At the power-limit condition i.e. for maximum PR (a) leading VARS (Qp) goes to the load for any values of Veand V, S (b) leading VARS (Qp) goes to the load ONLY for Vs= VR (c) lagging VARS (Qp) goes to the load for any values of Vg and VR (d) lagging VARS (Qp) goes to the load ONLY for Vs = VR %3D

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At the power-limit condition i.e. for maximum P
(a) leading VARS (Qp) goes to the load for any
values of Veand V,
R
(b) leading VARS (Qp) goes to the load ONLY for
Vs= VR
(c) lagging VARS (Qp) goes to the load for any
values of Vg and VR
.
(d) lagging VARS (Qp) goes to the load ONLY for
Vs = VR
Transcribed Image Text:At the power-limit condition i.e. for maximum P (a) leading VARS (Qp) goes to the load for any values of Veand V, R (b) leading VARS (Qp) goes to the load ONLY for Vs= VR (c) lagging VARS (Qp) goes to the load for any values of Vg and VR . (d) lagging VARS (Qp) goes to the load ONLY for Vs = VR
The active and the reactive power delivered at
the receiving end of a short transmission line of
impedance ZZY are respectively given by
VsVR
PR-
cos(4 – 8) –
Cos Y and
%3D
V VR
Qp = Qp = VR
sin(Y – 8)-
sinY , with
Z.
%|
%3D
Vg and Vz being the magnitude of voltage at the
sending and receiving ends, & the power-angle.
Transcribed Image Text:The active and the reactive power delivered at the receiving end of a short transmission line of impedance ZZY are respectively given by VsVR PR- cos(4 – 8) – Cos Y and %3D V VR Qp = Qp = VR sin(Y – 8)- sinY , with Z. %| %3D Vg and Vz being the magnitude of voltage at the sending and receiving ends, & the power-angle.
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