Author Archive

New Short Names for Nucleonica Apps

April 30th, 2019

Nucleonica applications are represented as “tiles” in the App Portal. For every application there is a tile consisting of a header “Short Name” and a body “Full Name”. As an example, in the image below, the short name GSG refers to the application Gamma Spectrum Generator++.
To make the tile names more intuitive, new “Short Names” have been introduced for many Apps. These are shown in the image below for the filter category “last used”.
NewShortNames2As can be seen the new short names are more intuitive than the older names e.g. Datasheet (old name NuDat++), Explorer (Expl++), decay (DE++), Search (NuS/RaS). It should be noted that the Radiological Converter and Mass Activity Converter new short names are Conv. Pro and Conv. respectively. The gamma library apps have also been renamed to gLib Pro and gLib. The gamma dosimetry and shielding apps have the new short names gH*(10) and gD&S.

More info…
App Portal wiki page

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Nuclear Security Exercises now available to all Nucleonica users

March 28th, 2019

In Nucleonica’s e-Learning center (e-Learn app), a series of nuclear security exercises has been released for all Nucleonica users.
eL-NSENucleonica’s e-Learning Centre showing the nuclear security exercises.

These exercises have been developed jointly with Dr. Emily Alice Kröger from the Federal Office for Radiation Protection (Bundesamt für Strahlenschutz) and the Nucleonica Team. The exercises were developed for use in BfS training courses on Nucleonica held on a regular basis. Because of the general interest in these presentations, we have released them for general use by Nucleonica users.

More info…
Nucleonica’s e-Learing Centre

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webKORIGEN and DELNuS updates

March 26th, 2019

WebKORIGEN is a Nucleonica application for the simulation of the time evolution of a nuclide inventory in power reactors. A related application, DELNuS (Decay Engine for Large Nuclide Sets), allows the user to make decay calculations for a large number of nuclides (typically present in a reactor).
Following a new compilation (2019), a number of updates and improvements in the webKORIGEN and DELNuS applications have been made:
webKORIGEN:
– it is now possible to make Ra226 irradations in the flux mode.
– new tabs show the cross section data (also burnup dependent ) and decay data used in the calculations for the various reactor types.
– in the results grid, nuclide half-lives have been added
wKOwebKORIGEN user interface

DELNuS
– a problem with using mixtures in DELNuS has been resolved.
– in the results grid, the nuclide half-lives have been added
– decay data used in the calculations are displayed
DELNuSDELNuS user interface

More info…
webKORIGEN
Neutron irradiation with webKORIGEN
DELNuS

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Ra-226 irradiations now possilbe with webKORIGEN

March 22nd, 2019

Qu. (from D. B. Garching, Germany):
Dear Nucleonica Team, if I let Ra-226 irradiate in a certain flux for a certain time, why I do not get nuclides with mass numbers higher than 226?

Ans. (Nucleonica Team)
This problem has now been resolved.

Results are shown below for an irradiation of Ra-226 (2g) in a dedicated facility with a thermal neutron flux of 2e14 neutrons per cm2 per s for a period of 100 days.
Ra226 Irrad

More info…
– webKORIGEN++ neutron activation wiki page

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Problem with using mixtures in DELNuS++

February 25th, 2019

Some of our users have reported that the results of a decay calculation using DELNuS++ for a mixture does not give the same result as the sum of the results for the single nuclide calculations.
As an example, the activity of Cs137 or Kr85 produced from a mixture of Cf252 and Cf250 is almost a factor two higher that from the sum of the results using the single nuclides Cf252 and then Cf250.
The problem has now been identified and resolved.
The results obtained using DELNuS++ for the mixture are now consistent with the sum of the results for the individual component nuclides. The results also agree with those obtained using the Decay Engine++ (which can also account for fission products).

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Ambient dose rates caused by different types of radiation

February 8th, 2019

Ambient dose equivalent H*(d) is the normal monitoring (area monitoring) quantity for X, gamma and neutron radiation where d is the depth at which the dose applies. International convention in radiation protection is to use the ambient dose equivalent at 10 mm depth i.e. H*(10). The ambient dose gives a conservative estimate of the effective dose a person would receive when staying at the point of the monitoring instrument (NPL).
In Nucleonica applications, the photon (X+gamma), beta, and neutron doses are calculated separately using analytical and semi-analytical formulae. To obtain the (total) ambient dose H*(d), these individual doses must be added. Following Otto, the ambient dose from a radionuclide can be represented as a sum of components caused by different radiation types, i.e.
ADR_Radiations3This is the notation which will be used in various Nucleonica applications for ambient doses and dose rates i.e.
ADR_Radiations4
For control of doses to skin and lens of eye, the directional dose equivalent is used. The directional dose equivalent denoted by H′(d) is intended for use with less penetrating radiation such a beta particles. Its main use is for skin dose at a depth of 0.07 mm. For beta radiation and electrons, for example, this is denoted as i.e. H'(0.07)e.
ADR_Radiations6

More info…
– T. Otto, Personal Dose-Equivalent Conversion Coefficients for 1252 Radionuclides, Radiation Protection Dosimetry (2016), Vol. 168, No .1, pp1-70. Link
NPL: Measurement of dose rate
Operational quantities (Wikipedia)

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World’s oldest periodic table chart found in St Andrews

January 22nd, 2019

A periodic table discovered at the University of St Andrews is thought to be the oldest in the world. Following Menedleev’s famous discovery of periodicity in the chemical elements in 1869, a number of such periodic tables were created. The St. Andrews periodic table is similar to Mendeleev’s second table from 1871. Original_PT2Periodic Table discovered at St. Andrews University, Scotland (Courtesy St. Andrews University).
The United Nations has designated 2019 as the international year of the Periodic Table of chemical elements, recognizing it as an instrument ‘central to linking cultural, economic and political aspects of the global society through a common language’.

More info…
St. Andrews University News
Article in Der Spiegel (in German)
United Nations Year of the Periodic Table

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Karlsruhe Nuclide Chart (Contour Chart) at URENCO, Netherlands

January 14th, 2019

Nucleonica has arranged the installation of a “contour” version of the Karlsruhe Nuclide Chart at the URENCO premises in Almelo, Netherlands.
The Chart was produced using a 4mm Dibond aluminium plate “cut-out” to fit in a space of height 2m and width 5m and assembled a small distance from the wall. The text is cut from adhesive foil and glued directly on the wall.
UERENCO_KNC_2018Karlsruhe Nuclide Chart (Contour Chart) at the URENCO premises in the Netherlands, Courtesy URENCO. For further information, contact info@nucleonica.com.

More information…
Other print versions of the Karlsruhe Nuclide Chart
Nuclide Charts
Contour Nuclide Chart for European Dialogue Centre

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Energy deposited in matter by nuclear and electronic stopping processes

January 14th, 2019

Qu. (from G.D. Fz-Juelich):
Dear Nucleonica Team, we have the following question regarding the energy deposited in matter by nuclear and electronic stopping processes:
We are interested in the respective contributions of nuclear stopping and electronic stopping to the (integral) energy deposited in solid materials during irradiation with heavy ions with defined energy (e.g. Au-197 ions with 5 MeV). Using the Range & Stopping Power++ App in Nucleonica, the results table provides only the values for the electronic and nuclear stopping at the materials’ surface (e.g. in keV/µm at depth 0 µm).
Bragg curve for 5MeV Au-197 on Water (liquid)
Integrating the Bragg curves (using the downloaded graph data) by the trapezoidal method suggests that the sum of the energies deposited by nuclear and electronic amounts only to 80 to 90% of the initial energy of the projectile. Is this correct (and if so, where is the remaining energy), and is there a more convenient way to directly calculate the amounts of energy deposited by each nuclear and electronic stopping, respectively, using either the Range & Stopping Power++ App in Nucleonica or SRIM/TRIM.

Ans. (Nucleonica Team)
The difference in the sum of the energies deposited by nuclear and electronic contributions come most probably from the limitations of numerical calculation procedure.
The difference is not due, for example, to Bremsstrahlung since Bremsstrahlung is considered only for light particles, i.e. incoming electrons and positrons. The R&SP++ app does not calculate Bremsstrahlung for heavy ions. This difference probably comes from the numerical procedure. Note the R&SP++ app uses the SRIM engine for heavy ions, so R&SP++ app and SRIM’s results are the same.
The Nucleonica Team will investigate this difference further.

More info…
Range and Stopping Power wiki page

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Nucleonica Newsletter 2019

January 6th, 2019

Dear Nucleonica Users,
Hopefully you had a great start into the New Year, and we wish you every success in 2019. For the Nucleonica Team, a major focus over the past year was the development and improvement of new and existing applications. Detailed information on these activities is described in this Newsletter.
A highlight in 2018 was the launch of the new 10th Edition of the Karlsruhe Nuclide Chart in early 2018. You can order your copy here.
A further highlight was the development of a new online e-Learning Training Centre, making the Nucleonica product knowledge more transparent and accessible.
NN2019The Nucleonica Team would like to thank you for your continued support.
Best wishes for 2019, Sincerely yours,
Joseph Magill, Managing Director

More information…
Nucleonica Newsletter 2019
Previous Newsletters
Nucleonica Newsletter 2018
Nucleonica Newsletter 2017
Nucleonica Newsletter 2016
Nucleonica Newsletter 2015
Nucleonica Newsletter 2014
Nucleonica Newsletter 2013
Nucleonica Newsletter 2012

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