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Three-phase overhead line which includes effects that vary as a function of frequency

**Library:**Simscape / Electrical / Passive / Lines

The Frequency-Dependent Overhead Line (Three-Phase) block represents a high-fidelity frequency-dependent overhead line that offers accurate transient response simulation from 0.01 Hz to 100 kHz.

The block computes frequency-dependent impedance and admittance matrices. The calculations also depend on the loss, inductance, and capacitance of the return path.

For more information on using a frequency-dependent overhead line (three-phase), see Engineering Applications.

The electromagnetic behavior of a multiconductor transmission line is described by the telegrapher's equation.

$-\frac{dV}{dx}=ZI$

$-\frac{dI}{dx}=YV$

Where:

*V*is the vector of line phase voltages.*I*is the vector of phase currents.*Z*is the series impedance matrix in per unit length.*Y*is the shunt admittance matrix in per unit length.

These are general solutions for the vector of currents and voltages.

$I\left(x\right)={e}^{-\text{\Psi}x}{C}_{1}+{e}^{\text{\Psi}x}{C}_{2}$ | (1) |

${Y}_{c}V\left(x\right)={e}^{-\text{\Psi}x}{C}_{1}-{e}^{\text{\Psi}x}{C}_{2}$ | (2) |

Where $$\text{\Psi}=\sqrt{YZ}$$ is the propagation matrix and ${Y}_{c}={(\sqrt{YZ})}^{-1}Y$ is the characteristic admittance.

Consider now a transmission line segment of length *x* =
*l*. At the beginning of one of its ends, when *x* =
*0*, the equations 1 and 2 are evaluated as follows.

${I}_{1}={C}_{1}+{C}_{2}$ | (3) |

${Y}_{c}{V}_{1}={C}_{1}-{C}_{2}$ | (4) |

The integration constant vectors *C _{1}* and

${C}_{1}=\frac{({I}_{1}+{Y}_{c}{V}_{1})}{2}$ | (5) |

${C}_{2}=\frac{({I}_{1}-{Y}_{c}{V}_{1})}{2}$ | (6) |

Similarly, at *x* = *l*, equations 1 and 2 are
evaluated as follows.

${I}_{2}={e}^{-\Psi \text{l}}{C}_{1}+{e}^{\Psi \text{l}}{C}_{2}$ | (7) |

${Y}_{c}{V}_{2}={e}^{-\Psi \text{l}}{C}_{1}-{e}^{\Psi \text{l}}{C}_{2}$ | (8) |

To obtain the two fundamental equations for the transmission line model, first you use equations 7 and 8 to perform this calculation.

${I}_{2}-{Y}_{c}{V}_{2}=-2{e}^{-\Psi l}{C}_{1}$ | (9) |

Then you substitute equation 5 into equation 9.

${I}_{2}-{Y}_{c}{V}_{2}=-H({I}_{1}+{Y}_{c}{V}_{1})$ | (10) |

Where $H={e}^{-\text{\Psi}l}$ is the propagation factor matrix. Equation 10 establishes the relation between voltages and currents at the terminals of a multi-conductor line section.

You can obtain a companion expression providing the model for the terminal 1 at
*x* = *0*.

${I}_{1}-{Y}_{c}{V}_{1}=-H({I}_{2}+{Y}_{c}{V}_{2})$ | (11) |

Define:

${I}_{sh,1}={Y}_{c}{V}_{1}$ — Shunt current vector produced at terminal 1 by injected voltages

*V*_{1}${I}_{sh,2}={Y}_{c}{V}_{2}$ — Shunt current vector produced at terminal 2 by injected voltages

*V*_{2}${I}_{rfl,1}=\frac{1}{2}({I}_{1}+{Y}_{c}{V}_{1})$ — Reflected currents of terminal 1

${I}_{rfl,2}=\frac{1}{2}({I}_{2}+{Y}_{c}{V}_{2})$ — Reflected currents of terminal 2

And finally rewrite equations 10 and 11 as follows:

${I}_{1}={I}_{sh,1}-2H{I}_{rfl,2}$

${I}_{2}={I}_{sh,2}-2H{I}_{rfl,1}$

These equations constitute a traveling wave line model for the segment of length L.

Particularly for transmission lines with ground return, the parameters are highly dependent on frequency. Model solutions are then carried out directly in the phase domain. The block computes automatically the impedance and the characteristic admittance matrices on the full frequency range, performing an approximation through rational fitting.

Rational fitting for this model is performed by using the vector fitting (VF)
procedure. For more information on the phase domain line model and the state-space
analysis, see *Wide-Band Line Model Implementation in Matlab for EMT
Analysis* [1].

Use the **Variables** settings to specify the priority and initial target
values for the block variables before simulation. For more information, see Set Priority and Initial Target for Block Variables.

[1] Ramos-Leanos, O, Iracheta R..
* Wide-Band Line Model Implementation in Matlab for EMT
Analysis*. Arlington, TX: IEEE North American Power Symposium
(NAPS), 2010.

[2] Ramos-Leanos, O.
* Wideband Line/Cable Models for Real-Time and Off-Line Simulations of
Electromagnetic Transients*. Diss. École Polytechnique de Montréal,
2013.

[3] Ramos-Leanos, O., J. L. Naredo, J.
Mahseredjian, I. Kocar, C. Dufour, and J. A. Gutierrez-Robles. * A wideband
line/cable model for real-time simulations of power system
transients*. IEEE Transactions on Power Delivery, 27.4 (2012):
2211-2218.

[4] Iracheta, R., and O. Ramos-Leanos.
* Improving computational efficiency of FD line model for real-time
simulation of EMTS*. Arlington, TX: IEEE North American Power
Symposium (NAPS), 2010.

[5] Dommel, H. W.
* Electromagnetic transients program (EMTP) theory
book*. Portland OR: Bonneville Power Administration, 1986

AC Cable (Three-Phase) | Coupled Lines (Three-Phase) | Transmission Line | Transmission Line (Three-Phase)