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Zbus vs Ybus; off-nominal transformer model

Short answer

Ybus is sparse, formed by inspection, used for load flow; Zbus is full, built algorithmically, used for fault analysis. For an off-nominal transformer 1:t with leakage admittance y, Ybus = [[t²y, –ty],[–ty, y]]. The π-model has series ty, shunt t(t‑1)y on the tap side, and (1–t)y on the other side.

What are difference between bus impedance matrix (Zbus) and bus admittance matrix (Ybus)? Develop Ybus for regulating transformers whose off-nominal turn ratio is 1:t and draw the equivalent π-model for this transformer.

Zbus versus Ybus

PointYbusY_{bus}ZbusZ_{bus}
RelationI=YbusV\mathbf{I} = \mathbf{Y}_{bus}\mathbf{V}V=ZbusI\mathbf{V} = \mathbf{Z}_{bus}\mathbf{I}
StructureSparseFull (dense)
FormationBy inspection, simpleBuilding algorithm or inversion
ElementsDriving-point and transfer admittancesDriving-point and transfer impedances
Main useLoad flow (G-S, N-R)Short-circuit (fault) studies
ModificationEasyNeeds building steps

Ybus for a regulating (off-nominal tap) transformer

Model the transformer as an ideal transformer of ratio 1:t1 : t in series with its per-unit leakage admittance y=1/zy = 1/z placed on the tap (bus q) side. Bus p is on the "1" side, bus q on the "t" side.

  p   Ip      1 : t     x    y     Iq   q
  o----->----)|(------o--[===]----<-----o
  Vp              Vx = t Vp

Ideal transformer: Vx=tVpV_x = tV_p. Let Ixq=y(Vx−Vq)I_{xq} = y(V_x - V_q) be the current leaving node x towards q, so Iq=−IxqI_q = -I_{xq}. Being lossless, VpIp∗=VxIxq∗V_pI_p^* = V_xI_{xq}^*, which with real tt gives Ip=tIxqI_p = tI_{xq}:

Iq=y(Vq−tVp)=−tyVp+yVqIp=t y(tVp−Vq)=t2yVp−tyVq\begin{aligned} I_q &= y(V_q - tV_p) = -tyV_p + yV_q \\ I_p &= t\,y(tV_p - V_q) = t^2yV_p - tyV_q \end{aligned}

In matrix form:

[IpIq]=[t2y−ty−tyy][VpVq]\begin{bmatrix} I_p \\ I_q \end{bmatrix} = \begin{bmatrix} t^2y & -ty \\ -ty & y \end{bmatrix} \begin{bmatrix} V_p \\ V_q \end{bmatrix}

So the transformer adds t2yt^2y to YppY_{pp}, yy to YqqY_{qq} and −ty-ty to YpqY_{pq}, YqpY_{qp}.

Equivalent π-model

Match a π circuit (series AA, shunts BB at p and CC at q) to the matrix: Ypq=−AY_{pq} = -A, Ypp=A+BY_{pp} = A + B, Yqq=A+CY_{qq} = A + C:

A=ty,B=t2y−ty=t(t−1)y,C=y−ty=(1−t)yA = ty,\qquad B = t^2y - ty = t(t - 1)y,\qquad C = y - ty = (1 - t)y
  p          t*y            q
  o--------[=====]----------o
  |                         |
 [ t(t-1)y ]          [ (1-t)y ]
  |                         |
 ===                       ===

If t=1t = 1, the shunts vanish and the model becomes the simple series admittance yy. For t≠1t \ne 1 the two shunt branches have opposite signs (one acts inductive, the other capacitive), which is how the tap changes reactive power flow and bus voltage.

✓ Answer checked by Claude Sonnet 5.5

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