At the power-limit condition i.e. for maximum P(a) leading VARS (Qp) goes to the load for anyvalues of Veand V,R(b) leading VARS (Qp) goes to the load ONLY forVs= VR(c) lagging VARS (Qp) goes to the load for anyvalues of Vg and VR.(d) lagging VARS (Qp) goes to the load ONLY forVs = VR The active and the reactive power delivered atthe receiving end of a short transmission line ofimpedance ZZY are respectively given byVsVRPR-cos(4 – 8) –Cos Y and%3DV VRQp = Qp = VRsin(Y – 8)-sinY , withZ.%|%3DVg and Vz being the magnitude of voltage at thesending and receiving ends, & the power-angle.

we need to explain power limit condition for maximum PR.

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

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

Introductory Circuit Analysis (13th Edition)

13th Edition

ISBN:9780133923605

Author:Robert L. Boylestad

Publisher:Robert L. Boylestad

Chapter1: Introduction

Section: Chapter Questions

Problem 1P: Visit your local library (at school or home) and describe the extent to which it provides literature...

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Question

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.

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