2018
DOI: 10.1049/iet-gtd.2018.0376
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Contribution of FACTS devices in power systems security using MILP‐based OPF

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Cited by 28 publications
(34 citation statements)
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“…To compromise between accuracy and tractability, the proposed MINLP optimisation problem in (1)-(31) is recast into an MILP problem by linearising the non-linear and non-convex constraints in (7)-(9). To obtain a linear approximation for the non-linear and non-convex nodal active and reactive power balance equations in (7) and (8), it is assumed that the voltage magnitudes are close to 1 pu, the differences of voltage angles between adjacent buses are within [ − π/6, π/6], the reactance/resistance ratios for transmission lines are considerably high (the reactance/resistance ratio is >10) [32]. Hence, given a specific xl i,j , the linear approximation of the nodal active and reactive power flow equations in (7) and (8) can be obtained by the proposed linearisation technique in [32] with sufficient accuracy as follows: (see (32)) (see (33)) where δ i, j in (32) and (33) is equal to θ n − θ j .…”
Section: Linear Coordinated Planning Modelmentioning
confidence: 99%
See 3 more Smart Citations
“…To compromise between accuracy and tractability, the proposed MINLP optimisation problem in (1)-(31) is recast into an MILP problem by linearising the non-linear and non-convex constraints in (7)-(9). To obtain a linear approximation for the non-linear and non-convex nodal active and reactive power balance equations in (7) and (8), it is assumed that the voltage magnitudes are close to 1 pu, the differences of voltage angles between adjacent buses are within [ − π/6, π/6], the reactance/resistance ratios for transmission lines are considerably high (the reactance/resistance ratio is >10) [32]. Hence, given a specific xl i,j , the linear approximation of the nodal active and reactive power flow equations in (7) and (8) can be obtained by the proposed linearisation technique in [32] with sufficient accuracy as follows: (see (32)) (see (33)) where δ i, j in (32) and (33) is equal to θ n − θ j .…”
Section: Linear Coordinated Planning Modelmentioning
confidence: 99%
“…To obtain a linear approximation for the non-linear and non-convex nodal active and reactive power balance equations in (7) and (8), it is assumed that the voltage magnitudes are close to 1 pu, the differences of voltage angles between adjacent buses are within [ − π/6, π/6], the reactance/resistance ratios for transmission lines are considerably high (the reactance/resistance ratio is >10) [32]. Hence, given a specific xl i,j , the linear approximation of the nodal active and reactive power flow equations in (7) and (8) can be obtained by the proposed linearisation technique in [32] with sufficient accuracy as follows: (see (32)) (see (33)) where δ i, j in (32) and (33) is equal to θ n − θ j . Also, the parameters α, α, β, and β in (32) and (33) can be obtained from (34) and (35) where Δδ is the deviation of the voltage angle and the functions Φ and Ψ are defined in the constraints (7) and (8), respectively.…”
Section: Linear Coordinated Planning Modelmentioning
confidence: 99%
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“…The first stage problem, Equations (1)‐(21), includes uncertain parameters such as active and reactive load, P D , Q D and D MG , energy price, λ , photovoltaic power, P PV , wind system power, P W , EVs charge/discharge rate, CR EV / DR EV , and EVs plugged‐in/plugged‐out time energy, E arr / E dep . Hence, the scenario‐based stochastic programing is implemented to model the load based on normal probability distribution function (PDF), 35 photovoltaic and wind system power model according to Beta and Weibull PDF, 36 and EVs parameters model depending on the Rayleigh PDF 37 . Furthermore, the Roulette Wheel Mechanism (RWM) and Kantorovich method are applied to generate and reduce the scenario samples, respectively, 38 where more details of this technique were expressed in 38 …”
Section: Two‐stage Model Of the Coupling Of Cema And Shs In Sdnmentioning
confidence: 99%