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As shown in Table 1, experimentally determined masses match those expected theoretically within the experimental uncertainty.
Within the experimental uncertainty, no significant hysteresis was observed.
The total experimental uncertainty is obtained as 4.2%.
Quantitative estimates of the experimental uncertainty are presented.
This is of the same order of magnitude as the experimental uncertainty.
Here we demonstrate how the experimental uncertainty and variability[2, 3] affect Matched Molecular Pair Analysis.
Both converge towards a same value, around θ = 92°, up to experimental uncertainty.
The experimental uncertainty for the average heat transfer coefficient is calculated as (4).
Next, the experimental uncertainty is added to S, which defines the sample (S_{noise}).
As indicated in Table 10, although the predicted values are not exactly within experimental uncertainty in some cases (the predicted values are within the experimental uncertainty of ± 0.05 in Chen et al. [87]), the sigma values are better than 0.05.
Furthermore, the velocity variations measured for all the flow rates all fall within the experimental uncertainty values of the measurement.
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