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On the average, we achieved a of around with low and errors of around, and respectively.
For ECr11, we tried to determine the V p of the uppermost mantle beneath the arc by using Moho reflections of the subducting PHS plate (e.g., Fig. 6c), but the fitting between the observed and the calculated travel times sometimes shows errors of around 0.5 s.
We find the Swarm vector residuals have low means with rms errors of around 4 nT or less.
It is a method to obtain estimates in the local and global domains of the chamber, and there are some studies that predict temperatures with errors of around 3%% [5, 6].
We use single precision in calculating interactions, but all components are accumulated in double precision so we can achieve force errors of around 10−5%, well below what is needed for these simulations.
Depending on the individual systems used, recent studies reveal mean displacement errors of around 2 mm between different fractions and about 1 mm within fractions.
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A 10-cm vertical or longitudinal offset both result in a translation error of around 6% (Figure 13, bottom two).
Furthermore, the ratio between the 2-D and 1-D simulations, shown in Fig. 3b, gives a minimum value close to 40%, illustrating that the 1-D simulation can result in an error of around 60%.
For each P value, 40 000 permutations were generated in order to obtain a standard error of around 0.001.
However, positional errors were greater for homes outside the large metropolitan areas (Bonner et al. 2003), and rural addresses in Iowa had a median positional error of around 200 meters (Ward et al. submitted).
The initial report is an estimate with a margin of error of around 100,000 people.
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