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Clearly, the fidelity of the nuclear cross-sections is essential to correct specification of shield design and sensitivity to cross-section error is important in guiding experimental validation of cross-section models and database.
The dynamic cross section, soft error rate and mean work between failures are calculated based on the experimental results.
The right column f-j show the 100th cross section phase errors.
For the trapezoidal cross section, the maximum error of critical flow depth is less than 6 × 10−6% (near exact solution) and the maximum error of normal depth is less than 0.25% (very accurate solution).
a, b The vertical cross section of hypocenter error distribution.
As a result, the modified 2D model and three zone 2D model can similarly provide more accurate cross section which reduces the error from 2000 to 300 pcm.
Owing to the small cross section of C for He ion, the error on the absolute H content calculated by this method is about 25%.
Aggregate heights were measured from the height in cross section of the topographic AFM images; standard errors are reported.
When comparing the increasing of the cable cross section (and therefore its stiffness) the values of the error are consistently decreasing for the cable tension.
The maximum error of normal flow depth for parabolic cross section is also less than 8 × 10−3% (near exact solution).
The result is a database that is a blend of cross section and time series, with an unknown degree of measurement error in either dimension.
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