71&+02
0 . 00&+ 0 0
5 . 71J:+02
67
1 . 33&+ 0 3
3 . 30E+00
1 . 33&+03
GA
67
1 . 59E+ 0 1
1 . 7 6E+ 0 1
3 . 35&+01
GI:
67
9 . 4 3E+ 02
2 . 1 0E+ 0 1
9 . 64E+02
GA
68
9 . 83&+02
1 . 4 8E+ 0 1
9 . 97&+02
GE
68
0 . 0 0E+OO
l . 0 4E+Ol
l . 04E+01
AS
69
9 . 17E+ 02
1 . 5 8E+Ol
9 . 32&+02
GI:
69
4 . 7 1E+ 02
l . 6 9E+Ol
4 . 8 8E+ 0 2
ZN
6 9M
6 . 5 8E+Ol
6 . 5 6E+OO
7 . 23E+01
ZN
69
l . 43E+03
9 . 21&-05
1 . 43&+03
AS
70
9 . 4 6E+ 0 2
5 . 69E+Ol
1 . 0 0 &+ 0 3
GA
70
l . l 8E+o3
1 . 3 5 &- 0l
l . 1 8E+ 03
CU
CU
SE
70
8 . 71E+02
2 . 62&+ 0 1
8 . 9 811:+02
AS
71
6 . 95E+02
l . 5 8E+Ol
7 . 1 011:+ 0 2
GI:
71
0 . 00&+ 0 0
l . 05E+Ol
l . 05E+ 0 1
ZN
71M
1 . 24E+03
2 . 36E+ 0 1
1 . 27&+ 0 3
AS
72
8 . 7 9E+ 02
2 . 65E+Ol
9 . 0 5E+o2
GA
72
l . 33E+ 0 3
3 . 5 0E+Ol
1 . 36&+ 0 3
ZN
72
9 . 25E+02
1 . 30E+01
9 . 38E+02
AS
73
O . OOE+OO
2 . 15E+01
2 . 15E+Ol
GA
73
1 . 33E+03
l . 62E+Ol
l . 34E+03
SE
73M
2 . ( 6E+ 02
4 . 99E+OO
2 . 5111:+02
SE
73
8 . 57E+ 02
2 . 0 0E+Ol
8 . 7711:+02
AS
74
8 . 82E+ 02
l . 38E+Ol
8 . 9 6E+ 02
BR
74M
8 . 8 1&+02
5 . 4 0E+Ol
9 . 35E+02
BR
74
9 . 30E+02
5 . 53&+01
9. 851i+02
D
74
9 . 2 3E+ 02
l . 9 3E+Ol
9 . 42&+02
- 24
-
BR
75
e . 63E+02
l . e 6z+Ol
e . e 2z+02
GE
75
l . 35E+03
5 . 33E-Ol
l . 35E+03
SE
75
6 . 931!!+ 01
l . 55E+Ol
e . 4 8E+Ol
AS
76
l . 0 31!!+ 0 3
6 . 3211:+00
l . 0411:+03
BR
76
6 . leE+02
3.4 5E+Ol
6 . 53E+02
Jal
76
l . 2 0E+Ol
l . 55E+Ol
2 . 7611:+ 01
AS
77
l . 4611:+03
l . 36E-Ol
l . 4 6E+03
BR
77
5 . 0U:+Ol
l . 2eE+Ol
6 . 2 811: + 0 1
GE
77
l . 2 111:+ 0 3
l . 5511:+01
l . 2311:+03
Jal
77
9 . 92E+02
l . e 311+0l
l . OlE+03
SE
77)(
l . 3311:+03
4 . e511+00
l . 3 411:+03
AS
7e
l . 0011:+03
l . 7 311+01
l . 0211:+03
GE
1e
l . 4 811:+03
4 . 3511+00
l . 4 8E+03
Jal
79
l . 30E+02
l . 0 9E+Ol
l . 4lE+02
RB
79
l . 5111:+03
2 . 34E+Ol
l . 53E+03
SE
79
2 . 4 31!!+ 0 2
O . OOE+OO
2 . 43E+02
BR
eOM
0 . 001+00
l . 151+01
l . 1 51+01
BR
eo
l . 0711:+03
l . 651+00
l . 0 811:+03
RB
eo
8 . 5211+02
l . 941+01
8 . 72E+02
SR
eo
0 . 001!+00
6. 391+00
6 . 39&+00
Jal
elM
e . 971+02
4 . 07&+00
9 . 01&+02
Jal
e1
2 . 771!-0l
7 . 251+00
7 . 53&+00
RB
8lM
2 . 38&-0l
4 . 751+00
4 . 99&+00
RB
e1
l . 3lE+03
l . 61&+01
1 . 32&+03
SE
8lM
l . 20E+02
6 . 581!+00
l . 271+02
SE
e1
l . 2lE+ 0 3
l . 42E-01
1 . 21&+03
SR
e1
9 . 52E+02
2.1 2E+Ol
9 . 7 3&+02
BR
82
l . 3lE+03
3 . e 3E+Ol
1 . 351+03
RB
82M
3 . 5 61:+02
4 . 52E+Ol
4 . 011+02
RB
82
e . 8 21!!+ 02
l . 69E+Ol
e . 991!+02
6 . 2 911:+ 0 0
SR
82
0 . 0 01!! + 00
6 . 2 9E+OO
BR
e3
1 . 4llH 03
l . 1711-0l
1 . 421+03
Jal
e3M
0 . 0 01!!+ 0 0
3 . 34E+OO
3 . 341:+ 00
RB
83
l . 54E+OO
l.5 8E+Ol
1 . 7 31+01
SE
83
1 . 3 31!!+ 0 3
3 . 3811:+01
1 . 36&+03
SR
83
3.331!!+ 02
1 . 9711:+01
3 . 53E+02
BR
84
l . 08E+03
2 . l3E+Ol
l . 10E+o3
RB
e4
4 . 2 0E+02
l . 7 9E+Ol
4 . 38E+02
Jal
85M
1 . 3 61!!+ 0 3
3 . l7E+OO
l . 36E+03
l . UE+03
Jal
85
1 . 44E+03
4. 4 0E-Ol
SR
85M
6. 3 01!!+ 01
4 . 0711:+00
6. 7111:+01
SR
85
e . 2 3E+OO
l . 4 0E+Ol
2 . 22E+01
RB
86
l . l 8E+03
l . 33E+OO
l . l8E+03
y
86M
l . 5lE+02
3 . 5111:+00
1 . 551!+02
y
86
4 .l4E+02
4 . e 6E+Ol
4 . 63&+02
ZR
e6
9.lOE+Ol
1.4611:+01
l . 061+02
Jal
87
l . OlE+03
l . 2 6E+Ol
l . 021!+03
RB
87
l . 3 41!! + 0 3
0 . 0 0B+OO
l . 341:+03
SR
87M
2 . 48E+02
5 . 9211:+00
2 . 541:+02
y
e1
6 . l 8E+OO
l . 2 6E+Ol
l . ees+Ol
Jal
ee
l.36E+03
2 . 3 6E+Ol
l . 3eB+03
NB
88
9 . 00E+02
6 . 3 0E+Ol
9 . 6 31!!+ 0 2
RB
88
9 . l2E+02
l . l 9E+Ol
9 . 2411:+ 0 2
y
88
3 . 8 3E+OO
3.7 9E+Ol
4 . l7E+Ol
ZR
88
3 . 9lE+Ol
l . l 6J:+Ol
5 . 0711:+01
NB
8 9short e . 9 31!! + 02
2 . 99&+01
9 . 2 3B+02
NB
89long
7 . 00E+02
l . 9lB+Ol
7 . 191+02
RB
89
l . llE+0 3
2. 66E+Ol
l . l4B+03
SR
89
l . 22E+03
l . 23B-03
1 . 2 2E+03
ZR
e9
3 . 50E+02
2 . 07E+Ol
3 . 7111:+02
- 25 -
MO
90
1 . 00E+03
1 . 7711:+01
1 . 0 2 11:+ 0 3
NB
90
1 . 4 7 1!:+ 0 3
5 . 53E+Ol
1 . 5311:+03
SR
90
1 . 4 61!:+ 0 3
0 . 0 01!:+ 0 0
1 . 4 6JE+ 0 3
y
9011:
1 . 8 6 1!:+ 0 2
9 . 7 6E+OO
1 . 951:+02
y
90
1 . 07E+03
8 . 18E-04
1 . 07JE+03
SR
91
1 . 2 21!:+ 0 3
1 . 00E+Ol
1 . 2 3E+ 0 3
y
9111:
5 . 691!:+01
8 . 2 3 11:+ 0 0
6 . 5111:+01
y
91
1 . 20E+03
4.9U-02
1.2011:+ 0 3
SR
92
1.4111:+03
1 . 7711:+01
1 . 4 3 11:+ 0 3
y
92
9 . ·7211:+02
3 . 5511:+ 0 0
9 . 7511:+02
MO
9311
7 . 7 3JE+ 02
3 . 0911:+01
8 . 0CJ:+ 02
MO
93
0 . 0 0 11:+ 0 0
4 . 4111:+ 0 0
4 . 4111:+ 0 0
7 . 7611:-01
NB
9311
0 . 0011:+ 0 0
7 . 7 611:-01
TC
9311
2 . 9311:+02
9 . 8CJ:+OO
3 . 0211:+02
TC
93
8 . 1 911:- 0 1
2.2511:+01
2. 3·3&+ 0 1
1.0111:+03
y
93
1 . 0 1 11:+ 0 3
1 . 2011:+ 0 0
ZR
93
0 . 0011:+ 0 0
0 . 0011:+ 0 0
0. 0 0 11:+ 0 0
NB
94
1 . UE+ 0 3
2 . 341:+01
1 . 4 611:+ 0 3
2 . 1611:+01
IW
94
9 . 82E+OO
1 . 1 811:+01
TC
9CK
7 . 1211:+02
2.7U+Ol
7 . 3911:+02
TC
9C
1 . 7 8E+ 0 2
4 . 2 7 11:+01
2 . 2 011:+02
y
9C
9 . 2 81:+ 0 2
1 . 5U+Ol
9.4411:+ 0 2
NB
95N
1.721:+03
4 . 0711:+ 0 0
1.7211:+ 0 3
1 . 3611:+02
NB
95
1 . 241!:+ 0 2
1 . 1 511:+ 0 1
TC
95N
9 . 7311:+01
1 . 3911:+ 0 1
1 . 1111:+02
TC
95
1 . 7 9E+OO
1 . 56E+01
1.7'&+ 0 1
y
95
1 . 01E+03
1 . 031!:+ 0 1
1 . 021:+ 0 3
ZR
95
1 . 1 7E+ 0 3
1 . 1111:+ 0 1
1 . 1 81: + 0 3
NB
96
1 . 45E+03
3. 62E+Ol
1.491!:+03
'l'C
9 611:
O . OOE+OO
2 . 6 9E+OO
2 . 6 91!:+ 0 0
TC
96
4 . 37E+OO
4 . 02E+Ol
4 . 4 6E+ 0 1
NB
9711:
2 . 121!:+01
1 . 09E+01
3 . 2 2 1: + 0 1
NB
97
1 . 3 01!:+ 0 3
9 . 9511:+ 0 0
1 . 311:+03
IW
97
8 . 941!:+01
7 . 4 91!:+ 0 0
9 . 6911:+ 0 1
TC
9711:
3 . 1 21!:+ 0 1
2 . 8 31!:+ 0 0
3.4011:+01
TC
97
0 . 0 01!:+ 0 0
4 . 03E+OO
4 . 0 3 11:+ 0 0
ZR
97
1.16E+03
2 . 531:+00
1 . 1 611:+ 0 3
NB
98
1 . 1 0 11!+ 0 3
3 . 4 61!:+ 0 1
1 . 1 31: + 0 3
TC
98
1 . 521!:+ 0 3
2 . HE+Ol
1.5411:+03
MO
99
l.35E+03
2 . UE+OO
1 . 3511:+03
1 . 391:+02
RH
99N
l . 26E+02
1 . 341!:+ 0 1
RH
99
8.4 5E+Ol
l . 32E+Ol
9 . 771:+01
TC
99N
2 . 59E+02
2 . 2 1E+OO
2 . 6111:+02
TC
99
l . 13E+ 0 3
O . OOE+OO
1 . 1311:+03
PO
100
8 . 0SE+OO
7 . 0 0E+OO
1 . 511:+01
RH
100
6 . 1211:+01
3 . 831!:+ 0 1
9 . 9511:+ 0 1
MO
101
1 . '1E+03
1 . 8 1E+Ol
1 . 4311:+03
PO
101
l . 28E+02
1 . 041:+01
1 . 3911:+ 0 2
RH
1 0 111:
2 . 19E+02
8 . 0SE+OO
2 . 2711:+02
RH
101
2 . 92E+02
8 . 0lE+OO
3 . 00&+02
TC
101
l . 32E+ 0 3
6 . 03E+OO
1 . 3311:+ 0 3
AG
102
7 . 32E+ 02
4". 7 1E+Ol
7.7911:+02
RH
1 0 211:
4 . 36E+02
9 . 43E+OO
4 . 4 6E+ 02
RH
102
l . 2 7E+Ol
3 . 4 8E+Ol
4 . 7511:+01
AG
103
5 . 05E+02
l . 3 0E+Ol
5 . 1 8E+02
PO
103
O . OOE+OO
3 . 30E+OO
3 . 3011:+00
RH
1 0 311
0. 0 0 11:+ 0 0
3 . 76E-01
3 . 7 611: - 0 1
IW
103
5 . 29E+02
7 . 331:+00
5 . 371:+02
AG
lOCK
4 . 2 61:+02
1 . 711:+01
4 . '311:+02
AG
104
2.201!:+02
4 . 0711:+01
2 . 6 111: + 0 2
- 26
-
2 . 2 811:+ 0 1
CD
104
1 . 531:+01
7 . '7B+OO
TC
104
9 . 681:+02
2 . 6111:+ 01
9 . 9 411:+ 02
AG
105
3 . 731:+01
l . 13E+Ol
4 . 8711:+ 0 1
RH
105
1 . 2311:+03
1 . 2211:+ 0 0
1 . 2 311:+ 0 3
RU
105
l . 35E+03
l . 18E+Ol
1. 3611:+03
6 . 4 211:+ 0 1
AG
106M
2 . l OE+Ol
4 . 32E+Ol
AG
106
6 . 52E+02
1 . 201:+01
6 . 6411:+02
RH
1 0 6M
l . 43B+03
4 . 201:+01
l . '71:+03
9 . 5 61:+02
RH
106
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3 . 23E+OO
3 . 2 7 11:+ 0 0
l'U
235
2 . 03E+OO
5 . 85E+OO
7 . 8 8 !:+ 00
u
235
9 . UE+Ol
C . 60E+OO
9 . 90E+Ol
2 3 6long
l . 30E+03
1 . 23E+Ol
1 . 311:+03
NP
2 3 6 short 6 . 42E+02
2 . 97E+OO
6 . CSE+02
l'U
236
2 . 07&-01
l . 05E+OO
1 . 25!:+ 0 0
NP
u
236
4 . 2 711: -01
8 . 98E-01
1 . 3311:+00
AM
2 37
8 . 03E+02
1 . 0511:+01
8 . 1311:+02
NP
237
2 . 7U:+Ol
5. 741:+00
3 . 3111:+01
l'U
237
1 . 141!:+00
C . 5511:+00
5 . 7 0 11:+ 0 0
u
237
1 . 041:+03
7 . 3211:+00
1 . 051!:+03
AM
238
3 . 83E+Ol
l . 73E+Ol
5 . 56E+Ol
CM
238
3 . 33E+OO
3 . 93E+OO
7 . 2 61!:+00
9 . 54!:+02
NP
238
9 . 44E+02
1 . 0 3E+Ol
l'U
238
2 . 6 4E-02
9 . l 7E - Ol
9 . UE - 0 1
u
238
O . OOE+OO
7 . 90E-01
7 . 9 0 11! - 0 1
AM
239
l . 22E+03
1 . lSE+Ol
l . 23E+03
NP
239
2 . 1 9!:+03
6 . 69E+OO
2 . 1 911:+03
l'U
239
o . ooz+oo
3 . Ull: - 0 1
3 . UE-01
u
239
1 . 33!:+03
1 . 961:+00
l . 3U:+03
AM
2CO
2 . 581!:+01
2 . 09!:+01
4 . 6711:+01
CM
240
O . OOE+OO
8 . 9211: - 0 1
8 . 921:- 01
NP
2 C OM
1 . 20E+03
8 . 141!+00
1 . 2111:+ 0 3
NP
240
2 . 82E+03
2 . 811:+01
2 . 8 51:+ 03
- 35 -
PU
240
6 . 26E-02
8 . 7311:-01
9 . 3611:-01
u
240
1 . 0411:+03
3 . 2811:+00
1 . 0411:+03
u
NAT
O . OOE+OO
0 . 0 0 11:+00
0 . 00E+OO
DI
241
5 . 92E-02
5 . 5511:+00
5 . 6111:+00
ex
241
6 . 14E+02
1 . 4 511:+ 01
6 . 29Z+02
PU
241
0 . 0011:+00
5. 4 011: - 0 4
5 . 4011: -04
DI
2 4 2N
2 . 3411:-04
1 . 9211:+00
1 . 9211:+00
DI
242
1 . 1511:+03
2 . 3811:+00
1 . 1511:+03
ex
242
1 . 4611:-05
8 . 0 811: - 0 1
8 . 0811:-01
PU
242
6 . 2111:-02
7 . 2511:- 0 1
7 . 8711: -01
DI
243
2 . 4111:-02
2 . 3311:+00
2 . 3511:+00
1 . 0711:+03
ex
243
1 . 0711:+03
6 . 2411:+00
PU
243
1 . 3311:+03
1 . 3311:+00
1 . 3311:+03
DI
2 4 41C
1 . 2711:+03
5 . 6911:-01
1 . 2711:+03
DI
244
2 . 5111:+03
1 . 8511:+01
2 . 5311:+03
a
244
0 . 0011:+00
7 . 1111:-01
7 . 1111: -01
ex
244
0 . 0011:+00
7 . 5111:- 0 1
7 . 5111:-01
PU
244
0 . 0011:+00
6 . 1 9 11: - 0 1
6 . 1 911:-01
DI
245
1 . 7811:+03
1 . 1411:+00
1 . 7811:+03
1 . 7311:+03
BK
245
1 . 7211:+03
8 . 5811:+00
ex
245
3 . 6011:+02
5 . 9511:+00
3 . 6611:+02
PU
245
2 . 0211:+03
8 . 3011:+00
2 . 0311:+03
DI
2 4 611
1 . 3911:+03
1 . 6011:+01
1 . 4011:+03
DI
246
4 . 0411:+03
1 . 8611:+01
4 . 0611:+03
BK
246
1 . 4811:+01
1 . 9311:+01
3 . 4111:+01
a
246
l . 75E-01
4 . 8 4 11: - 0 1
6 . 5811:-01
ex
246
0 . 0011:+00
6 . 6 811: -01
6 . 6811: -01
PU
246
6 . 85E+02
5 . 4 0 11:+00
6 . 9111:+02
BK
24 7
8 . 3411:+o2
2 . 7811:+00
8 . 3711:+02
ex
2'7
1 . 0911:+02
5 . 6811:+00
1 . 1511:+02
a
248
0 . 0011:+00
4 . 84 11:-01
4 . 8411:-01
ex
248
0 . 0011:+00
5 . 1 1 11: - 0 1
5 . 1111:-01
BK
249
1 . 5611:+01
1 . 8711: - 0 6
1 . 5611:+01
a
249
2 . 2811:+02
7 . 1 0 11:+ 0 0
2 . 3511:+02
ex
249
1 . 3911:+03
3 . 1311:-01
1 . 3911:+03
BK
250
1 . 40.&:+03
1 . 39.&:+0l
1 . 4211:+03
a
250
0 . 00.&:+00
4 . 6111:-01
4 . 61&-0l
ex
250
0 . 0011:+00
0 . 0011:+00
0 . 0011:+00
•s
250
l . 33E+Ol
8 . 52.&:+00
2 . 1811:+01
a
251
l . '7.&:+03
6 . 89.&:+00
l . '711:+03
ll:S
251
2 . 00E+02
4 . 76B+OO
2 . 051+02
a
252
l . 38E-01
4 . 411- 0 1
5 . 791-01
"'
252
0 . 0011:+00
3. 7 4 B -01
3 . 741-01
a
253
7 . 7111:+02
8 . 33B-03
7 . 711+02
ES
253
8 . 0311:-01
2 . 801-01
1 . 081+00
"'
253
1 . 6811:+02
3 . 601+00
1 . 7211:+02
a
254
0 . 0011:+00
1 . 5011: - 0 3
1 . 5011:- 0 3
ES
25.UC
1 . 3311:+03
8 . 441+00
1 . 341+03
ES
254
2 . 2511:-04
5 . 7011:+00
5 . 701+00
"'
254
7 . 39E-02
3 . 95B-Ol
4 . 691-01
"'
255
1 . 7 411: - 0 2
4 . 7 4 11:+ 0 0
4 . 751+00
"'
257
6 . 43E+02
5 . 42E+OO
6 . 4911:+02
MD
257
2 . 46E+Ol
3 . 6811:+00
2 . 83B+Ol
MD
258
3 . 60E-04
1 . 6411:+00
l . 64E+OO
l!al
89
8 . 83B+02
2 . 3311:+01
9. 06B+02
XE
1 37
8 . 98E+02
2 . 84B+OO
9 . 00B+02
lCY
999M
0 . 0011:+00
0 . 0011:+00
0 . 001+00
- 36 -
Appendix
Table A 2
Dose equivalent at 1 0 mm depth in the ICRU sphere at the main axis,
H' ( l O) , for radionuclides emitted from point sources at a distance of
100 cm from the surface of the sphere.
The <loses are given in mSv
·
h-1 • GBq-1•
- 37
11.lement
z
11.lectron
Contribution
-
Photon
Sum
Contribution
B
3
O . OOE+OO
6 . 9111. - 0 9
6 . 9111-09
B&
7
0 . 00E+OO
7 . 761-03
7 . 76&-03
B&
10
O . OOE+OO
0 . 00&+00
0 . 0011:+00
c
11
4 . 761:-08
1 . 60&-0l
1 . 6011.-01
N
13
4 . 21&-0 6
1 . 6011.-01
1 . 60&-0l
c
14
O . OOE+OO
0 . 0011.+00
0 . 0011.+00
0
15
2 . 4911.-04
1 . 6111.-01
1 . 6111.-01
1 . 6011.-01
r
18
O . OOE+OO
1 . 6011.-01
N&
19
4 . 28&-03
1 . 6211.-01
1 . 66&-0l
IQ
22
4 . 74&-07
3 . 3011.-01
3 . 3011.-01
5 . 061-01
3 . 82& - 0 1
IQ
2•
5 . 9811.-05
5 . 0511.-01
AL
26
5 . 391:-06
3 . 8211.-01
AL
28
7 . 16E-02
2 . UE-01
3 . 1511.-01
lfG
28
O . OOE+OO
2 . 141:- 01
2 . lU-01
p
30
2 . llE-01
1 . 6011.-01
3. 7111.-01
SI
31
• . 491:-05
1 . 3011.-04
1 . 751:-0•
1 . !1711.-04
p
32
1 . 971:-04
0 . 00&+00
SI
32
O . OOE+OO
0 . 0011.+00
0 . 00E+OO
p
33
O . OOE+OO
0 . 0011.+00
O . OOE+OO
s
35
O . OOE+OO
0 . 00&+00
0 . 00&+00
CL
36
O . OOE+OO
2 . 3711.-05
2 . 37&-05
AR
37
0 . 00&+00
4 -. 1 8& -09
4 . 1811.- 0 9
CL
38
1 . 35E+OO
1 . 9611.-01
1 . 551:+00
lt
38
4 . 59E-02
4 . 3U-01
4 . 8 0 1: - 0 1
AR
39
O . OOE+OO
1 . 87&- 0 4
1 . 871:-04
CL
39
3 . 13E-02
2 . 1 0 11.-01
2 . 4111.-01
lt
40
2 . 09E-05
2 . 241:-02
2 . 2411.-02
AR
41
1 . 631:-04
1 . 8 8 1: - 0 1
l . 8 8& - 0 1
CA
41
0 . 00&+00
3 . 8 6 11. - 0 8
3 . 8611.-08
lt
42
4 . 2511.-01
3 . 921:-02
4 . 641:-01
1 . 5211.-01
lt
43
7 . 951:-06
1 . 52&-01
SC
'3
1 . 021:-06
1 . 741:-01
1 . 7411.-01
lt
"
1 . 261:+00
2 . 89 11.- 01
1 . 55&+00
4 . 4711.-02
SC
UM
O . OOE+OO
4 . 47&-02
SC
"
4 . 261:-05
3 : 241:-01
3 . 2U-01
n
"
O . OOE+OO
2 . 5711:-02
2 . 57&-02
CA
45
O . OOE+OO
2 . 0U:- 0 8
2 . 01&- 0 8
lt
45
4 . 76E-02
2 . 54E-01
3 . 0211:-01
TI
45
4 . 23E-07
l . 36E-01
1 . 361:-01
SC
46
1 . 99E-09
2 . 991:-01
2 . 991:-01
CA
47
2 . 071:-04
1 . 561:-01
1 . 5611.-01
SC
47
O . OOE+OO
1 . 701:-02
1 . 7011.-02
V
47
7 . 36E-04
l . 55E-Ol
1 . 561-01
CR
'8
· 0 . 001:+00
7 . 1411.-02
7 . lU-02
SC
'8
6 . 7 51: - 0 4
4 . 9511.-01
4 . 95&-0l
V
'8
1 . 77E - 0 6
4 . 321:-01
4 . 3211:-01
CA
49
3 . 55E-03
3 . 23E-01
3 . 2 711:-01
CR
49
5 . 13E-05
1 . 66E-01
1 . 661:-01
SC
49
l . 26E- 0 3
l . UE -04
1 . 4111. -03
V
49
O . OOE+OO
6 . 8511:-07
6 . 851:-07
CR
51
O . OOE+OO
5 . 191:-03
5 . 191:-03
MN
51
3 . 62E-03
1 . 5511:-01
1 . 591:-01
FE
52
O . OOE+OO
1 . 161:-01
1 . 1 6 11: - 0 1
-
38
-
MN
52X
3 . 02E- 0 2
3 . 58E-Ol
3 . 8 9E - 0 l
MN
52
l . 50E-07
5 . 1 0 11: - 0 l
5 . 1 0 11: - 0 l
MN
53
O . OOE+ O O
3 . 6 411: - 0 6
3 . 6 411: - 0 6
MN
54
O . OOE+OO
1 . 2611:-01
l . 26E-01
CO
55
2 . 57E-05
3 . 02E-Ol
3 . 0 2 11: - 0 1
r11:
55
0 . 0011:+00
7 . 9111:-06
7 . 9 1 11: - 0 6
CO
56
7 . 7211:- 0 6
4 . 8 5 11: - 0 1
4 . 8 5 11: - 0 1
MN
56
3 . 6 9:&: - 0 2
2 . 3 8 11: - 0 1
2 . 75&-0l
NJ:
56
5 . 8 7 11: - 0 8
2 . 6011:-01
2 . 60&-0l
CO
57
0 . 00&+00
2 . 1 1 11:- 02
2 . 1 111: - 0 2
NI
57
0 . 00&+00
2 . 7 811: - 0 1
2 . 7 811: - 0 1
CO
58X
o . ooa:+oo
3 . 7 811: - 0 5
3 . 7 811: - 0 5
CO
58
9 . 43:&:-11
1 . 4711:-01
1 . 4711:- 0 1
n:
59
1 . 7 811: - 0 7
1 . 7511:-01
1 . 7 5 11: - 0 1
NJ:
59
0 . 00:&:+00
3 . 3611:-05
3 . 3 6 11: - 0 5
CO
60X
1 . 5311:-07
8 . 1'&-04
8 . 1 4&-04
CO
60
2 . 2111: - 0 7
3 . 6611:-01
3 . 6611:- 0 1
5 . 9611: - 0 1
CU
60
5 . 1 8 11: - 0 2
5 . 4 411: - 0 1
n
60
0 . 00&+00
0 . 0011:+00
0 . 0011:+00
CO
CU
61
5 . 03:&: - 0 6
1 . 6 711: - 0 2
1 . 6 7 11: - 0 2
61
2. 9911: - 0 6
1 . 28&-0l
1 . 2 811: - 0 1
CO
62X
5 . 05 & -02
3 . 8511:-01
4 . 3 6 11: - 0 1
CU
62
9 . 1 411: - 0 2
1 . 5711:-01
2 . 4 911: - 0 1
ZN
62
0 . 0011:+00
7 . 0 111:- 0 2
7 . 0 111: - 0 2
111:
63
0 . 0011:+00
0 . 0011:+00
0 . 0 011:+ 0 0
ZN
63
6 . 5 111:- 0 3
1 . 69&-01
1 . 7 5 11: - 0 1
64
0 . 0011:+00
2 . 9611:-02
2 . 96&-02
GA
65
2 . 4 0 11: - 0 3
1 . 8 1 11: - 0 1
1 . 8 3 11: - 0 1
NI
65
1 . 4 7 11: - 0 3
7 . 96&-02
8 . 1 0 11: - 0 2
ZN
CU
65
1 . 5 6& - 0 8
8 . 6111: - 0 2
8 . 6111: - 0 2
66
2 . 60&-02
1 . 2 6 11: - 0 2
3 . 8.511: - 0 2
GA
66
5 . 68&-01
3 . 09 & - 01
8 . 77& -01
GE
66
4 . 1511:- 0 8
1 . 0 811: - 0 1
1 . 0 8 11: - 0 1
NI
CU
66
0 . 00:&:+00
o . ooa:+oo
0 . 0 0 11:+ 0 0
67
0 . 0 0 :&:+ 0 0
1 . 82&-02
1 . 8 2 E - 02
GA
67
o . ooa:+oo
2 . 5 3E - 0 2
2 . 53&-02
Gll:
67
1 . 94&-01
2 . 13:&:-01
4 . 0 7 :&: - 0 1
GA
68
6 . 5111: - 0 4
1 . 48E-01
1 . 4 9E - 0 1
Gll:
68
0 . 00&+00
4 . 1 1 1\ - 0 4
4 . 1111: - 0 4
AS
69
g . 1 811: - 0 2
l . 58E-01
2 . 5 0 11: - 0 1
Gll:
6 !1
1 . 6 0 :&: - 0 6
l . 32E - 0 1
1 . 32:&:-01
ZN
69X
0 . 0011:+00
6 . 6 6 & - 02
6 . 6 6& - 0 2
ZN
69
1 . 4 7 11: - 1 1
!1 . 5 711: - 0 7
!1 . 5 7 11: - 0 7
CU
AS
70
7 . 50&-03
5 . !1 5 E - 0 1
6 . 03&-01
GA
70
1 . 27:&:-04
1 . 1 3:&: - 0 3
1 . 2 6& - 0 3
Sll:
70
5 . 4 1 1\ - 0 5
1 . 58:&:- 0 l
1 . 58&-01
AS
71
0 . 00:&:+00
8 . 7 8:&: - 0 2
8 . 7 811: - 0 2
GE
71
O . OOE+OO
4 . 16E-04
4 . 1 6& - 0 4
ZN
7 1X
2 . 57& - 0 4
2 . 40E-01
2 . 4 0E - 0 1
AS
72
7 . 0 1 1\ - 0 2
2 . 6!1&-01
3 . 3 9 1: - 0 1
GA
72
1 . 7 8:&: - 0 2
3 . 6 811:- 01
3 . 8 6E - 0 1
ZN
72
O . OOE+ O O
2 . 57&- 0 2
2 . 57&-02
AS
73
O . OOE+OO
3 . 12E-03
3 . 12E-03
GA
73
6 . 1 4 :&: - 0 6
5 . 1 9 1: - 0 2
5 . 1 91: - 0 2
SE
73X
5 . 7 0 :&: - 0 5
3 . 8 0 11: - 0 2
3 . 80E-02
SE
73
8 . 2 5 :&: - 0 6
1 . 7 0 :- 01
l . 74E-01
AS
74
7 . 36E-06
1 . 17E-01
1 . 1 7 11: - 0 1
BR
74X
7 . 97&-0l
5 . 50E-Ol
l . 35E+OO
BR
74
4 . 651: - 0 1
5 . 5 6 1: - 0 1
l . 02E+OO
D
74
1 . 811\-0 3
1 . 8311:-01
1 . 8 5 11: - 0 1
- 39 -
BR
75
1 . 44&-0'
l . 89 E - 01
1 . 89&-01
G&
75
2 . 2611:-06
5. 50&-03
5 . 50&-03
sz
75
o . ooa:+oo
6. ' 0 & - 02
6 . ,0&-02
AS
76
6 . 72&-02
6. 44&-02
1 . 32&-01
BR
76
1 . ,711:-01
3 . 57&-01
5 . 03&-0l
KR
76
0 . 00&+00
7 . 35&-02
7 . 35&-02
AS
77
0 . 00&+00
1 . 39&-03
1 . 39&-03
BR
77
0 . 00&+00
5 . 07&-02
5 . 07&-02
G&
77
2 . UE-03
1 . 60&-01
1 . 63&-0l
KR
77
3 . 62&-0'
1 . 60&-01
1 . 60&-01
S&
77M
o . ooa:+oo
l . '3&-02
l . ,3&-02
AS
78
6 . 23&-0l
1 . 81&-01
8 . 0U-01
G&
78
0 . 00&+00
, . 53&-02
, . 53&-02
KR
79
0 . 00&+00
, . 2U-02
, . 2u-02
RB
79
' . 8 8111 - 0 3
2 . 1 2& - 01
2 . 17&-0l
SS
79
0 . 00&+00
0 . 00&+00
0 . 00&+00
BR
80M
0 . 00&+00
l . 20•-02
1 . 2011:-02
BR
80
8 . 83&-0'
1 . 23&-02
1 . 32&-02
RB
80
1 . 55&+00
l . 9U-Ol
l . 7U+OO
SR
80
O . OOE+OO
7 . , 8& - 0 3
7 . ' 8& - 0 3
KR
81M
0 . 001!:+00
2 . 1'&-02
2 . lU-02
KR
81
O . OOE+OO
, . 17&-03
, . 17&-03
RB
81M
0 . 00&+00
6 . 241!: - 0 3
6 . 241:- 03
RB
81
1 . 72&-07
1 . 0 1 1 -01
1 . 011 - 01
S&
81M
l . '3&-09
3 . 9511:-03
3 . 95&-03
S&
81
7 . 911-05
l . ,5&-03
1 . 53&-03
SR
81
3 . 23&-02
2 . 15&-0l
2 . ,7&-01
BR
82
0 . 00&+00
3 . 95&-0l
3 . 95&-01
RB
82M
3 . 1 7 & -0 6
, . 36&-01
, . 361:-01
RB
82
2 . 57&-01
1 . 70&-01
, . 27&-01
SR
82
0 . 0 01!!+ 00
7 . 3 61!! - 0 3
7 . 361:- 03
BR
83
1 . 5711:-09
1 . 1 7 1: - 03
1 . 17&-03
KR
83K
O . OOE+OO
1 . 5711:-03
1 . 57&-03
RB
83
o . ooa:+oo
8 . 201:-02
8 . 2011:-02
SE
83
6 . 8111:-03
3 . 5 51!! - 0 1
3 . 62&-01
SR
83
l . l 7&-06
1 . 27&-01
1 . 27&-01
BR
8,
7 . 02&-0l
2 . 21&- 0 1
9 . 2311:-01
RB
8'
2 . 08&-05
l . UE - 0 1
l . UE-01
KR
85M
O . OOE+OO
2 . 5 7111 - 0 2
2 . 57&-02
KR
85
0 . 00&+00
5 . 7 81: -0,
5 . 78&-0'
SR
8 5M
0 . 00&+00
3 . 511:-02
3 . 511-02
SR
85
O . OOE+OO
8 . 55E-02
8 . 5511:-02
RB
86
3 . 661:-0,
l . ,OE-02
1 . 441:-02
y
86K
2 . 811:-07
3. 4 '11:-02
3. UZ-02
y
86
, . 67111 - 0 3
5 . 1 0 11:- 01
5 . 1511:-01
6 . 93&-02
ZR
86
O . OOE+OO
6 . 93&-02
KR
87
3 . 9211:-01
1 . 09E- 01
5. 011-01
RB
87
0 . 00&+00
0 . 00&+00
0 . 00&+00
SR
87K
0 . 00&+00
5 . 33&-02
5 . 33&-02
y
87
0 . 0 01!!+ 00
7 . 9711:-02
7 . 97&-02
KR
88
1 . 5011:-02
2 . ,9&-01
2 . 6U-01
NB
88
8 . 611:-02
6 . 33&-0l
7 . 19&-0l
RB
88
2 . 22Z+OO
9 . 0 8 11: - 0 2
2 . 311+00
y
88
5 . 0611:-06
3 . 801!:- 0l
3 . 80&-01
ZR
88
0 . 0 01!!+ 00
7 . 62Z-02
7 . 62&-02
NB
89ahort 7 . 4 51!! - 0 3
2 . 991!:-01
3 . 06&-01
NB
89long
l . 97Z-01
1 . 9611:-01
3 . 92&-0l
RB
89
3 . 75Z-01
2 . 8 31!! - 0 l
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90
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92
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93
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94
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94
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97
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97
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97
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98
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98
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99
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101
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142
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142
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142
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143
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143
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143
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143
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144
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145
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145
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145
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145
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145
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146
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146
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146
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146
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147
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147
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147
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147
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147
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147
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147
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148
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148
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151
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151
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151
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159
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193
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199
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199
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200
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202
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203
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BI
205
2 . 4 2& - 0 5
2 . 3 9 & - 0l
2 . 39&-01
PB
205
0 . 00&+00
6 . 57&-04
6 . 57&-04
PO
205
2. 05&-06
2 . 3 311: - 0 1
2 . 33&-01
BI
206
2 . 57& - 0 6
4 . 87&-0l
4 . 87&-01
'l'L
206
4 . llE-05
1 . 9111: - 0 5
6 . 02&- 0 5
A'l'
207
1 . 3 0 11: - 0 6
1 . 98&-0l
l . 98&-01
BI
207
9 . 16&-06
2 . 33&-01
2 . 33&-01
PO
207
4 . 1 4 11: - 0 6
2 . 0 1 11: - 0 1
2 . 0 1 11: - 0 1
'l'L
207
l . 9 1 11: - 0 5
3 . 32&-04
3 . 5 1 11: - 0 4
'l'L
208
2 . 86&-03
4 . 1 6& - 0 1
4 . 1 9& - 0 1
PB
209
0 . 00&+00
0 . 0011:+00
0 . 00& + 00
'l' L
209
3 . 26&-04
2 . 9 6 & - 01
2 . 96&-0l
BI
2 1 0M
0 . 00&+00
4 . 1 911:- 02
4 . 1 911: - 0 2
BI
210
1 . 6711: - 0 6
0 . 0011:+00
1 . 671:- 0 6
PB
210
0 . 0 0 11:+ 0 0
2 . 5 6 11: - 0 3
2 . 56&-03
l . 2 8& - 0 6
PO
210
O . OOE+OO
l . 2 811: - 0 6
AT
211
O . OOE+ O O
8 . 23 11:- 03
8 . 23& - 03
BI
211
O . OOE+OO
7 . 7 2E- 03
7 . 72& - 0 3
PB
211
1 . 1 9 11: - 0 5
7 . 79E-03
7 . 8 0& - 0 3
PO
211
O . OOE+ O O
1 . 1 811: - 0 3
1 . 1 81: - 0 3
BI
212
1 . 58E-03
2 . 7611:-02
2 . 9211: - 02
PB
212
O . OOE+OO
2 . 5 0 11: - 0 2
212
o . o p 11:+0 0
2 . 5 011:- 02
PO
BI
213
1 . 2 1 11: - 0 5
PO
213
0 . 00&+00
0 . 0011:+00
0 . 0 0 11:+ 0 0
BI
214
3 . 04E-02
2 . 0 8 11: - 0 1
2 . 39&-0l
PB
214
l . 3 1 11: - 0 8
4 . 14&-02
4 . 1 4 11: - 02
PO
214
0 . 0011:+ 0 0
l . 2 6 11: - 0 5
l . 26E-05
A'l'
215
O . O O E+ O O
3 . l2E - 0 5
3 . 121!- 0 5
PO
215
O . OOE+OO
2 . 821! - 0 5
2 . 82&-05
A'l'
216
0 . 00E+ O O
3 . 0 0 11: - 0 4
3 . 0 0 11: - 0 4
PO
216
0 . 00E+ O O
2 . 551!- 0 6
2 . 5511:- 0 6
A'l'
217
0 . 00E+OO
4 . 8 1 11: - 0 5
4 . 8 1 11: - 0 5
A'l'
218
O . OOE+OO
3 . 0 7 11: - 0 3
3 . 07&-03
PO
218
O . OOE+OO
1 . 37&-06
1 . 3711:- 0 6
RN
218
O . OOE+ O O
1 . 1 611: - 0 4
1 . 1 611: - 0 4
FR
219
0 . 001!+00
5 . 6 9 11:- 04
5 . 6 9 11: - 0 4
RN
219
O . OOE+OO
FR
220
O . OOE+OO
9 . 1 111: - 0 3
·
3. 0 8 11: - 0 3
3 . 0 8 11: - 0 3
RN
220
0 . 0 0 11:+ 0 0
5 . 9 7 1: - 0 5
5 . 9 7 11: - 0 5
FR
221
0 . 00E+ O O
5 . 0 7 11: - 0 3
5 . 0711:- 0 3
FR
222
9 . 83E-04
O . OOE+OO
9 . 8 311: - 0 4
RA
222
0 . 00E+ O O
1 . 5 1 11: - 0 3
1 . 5 1 11: - 0 3
0 . 0011:+00
0 . 0011:+ 0 0
2 . 12&-02
2 . 12& - 02
9 . llE-03
RN
222
0 . 00E+ O O
6 . 2311: - 0 5
6 . 2 3 11: - 0 5
AC
223
0 . 0011:+00
2 . 1 7 11: - 0 3
2 . 1 7 11: - 0 3
FR
223
5 . 6 5E - 0 7
1 . 681!-02
1 . 6 8 11: - 0 2
RA
223
O . OOE+OO
2 . 4311:-02
2 . 4 3 11: - 0 2
-
49 -
AC
224
O . OOE+OO
3 . 8 11: - 0 2
3 . 8 1 1: - 0 2
RA
224
0 . 0 0 11:+ 0 0
1 . 6 0 1: - 0 3
1 . 6 0 1: - 0 3
AC
2 25
0 . 0 0 &: + 0 0
4 . 9 6 1: -0 3
4 . 9 6 11 - 0 3
RA
2 25
0 . 0 011+00
7 . 3 311 - 0 3
7 . 331: - 0 3
AC
226
2 . 4 0 1: - 0 7
2 . 4 011 -0 2
2 . 401:- 02
RA
226
0 . 0011+00
1 . 1 411: - 0 3
1 . 1411: - 0 3
TH
226
0 . 0 0 11:+ 0 0
2 . 4 91: - 0 3
2 . 4 911: - 0 3
AC
227
O . O Oa:+OO
1 . 4 5 1: - 0 4
1 . 4 5 1: - 0 4
PA
227
O . O OE+OO
6 . 7 0 1: - 0 3
6 . 701:- 0 3
RA
227
3 . 3 6 1: - 0 6
3 . 821:-02
3 . 8 211: - 0 2
TH
227
0 . 0 0&:+00
2 . 3311-02
2 . 331:-02
AC
228
1 . 371:- 0 4
1 . 4 5 1: - 0 1
1 . 4 5 1: - 0 1
PA
228
7 . 5 1 1: - 1 0
1 . 6 811: - 0 1
1 . 6811: - 0 1
RA
228
0 . 001:+00
4 . 001:-11
4 . 0 0 1: - 1 1
TH
228
0 . 0 0 11:+ 0 0
1 . 8411-.03
1 . 8 4 1: - 0 3
TB
229
0 . 0 0 11:+ 0 0
2 . 661:-02
2 . 661:-0 2
PA
230
3 . 7 4 11: - 0 9
1 . 0 811: - 0 1
1 . 0 811: - 0 1
TB
230
0 . 0 0 11:+ 0 0
1 . 4 1 1: - 0 3
1 . 4 1 1: - 0 3
0
230
0 . 00&:+ 0 0
2 . 5 7 1: - 0 3
2 . 5 7 1: - 0 3
PA
23 1
0 . 0011+00
2 . OOB-02
2 . 0 01: - 0 2
TB
23 1
O . OOE+OO
1 . 9 411: - 0 2
1 . 9 4 1: - 0 2
0
23 1
O . OOB+OO
3 . 221: - 0 2
3 . 221:-02
NP
232
1 . 0 5 1: - 0 7
1 . 9 91: - 0 1
1 . 991:- 01
PA
232
8 . 95&-08
1 . 511:- 0 1
1 . 511:-01
TB
232
0 . 0 0 11:+ 0 0
1 . 3 5 1: - 0 3
1 . 351:- 0 3
0
232
0 . 0011+00
2 . 471:- 0 3
2 . 4 7 1: - 0 3
NP
233
0 . 001:+00
2 . 231:-02
2 . 231:-02
PA
233
0 . 0 011+00
4 . 1 4 1: - 0 2
4 . 1411: - 02
0
233
0 . 0 0&:+00
1 . 3 0 1: - 0 3
1 . 3 0 1: - 0 3
NP
23 4
2 . 42E-05
2 . 1 91: - 0 1
2 . 1 91: - 0 1
PA
234X
3 . 5 11: - 0 3
1 . 7 6& - 0 3
5 . 2 7 1: - 0 3
PA
234
5 . 3 9 E-07
2 . 8 1 11 - 0 1
2 . 8 1 1: - 0 1
PO
23 4
O . O OE+OO
1 . 85&-02
1 . 8 51:- 02
3 . 371: - 0 3
TH
23 4
0 . 00E+OO
3 . 371:-03
TB
NAT
0 . 0011+00
0 . 001:+0 0
0 . 0 0&:+0 0
0
234
O . OOE+OO
2 . 03&-03
2 . 0 3 1: - 0 3
NP
235
O . OOE+OO
8 . 2 411: - 0 3
8 . 2 411: - 0 3
PO
235
O . O OE+OO
2 . 631:-02
2 . 631:-02
2 . 8 411: - 0 2
235
0 . 0011+00
2 . 8 411: - 0 2
NP
2 3 6long
O . O OE+OO
4 . 6 411: - 0 2
4 . 6 4 11: - 0 2
NP
23 6short
O . OOE+OO
l . 32E-02
1 . 321:-02
PU
236
0 . 00&+00
2 . 7 0 1: - 0 3
2 . 7 0 11 - 0 3
0
23 6
0 . 00E+OO
l . 89E-03
1 . 8 91: - 0 3
AH
237
O . OOE+OO
7 . 271:-02
7 . 2 71:-02
1 . 811:-02
u
NP
237
0 . 00E+OO
1. 811:-02
PO
237
O . OOE+OO
1 . 8 01: - 0 2
1 . 8 0 1: - 0 2
0
237
O . OOE+OO
3 . 7 01! -02
3 . 7 0 1: - 0 2
AH
238
1 . 70&-06
1 . 4 5 1: - 0 1
1 . 451:- 0 1
CM
238
0 . 0 01!+00
2 . 05&-02
2 . 0 5 1: - 0 2
NP
238
1 . 8 0 11 - 0 6
8 . 90&-02
8 . 9 0 1: - 0 2
PU
238
O . OOE+OO
2 . 351: - 0 3
0
238
O . OOE+OO
2 . 351!- 03
·
1 . 66&-03
AH
23 9
O . OOE+OO
5 . 95E-02
5 . 95& - 02
NP
239
O . OOE+OO
3 . 93&-02
3 . 9 3 1: - 0 2
PO
239
O . OOE+OO
8 . 90E-04
8 . 90&-04
u
239
2 . 81E-06
1 . 2 411: - 0 2
1 . 251:-02
AH
240
1 . 12E - 0 7
1 . 7 1 11 - 0 1
1 . 711:- 0 1
CM
240
0 . 00E+OO
2 . 6 9 1! - 0 3
2 . 69&-03
IJIP
2 4 0N
8 . 94E-04
5 . 9 6 E-02
6 . O U : - 02
NP
240
O . O O E+ O O
2 . 25 & -0 1
2 . 251:- 01
1 . 6 6 11 - 0 3
- 50 -
PU
240
O . OOE+OO
2 . 2 411: - 0 3
2 . 2 411: - 0 3
u
240
0 . 0011:+00
9 . 3211:-03
9 . 3 2 11: - 0 3
u
HAT
0 . 0011:+00
O . OOE+OO
0 . 0 011:+00
AM
241
0 . 0011:+00
1. 93&-02
1 . 93&-02
CM
241
0 . 0011:+00
9 . 96&-02
9 . 96&-02
PU
241
0 . 0 01!+00
1 . 56S- 0 6
l . 56&-06
AM
2 4 2H
0 . 001! +00
6 . 41&-03
6 . 41&-03
AM
242
0 . 00&+00
9 . 37&- 0 3
9 . 37&-03
2 . 4 3& - 0 3
CM
242
0 . 00&+00
2 . 43&- 0 3
PU
242
0 . 0 01!+00
l . 86 &- 03
l . 8 6& - 0 3
AM
243
0 . 00&+00
1 . 45&-02
l . 45&-02
CM
243
0 . 00&+00
3 . 29&-02
3 . 29&-02
PU
243
0 . 0 0&+00
7 . 30&-03
7 . 30&-03
AM
2.UK
2 . 87&-05
2 . 04&-03
2 . 07&-03
AM
244
0 . 00&+00
l . 45&-01
1 . 45&-01
cr
244
0 . 00&+00
2 . 5 5& - 0 3
2 . 55&-03
CM
244
0 . 0 0&+00
2 . 26&-03
2 . 26&-03
PU
244
0 . 001!+0 0
1 . 59&- 0 3
1 . 59&-03
AM
245
0 . 00&+00
1. 30&-03
7 . 30&-03
Bit
245
0 . 0 01! +00
5 . 41&-02
5 . 41&-02
CM
245
O . O OE+OO
2 . 7 5 1! - 0 2
2 . 75K-02
PU
245
3 . 16&-07
7 . 02&-02
7 . 02&-02
AM
2 4 6K
2 . 5 2& - 0 4
1 . 53&-0l
1 . 54&-01
AM
246
9 . 35&- 0 7
1 . 35&-0l
1 . 35&-01
Bit
246
2 . 07&-07
1 . 6 1&-01
1 . 61&- 0 1
cr
246
0 . 00&+00
1 . 74&-03
1 . 74&-03
CM
246
0 . 0 0&+00
2 . 01&-03
2 . 0lK-03
PU
246
0 . 00&+00
3 . 40&-02
3 . 4 0&- 02
Bit
247
0 . 00&+00
2 . ll&-02
2 . llE - 02
CM
247
0 . 00E+OO
5 . 28E-02
5 . 2 8 11: - 0 2
cr
248
0 . 00E+OO
1 . 7411:-03
l . 7 411: - 0 3
CM
248
O . OOE+O O
1 . 5 4 11: - 0 3
1 . 54&-03
Bit
249
O . O OE+OO
1 . 54E-08
1 . 5 4 11: - 0 8
er
249
0 . 001! +00
6 . 0411:-02
6 . 04&-02
CM
249
0 . 00E+OO
3 . 02 1!- 03
3 . 02&-03
Bit
250
l . 91&-05
1 . 37E-01
1 . 3 7 1! - 0 1
1 . 6 5 1! - 0 3
a
250
O . OOE+OO
1 . 65E - 0 3
CM
250
0 . 001!+00
O . OOE+OO
0 . 0 01+00
&S
250
6 . 9 5 1! - 0 8
7 . 1 0&-02
7 . l O E - 02
cr
251
0 . 001! +00
3 . 6911:-02
3 . 6911:-02
&S
251
O . OOE+OO
2 . 81& -02
2 . 81K-02
a
252
O . OOE+O O
1 . 5 9& - 0 3
1 . 59&-03
nc
252
O . OOE+OO
1 . 521!-03
1 . 52 11: - 0 3
a
253
0 . 00E+OO
3 . 0lE-05
3 . 0 1 1! - 0 5
ES
253
0 . 00E+OO
1 . lOE-03
1 . lOE-03
nc
253
0 . 001!+00
2 . 27E-02
2 . 27&-02
Cl'
254
0 . 00E+OO
5 . 38E-06
5 . 38&-06
ES
2 5 4M
3 . 8 9E - 0 7
7 . 7 2 E- 02
7 . 7 2 11: - 0 2
2 . 1 411: - 0 2
ES
254
0 . 001!+00
2 . 1 411: -02
nc
254
0 . 001!+00
1 . 62E-03
1 . 6 2 1! - 0 3
nc
255
O . OOE+OO
1 . 631:-02
1 . 631:-02
nc
257
0 . 001:+00
3 . 1 8& - 0 2
3 . 1 81: - 02
.ICD
257
O . OOE+OO
2 . 66B-02
2 . 661:-02
.ICD
258
O . OOE+OO
7 . 4 01! - 0 3
7 . 4 01! - 0 3
KR
89
1 . 80E+OO
2 . 43E-01
2 . 0 51+00
XE
137
1 . HE+OO
2 . 911!-02
l . 17E+OO
XY
999M
O . OOE+OO
O . OOE+OO
0 . 0 0 1+00
- 51 -
App endix
Table A3
Dose equivalent H'(0.07) from skin contamination i n mSv·h-1 ·kB q - 1 ·cm2•
- 52 -
Element
z
Electron
Contribution
Photon
Sum
Contribution
R
3
0 . 0011:+00
6 . 4 9&-07
6 . 4911:-07
B&
7
1 . 3811:-07
3 . 33&-03
3 . 33&-03
B&
10
1 . 6211:+00
0 . 00&+00
1 . 62&+00
c
11
l . 65E+OO
6 . 96&-02
1 . 7211:+00
N
13
1 . 6611:+00
7 . 02&-02
1 . 7311:+00
c
14
3 . 03E-01
0 . 00&+00
3 . 0311:- 01
0
15
1 . 64&+00
7 . 06&-02
1 . 71&+00
r
18
l . 63E+OO
6 . 961:-02
1 . 70&+00
NI:
19
l . 64E+OO
7 . ll&-02
1 . 71&+00
NA
22
l . U&+OO
1 . 45&-01
1 . 59&+00
NA
24
1 . 63&+00
2 . 35&-01
l . 86&t00
AL
26
1 . 36&+00
1 . 6811:-01
1 . 52&+00
AL
28
1 . 6311:+00
1 . 07&-01
1 . 73&+00
IG
28
1 . 32&+00
9. 24&-02
1 . 41&+00
p
30
1 . 64E+OO
6 . 97&-02
1 . 71&+00
SI
31
1 . 62&+00
5 . 75&-05
1 . 62&+00
p
32
1 . 62&+00
0 . 00&+00
1 . 62&+00
SI
32
6 . 02E-01
0 . 00&+00
6 . 02&-01
p
33
7 . 76&-01
0 . 00&+00
7 . 76&-01
s
35
3 . 24E-01
O . OOE+OO
3 . 24&-01
CL
36
1 . 52&+00
1 . 03&-05
1 . 52&+00
AR
37
O . OOE+OO
0 . 00&+00
0 . 00&+00
CL
38
1 . 66&+00
8 . 77&-02
1 . 75&+00
lt
38
1 . 62&+00
1 . 94&- 0l
1 . 82&+00
AR
39
1 . 4SIE+00
2 . 45&-04
1 . 49&+00
CL
39
1 . 62E+OO
9 . 16&-02
1 . 72&+00
lt
40
1 . UE+OO
9. 85&-03
1 . 45&+00
AR
41
1 . 61E+OO
8 . 36&-02
1 . 701:+00
CA
41
O . OOE+OO
o . ooz+oo
0 . 00&+00
lt
42
1 . 64E+OO
1 . 72&-02
1 . 66&+00
lt
43
l . 55E+OO
6 . 5611:-02
1 . 621:+00
SC
43
1 . 35E+00
7 . 41&-02
1 . 421:+00
lt
44
1 . 66E+OO
l . 34&-01
1 . 80&+00
SC
UM
2 . 12E-01
1 . 7811:-02
2 . 301:-01
SC
44
1 . 57&+00
1 . t3&-01
1 . 71&+00
'l'I
u
7 . 16&-03
7 . 56&-03
1 . 47&-02
CA
45
7 . 8011:-01
4 . 65s-o8
7 . 80&-01
lt
45
1 . 63&+00
1 . 1211:-01
1 . 7411:+00
'l'I
45
1 . 4311:+00
5 . 93&-02
1 . 4SIZ+OO
SC
46
l . lOE+OO
1 . 35&-01
1 . 241:+00
CA
47
l . 52E+OO
6 . 8911:-02
1 . 59&+00
SC
47
1 . 33E+OO
6 . 0411:-03
1 . 34E+OO
V
47
1 . 59E+OO
6 . 7611:-02
1 . 66&+00
CR
48
5 . 45E-02
2. 6711:-02
8 . 12&-02
SC
48
1 . 47E+OO
2 . 22&-01
1 . 69&+00
V
48
8 . 49E-01
1 . 9211:-01
1 . 04&+00
CA
49
1 . 62E+00
1 . 61&-01
1 . 7 8&+00
CR
49
1 . 59E+OO
7 . 0211:-02
1 . 66&+00
SC
49
1 . 62E+OO
6 . 3311:-05
1 . 6211:+00
0 . 00&+00
V
49
o . ooz+oo
0 . 00&+00
CR
51
2 . 89E- 04
2 . 80&-03
3 . 09E-03
MN
51
1 . 59E+00
6 . 76E-02
1 . 66&+00
FE
52
9 . 65E-01
4 . 84&-02
1 . 011:+00
- 53 -
MN
52N
1 . 58E+OO
1 . 57E-01
1 . 73E+OO
MN
52
4 . 98E-01
2 . 28E-01
7 . 26E-01
MN
53
O . OOE+OO
7 . 29E-03
7 . 29E-03
MN
54
3 . 97E-04
5. 74E-02
5 . 78E-02
CO
55
1 . 26E+OO
1 . 3U - 0 1
1 . 39E+OO
FE
55
O . OOE+OO
7 . 71E-03
7 . 7 1E-03
CO
56
3 . 30E-01
2 . 21E-01
5 . 51E-01
MN
56
1 . 591:+00
1 . 081:-01
1 . 70E+OO
llfl:
56
2 . 8U-02
1 . lU-01
1 . 421:-01
CO
57
7 . ' 7E-02
2 . 26E-02
9 . 73E-02
NI
57
6 . 90E-01
l . 22E-01
8 . 12E-01
CO
58N
O . OOE+OO
7 . 09E-03
7 . 09E-03
CO
58
2 . 49E-01
7 . 09E-02
3 . 20E-Ol
FE
59
l . 06E+OO
7 . 79E-02
1 . 13E+OO
NI
59
O . OOE+OO
8 . UE-03
8 . 49E-03
CO
60N
4 . 03E-03
8 . 281:-03
l . 2 3E-02
CO
60
9 . 6811-01
1 . 6311-0 1
1 . 1 311+ 0 0
60
1 . 5 111+00
2 . 4211-01
1 . 75,+00
n
60
2 . 5911-01
0 . 0011+00
2 . 5911-01
CO
61
l . 59E+00
6 . 55E-03
1 . 5 911+ 0 0
61
1 . ou+oo
5 . 5511-02
1 . 0911+00
62N
1 . 62E+OO
1 . 7311-01
1 . 7911+00
62
l . 60E+OO
6 . 8511-02
1 . 6711+00
ZN
62
l . UE - 0 1
3 . 86E-02
1 . 8311-01
NI
63
O . OOE+OO
O . OOE+OO
O . OOE+OO
ZN
63
1 . 52&+00
7 . 39B-02
l . 59E+00
8 . 25E-01
l . 6U-02
8 . UE - 0 1
1 . 531:+00
7 . 741:-02
1 . 6111+ 00
1 . 601:+00
CU
CU
CO
CU
CU
u
ca
65
NI
65
1 . 561:+00
3 . 51J:-02
ZN
CU
65
2 . 2u-02
4 . UJ:-02
6 . 891:-02
66
1 . 621:+00
5 . 7011-03
1 . 631:+00
ca
66
9 . 371:-01
1 . Ull -0 1
1 . 081:+00
Gll
66
4 . 2 81: -0 1
5 . 3711-02
4 . 8211-01
NI
66
6 . 401:-01
O . OOB+OO
6 . 4011-01
67
1 . 35&+00
7 . 80B-03
1 . 351:+00
ca
67
2 . 66B-01
2 . UB-02
2 . 8811-01
Gll
67
l . 58E+OO
9 . 21B-02
1 . 68E+OO
ca
68
l . '7B+OO
6 . 45B-02
l . 53E+OO
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189
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194
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199
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