学术文献库

This note outlines the exact solution to the power flow problem in AC electrical networks under the assumption of 'flat' or uniform voltage profiles. This solution generalises the common 'DC power flow' approach to electrical network problems where the detail of the voltage profile is disregarded and the focus is on the distribution of active power flows and voltage phase angles. In the usual approach to the problem, network resistance is ignored and simplified power-angle relations are used based on branch reactances alone. The purpose of this note is to describe a tractable generalisation of this approach to account for arbitrary network resistances. The solution is worked in detail for a single network branch with resistance $R \geq 0$ and reactance $X > 0$, with explicit formulae derived linking branch impedance, active and reactive power flows, voltage phase displacement and losses under the 'flat' voltage profile assumption. These formulae have a convenient expression in terms of a 'coefficient of support' which relates the assumed active power flow to the corresponding reactive power consumed on the branch, and encapsulates much of the mathematical technicalities in the exact solution. It is shown that when network resistance is taken into account, the angle displacement $δ_j - δ_k$ between adjacent bus voltages is always larger than given by the lossless power-angle relation $\sin(δ_j - δ_k) = XP$. The approach is applied to the analysis of circulating power flows in large networks, building on the classic work of Janssens and Kamagate (2003). It is seen that in networks with nonzero branch resistances, a circulating flow of active power is always accompanied by a counter-circulating flow of reactive power.