# Mecanica De Fluidos Ugarte Pdf 11 😀

Mecanica De Fluidos Ugarte Pdf 11

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Mean and Pearson correlation coefficients (cor) with the observed $Q_{n}$ have been calculated for the

data sets. This helped us to characterize the real output of each component, namely the inliers, $Q_{inliers}^{n}$ and the outliers, $Q_{outliers}^{n}$.

It is defined as the difference between $Q_{inliers}^{n}$ and $Q_{outliers}^{n}$. It is important to note that the $Q_{0,thr}^n$ is calculated with the same dataset, thus once again, the $I_{thr}$ is a number very close to the one that would be calculated with the same data, that is, the data that has been used to calculate the $Q_{0,thr}^n$ in the first place.

Therefore, this definition assumes that a $Q_{0,thr}$ lower or equal to the $Q_{0,thr}$ calculated with the same dataset is not physically appropriate.

For this reason, the criterion $Q_{0,thr}^n \leq Q_{0,thr}^{n-1}$ is employed as the stop condition, which disables the oscillator if the latter is deemed not acceptable.

The stop condition is invoked after the first iteration, as after that the mean of the total physical component is determined.

The stop condition is invoked once the total physical component reaches an acceptable level, that is, when the prediction is physically appropriate.

The mean of the total physical component is then used to calculate the $Q_{0,thr}$ in the second iteration, that is, the mean of the total physical component is used to calculate the threshold in the second iteration.

Finally, after all iterations, $T$, the best calculated $Q_{0,thr}$ is used to calculate the threshold for the period being considered.

The following four scenarios were tested:

1. Large error on the $Q_{0,thr}$ determination: the $Q_{0,thr}$ is determined by a large error, which means that the $Q_{0,thr}$ is either: a) below the real $Q_{0,thr}$, or b) above the real $Q_{0,thr}$.