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The mean deviation for B X difference changes significantly from the V-ASM to the Z-ASM model, with an increase of 0.5 nT for both Swarm A and C datasets.
The last integral is equal to the incomplete gamma function and then the mean deviation for the OGE-W distribution is given by begin{array}rcl@ m_{1} z)=beta^{-1},sum_{k,r=0}^{infty} frac { -1)^{ -1(alpha+k),d_{k}}{(r+1)^{r}lambda^{-1}}}, alpha+k-1 choose r},d_{k}a(1+lambda^{-1},(r+1)(beta z)^{lambda}), end{ar+1y}.
Also, we see that the mean deviation for a beta random variable (X sim beta p,q)) is given by [14] mathit{MD}(X)= frac{2p^{p} q^{q}}{beta p,q)(p+q)^{p+q}} and, for a k-beta random variable (X simbeta_{k}(p,q)), mean deviation in terms of k is given by mathit{MD}_{k}(X) = frac{2(frac{p}{k})^{frac{p}{k}}(frac{q}{k})^{frac {q}{k}}}{beta_{k}(p,q)(frac{p+q}{k})^{frac{p+q}{k}}}.
The mean deviation for the two-goal kicking condition was +68.2 mm (SD = 318.4).
The mean deviation for the one-goal kicking condition was +23.9 mm (SD = 335.6).
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Equation (28) is the basic quantity to compute the mean deviations for the exp-G distributions.
It is useful to obtain the Bonferroni and Lorenz curves and mean deviations for the new model.
Mean deviation was also calculated for the Humphrey fields.
mean signed deviation for large trees.
mean signed deviation for small trees.
Figure 4 Mean track deviation for OoS-DPA.
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