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SCRX


Description

This is a general model of a static excitation system representing a Silicon-Controlled Rectifier. The exciter may be bus fed or solid fed. The model was described in [1] as part of study for load rejection over-voltages. The SCRX component was developed in line with the references [1] [2].

Mask and Parameters

Exciter Parameters

Expanding the "SCRX diagram" displays the block diagram in the parameters window.

Name

Description

Unit

Variable = {Possible Values}

Ta_Tb

Gain reduction ratio Ta/Tb

-

-

Tb

Time constant

s

-

K

Exciter gain

-

-

Te

Time constant

s

-

Emax

Maximum field voltage output

pu

-

Emin

Minimum field voltage output

pu

-

Cswitch

Voltage source switch – Bus fed = 0, Solid fed = 1.

-

[0, 1]

Rc_Rfd

Ratio of the crowbar resistance to field winding resistance Rc/Rfd

-

-

The choice of the Cswitch parameters switches the voltage signal between bus fed, which is the generator terminal voltage, or solid fed, which is a 1.0 pu signal.

The negative current logic switches the operation of the exciter between allowing or blocking the negative field current, Ifd. When bidirectional Ifd is allowed, the exciter represents two rectifier bridges connected in reverse polarity to allow for Ifd to flow in both directions. On the other hand, if unidirectional Ifd is allowed, the excitation system represents a single bridge rectifier. In the uni-directional case, the bridge is protected by a crowbar circuit with a resistance Rd and a reverse bypassing thyristor [1]. The logic depends on the value of the ratio of the crowbar resistance to the field winding resistance, Rc_Rfd. If Rc_Rfd = 0, then negative Ifd is allowed. In this case, Efd = Ex in all cases. On the other hand, if Rc_Rfd > 0, then the logic depends on the sign of the Ifd. If Ifd is positive, then Efd = Ex. Otherwise, if Ifd is negative, then Efd = – XadIfd*Rc_Rfd.

Initial Value Parameters


Name

Description

Unit

Parameter Range

Efd0

Exciter output voltage initial value

pu

--

The parameters Efd0 can be set manually, by entering a numerical value. It can also be set automatically based on load flow calculations, by entering a referenced synchronous machine variable. For instance, if the name of the synchronous machine on which the excitation system is connected is “SM1”, then Efd0 shall be set as “=SM1.EfdInit” if a thermal machine or a hydraulic machine is used, and as "=SM1.EFD_Init" if a pu standard or pu fundamental machine is used.

The HYPERSIM simulation option “Set Initial Conditions” must be checked for the automatic initialization to work properly.

Inputs and Outputs and Additional Signals Available for Monitoring

Inputs

NameDescription

Unit

Voel*

Overexcitation limiter output

pu

Vc1

Signal proportional to compensated terminal voltage. If a load compensator block is not used upstream from the exciter block, then Vc1 is equal to Vt (main alternator terminal voltage)

pu

Vuel*

Underexcitation limiter output

pu

Vref

Voltage regulator reference voltage

pu

Vs

Output voltage of a Power System Stabilizer (PSS)

pu

Ifd**

Synchronous machine field current

pu

Vd

d-axis component of generator terminal voltage

pu

Vq

q-axis component of generator terminal voltage

pu

*Vuel and Voel are normally inputs to the excitation system but the user has the option to use a fixed constant value directly in the component mask by choosing “internal”.

**The observable field current Ifd from the synchronous machine in HYPERSIM needs to be multiplied by the machine’s Xad = Xd – Xl prior to its input to the exciter.


The terminal voltage calculation is performed in terms of Vd and Vq using the following equation:

Outputs

NameDescription

Unit

Efd

Exciter output voltage

pu


References

1. F.P. de Mello, L. M. Leuzinger and R. J. Mills, "Load rejection overvoltages as affected by excitation system control," in IEEE Transactions on Power Apparatus and Systems, vol. 94, no. 2, pp. 280-287, March 1975, doi: 10.1109/T-PAS.1975.31853. 

2. PSS®E 34.2.0 Model Library. NY, USA: Siemens Industry, Inc., 2017.

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