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Initially developed for space applications, we demonstrate the applicability of this library of cutoff rigidity models for computing aircraft radiation dose.
This paper presents some of the usually ignored limits on the accuracy of the vertical cutoff rigidity models and describes some of the computational artifacts present in these models.
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The rigidity model we used is calculated using the 1D model in Table 1.
We shall point out that this is not a result of using a low rigidity model.
We have developed a dynamic geomagnetic vertical cutoff rigidity model that predicts the energetic charged particle transmission through the magnetosphere.
The classical body-and-bar rigidity model can be viewed as a body-and-cad structure that uses only one constraint from this new class.
We have a developed a dynamic cutoff rigidity model based on computed world grids of vertical cutoff rigidities derived from employing the Tsyganenko magnetospheric model.
Solar modulated primary particles are flltered with a new analytical fully angular dependent geomagnetic cutoff rigidity model, as a function of latitude, longitude, arrival direction, altitude and time.
Designated CARI-6, this program incorporates an updated geomagnetic cutoff rigidity model and a revision of the primary cosmic ray spectrum based on recent work by Gaisser and Stanev (1998).
In the average axial rigidity model, the slope of the linear regression was 1.23 and the y-intercept offset was 3142, suggesting that CTRA using average axial rigidity consistently over-predicts bone rigidity.
In the minimum axial rigidity model, the slope of the linear regression was 1.05 and the y-intercept offset was 69, indicating that CTRA is correlated without much skewness with mechanical testing results over the full range of the values tested.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com