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P_{i}^ = frac{{u_{i} hat{P}_{i}^{disch} }}{{sumlimits_{i = 1}^{L} {left( {u_{i} hat{P}_{i}^{disch} } right)} }}P_{TUi}^ (10 where ( u_{i} ) is the start-stop status of PCS i; ( SOC_{i}^ ) is the SOC of PCS i. 2) In the charging status (when ( P_{TUi}^ < 0 )): ( P_{i} ) is calculated by the SOD of each PCS i, ( SOD_{i} ) and allowable maximum charge power, ( hat{P}_{i}^{ch} ) of each PCS i.
That is, firstly, the initial target power of PCS i is calculated by (9).
1) In the discharging status (when ( P_{TUi}, >,0 )): ( P_{i}^ ) is calculated by the SOC of each PCS i, ( SOC_{i}^ ) and allowable maximum discharge power, ( hat{P}_{i}^{disch} ) of each PCS i.
The reactive power of each PCS is calculated based on the allowable maximum reactive power for PCS i, ( hat{Q}_{i}^ ), are as shown in (16).
Firstly, the initial target power of PCS i is calculated based on the SOD of each PCS unit using (11) and (12) as follows.
Q_{TUi}^ = frac{{u_{TUi} hat{Q}_{TUi}^{{sumlimits_{i = 1}^{L} {left( {u_{TUi} hat{Q}_{TUi}^ right)} }}Q_{all {text -} BESS}^ (14 where ( hat{Q}_{TUi}^ ) is calculated based on the maximum allowable apparent power of PCS i. ( bar{S}_{i}^ ) and the current active power of each PCS, ( P_{i}^ ), are as shown in (15).
Similar(49)
Tables 5 and 6 list P(w j |PC i ) and weight λ i for PC i.
Each column in the matrix "UK" represents a PC i.e. the loadings.
There are some toxic events after the long-PCI.
We drew the trial specific control group event rate, PC i, from a uniform distribution, PC i ~U PC-0.15, PC+0.15).
There were no significant differences between the two groups (classical vs. DK crush) pre-PCI or immediately post-PCI.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com