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We present an accurate and simple model for calculating the spillage and the power contribution at the receiver for each heliostat in a heliostat field, based on HFLCAL model [2].
This is because the power contribution of the VSC3 to the grid is smaller than that of the VSC1.
In the case of Multitasking, Eq. 27 is replaced by Eq. 28 in order to prioritize the power contribution of each application.
This can be readily seen from Fig. 3: decreasing r g causes the proportion of the power contribution from the BESS to increase.
In all cases, the power contribution of all connected ac systems also has certain influence on the harmonic interaction in the entire system.
For each wavelength, the power contribution of the i th ray generated by emitter (1 ≤ i ≤ N) after k reflections can be expressed by P i, k ( E, R, λ ) = 1 d k, R 2 R S ( θ k, R, θ ′, λ ) A eff ψ k, R t i, k = ∑ j = 1 k d j − 1, j c + d k, R c (5).
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The dashed lines represent the ray paths, and the solid ones the power contributions.
The RSRP for a specific cell is defined as the linear average over the power contributions of the resource elements, within the considered measurement frequency bandwidth, which carry the cell-specific reference signals [28].
RSRP is defined as the linear average over the power contributions (in W) of the resource elements that carry cell-specific reference signals within the considered measurement frequency bandwidth.
The RSRP measurement, R P, is the linear average of the power contributions by cell-specific resource elements that carry reference signals within the measurement frequency bandwidth as shown in Eq. (1).
RSRP for a specific cell is defined as the linear average over the power contributions (in W) of the Resource Elements (REs) which carry cell-specific reference signals within the considered measurement frequency bandwidth [11].
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Justyna Jupowicz-Kozak
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