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Making short-line regulation zero

Short answer

Voltage regulation of a short line is made zero by operating the receiving end at a leading power factor equal to X/|Z| (tan φ = R/X). This is achieved by connecting a shunt capacitor or synchronous condenser to supply the required leading reactive power.

How can the voltage regulation of a short transmission line be made zero? Explain with necessary mathematical derivation.

The voltage regulation of a short line is zero when the receiving-end voltage at full load equals the sending-end voltage, i.e. ∣VS∣=∣VR∣|V_S| = |V_R|. This happens only for a suitable leading power factor at the receiving end.

Derivation

Short line: VS=VR+I(R+jX)V_S = V_R + I(R + jX). Take VRV_R as reference and the current at angle ϕ\phi (lagging taken positive):

I=Icos⁡ϕ−jIsin⁡ϕI = I\cos\phi - jI\sin\phi VS=VR+(Icos⁡ϕ−jIsin⁡ϕ)(R+jX)=(VR+IRcos⁡ϕ+IXsin⁡ϕ)+j(IXcos⁡ϕ−IRsin⁡ϕ)\begin{aligned} V_S &= V_R + (I\cos\phi - jI\sin\phi)(R + jX) \\ &= (V_R + IR\cos\phi + IX\sin\phi) + j(IX\cos\phi - IR\sin\phi) \end{aligned}

The quadrature part changes ∣VS∣|V_S| very little, so

∣VS∣≈VR+IRcos⁡ϕ+IXsin⁡ϕ|V_S| \approx V_R + IR\cos\phi + IX\sin\phi %VR≈I(Rcos⁡ϕ+Xsin⁡ϕ)VR×100\%VR \approx \frac{I(R\cos\phi + X\sin\phi)}{V_R}\times100

For a leading load the angle is negative, so sin⁡ϕ\sin\phi changes sign. Writing ϕ\phi from here on for the magnitude of the leading angle:

%VR≈I(Rcos⁡ϕ−Xsin⁡ϕ)VR×100\%VR \approx \frac{I(R\cos\phi - X\sin\phi)}{V_R}\times100

Condition for zero regulation

Rcos⁡ϕ−Xsin⁡ϕ=0tan⁡ϕ=RXcos⁡ϕ=XR2+X2=X∣Z∣ (leading)\begin{aligned} R\cos\phi - X\sin\phi &= 0 \\ \tan\phi &= \frac{R}{X} \\ \cos\phi &= \frac{X}{\sqrt{R^2 + X^2}} = \frac{X}{|Z|}\ \text{(leading)} \end{aligned}

Equivalently, the load angle ϕ=90∘−θ\phi = 90^\circ - \theta, where θ=tan⁡−1(X/R)\theta = \tan^{-1}(X/R) is the line impedance angle.

         I (leads Vr by phi)
        /      Vs (same length as Vr)
       /     .
      /   .   IZ (perpendicular to Vr+Vs bisector)
     / .
    O--------------> Vr

How it is achieved in practice

  1. Connect a shunt capacitor bank or synchronous condenser at the receiving end so that the net receiving-end pf becomes X/∣Z∣X/|Z| leading.
  2. Required leading reactive power (approx.): Qnet=−P R/XQ_{net} = -P\,R/X, so capacitor rating QC=Ptan⁡ϕload+P R/XQ_C = P\tan\phi_{load} + P\,R/X.
  3. If the load is already more leading than this (negative regulation), a shunt reactor is added instead.

Example: R=4 ΩR = 4\ \Omega, X=8 ΩX = 8\ \Omega: zero regulation needs cos⁡ϕ=8/80=0.894\cos\phi = 8/\sqrt{80} = 0.894 leading.

(For an exact value, solve ∣VR+Z(P−jQ)/VR∣=∣VR∣|V_R + Z(P - jQ)/V_R| = |V_R| for QQ; it gives a slightly more leading pf than the approximate formula.)

✓ Answer checked by Claude Opus 5.5 (high effort)

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