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where dg i represents the Haar measure over the group.
The gravity change Δg for each grid as calculated below: (2) where (dg i, j, dg i +1, j, dgi, j+1, dg i +1, j+1) are the gravity change at one grid square.
Whereas, it indicates that the reactive power output of DG i is less than the desired output, e.g., Q i < Q desired, and the DG i is on the condition of under-load.
The total amplitude can be written as A = ∫ ∏ i dg i A ( g 1, …, g n ) B ∗ ( g 1, …, g n ) Open image in new window (11).
The absolute value of ρ i, i.e., degree error of the reactive power sharing of DG i, increases gradually along with the increase of K e.
E i ∠θ i (i = 1,2,⋯) is the voltage output of DG i ; P i and Q i are the active and reactive power flowing into loads generated by DG i, respectively; V∠θ is the AC common bus voltage; Z i ∠φ i is the equivalent impedance.
Similar(13)
(2) M = I DG ∩ I DT List of mediator proteins is shown in Additional file 1: Table S1.
In (9), F DG,i in (left( {$/{text{h}}}} right)) is the production cost function of i th DG obtained from the slope a DG,i and intercept b DG,i of DG offer as shown below: F_{DG,i} = frac{1}{2}a_{DG,i} P_{DG,i}^{2} + b_{DG,i} P_{DG,i} (10).
If x DG,i,t = 1/−1/0, then the DG power output of bus i at time t reaches the upper limit/the lower limit/the forecasted value.
Given the DG power output (tilde{P}_{DG,i,t} in [overline{P}_{DG,i,t} - hat{P}_{DG,i,t},overline{P}_{DG,i,t} + hat{P}_{DG,i,t} ]), a robust model can be derived from the lower-level as hbox{min} sumlimits_{{i in A_{n} }}^ {R_{i} } (47) {text{s}}.
In DG I.10 he argues that the original ingredients are only potentially, and not actually, present in the resulting compounds of a mixing process.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com