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Recoveries were comprised between 82% and 114% with relative standard deviations about 5 15% (n=5) within a concentration range about 0.03 44 µg L−1.
The thermal expansion coefficients αT at 303 K, calculated from the density studies, exhibited significant positive deviations (about 20%) from ideality for piperidine water mixtures.
Because the state-vector equations accurately represent most physical systems, which only have small deviations about their steady-state behaviour, it follows that in the natural world small-scale control is almost always possible, at least in principle.
The atomic rms deviations about the average minimized coordinate positions for the secondary structure region of the N-terminal and C-terminal domains are 0.44 +/- 0.07 and 0.55 +/- 0.18 A for backbone atoms, and the 1.09 +/- 0.07 and 1.10 +/- 0.15 A for all heavy atoms, respectively.
Sum of squared deviations about the grand mean across all N observations.
The error bars represent the standard deviations about the mean (n = 3).
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Because the integral from negative infinity to 1.645 standard deviations is about 0.05.
These equations are well constrained and fit the data well (71% < R2 < 88%), but they have standard deviations of about 0.5 log units, such that the range defined by the mean ± one standard deviation spans about an order of magnitude.
The results, in terms of mean deviation between the experimental and calculated compositions, are satisfactory, with rms deviations of about 4%.
Measurements and comparisons between conventional light barrier timing systems and the RFID timing system with ankle-worn transponders show deviations of about 25ms.
The experimental and analytical thermal efficiency estimations agree reasonably well with a maximum deviation of about 12%.
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