Data Requirements For Calculating Geomagnetically Induced Currents PGDTF Meeting March 21, 2016 Michael Juricek PGDTF Chairman 1.

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Data Requirements For Calculating Geomagnetically Induced Currents PGDTF Meeting March 21, 2016 Michael Juricek PGDTF Chairman 1

Space Storm 2Michael Juricek – 3/21/2016 PGDTF Meeting

What are Geomagnetically Induced Currents (GIC)? Highly charged cloud of plasma is ejected from the sun – coronal mass ejection (CME) Some of the plasma enters the earth’s ionosphere The electro-magnetic interaction with earth’s magnetic field results in time varying electrojets of current in the ionosphere producing the auroras The fluctuating electrojet currents induce voltages and currents in the earth’s crust and electric transmission systems Michael Juricek – 3/21/2016 PGDTF Meeting3

What are Geomagnetically Induced Currents (GIC)? Induced voltage in the earth causes GIC in the lines Currents are “zero sequence” “quasi dc” currents Not displaced by 120 degrees like 60 Hz load currents To flow the currents need a path to circulate Path is typically provided by transformers and shunt grounding connections TSPs and Resource Entities are affected Michael Juricek – 3/21/2016 PGDTF Meeting4

Major Geomagnetic Storms in Past 1859 Carrington Storm Damaged telegraph systems Some operated without damaged batteries Sparks shocked operators and caused fires Lasted for 12 days 1921 Storm Less severe than 1859, but still damaged telegraph systems March 13, 1989 Storm 1/10 th strength of 1921 storm Damaged transformers in USA and other countries Blackout in Canada (Hydro Quebec/Hydro One) in 92 seconds Auroral zone expanded to Gulf Coast Michael Juricek – 3/21/2016 PGDTF Meeting5

GIC data files for PSS/E Model GIC Data File Identification Data Substation Data Bus Substation Data Transformer Data Bus Fixed Shunt Data Branch Data User Earth Model Data Michael Juricek – 3/21/2016 PGDTF Meeting6

GIC Data Required data from TSPs and Resource Entities Geographic location of substations (longitude and latitude) Grounding resistance data for substations Bus substation numbers (allows all substation components in one location to be grouped together into one substation) DC resistance of transformer windings Winding grounding dc resistance Identification of GIC blocking device in the grounding connection Transformer vector group Bus Shunts DC resistance of transmission lines Number of cores in transformer K Factor Michael Juricek – 3/21/2016 PGDTF Meeting7

Substation Data I, NAME, UNIT, LATITUDE, LONGITUDE, RG, EARTHMDL Where: Michael Juricek – 3/21/2016 PGDTF Meeting8 ISubstation Number NAMESubstation Name UNITUnit for geophysical location (latitude and longitude) data = 0 for degrees At this time, only allowed unit for latitude and longitude is degrees. LATITUDESubstation latitude, positive for North and negative for South LONGITUDESubstation longitude, positive for East and negative for West RGSubstation grounding resistance, Default =0.1 ohm If RG =99.0, assumed that substation is ungrounded EARTHMDLName of the Earth Model

Bus Substation Data BUSNUM, SUBNUM Where: Michael Juricek – 3/21/2016 PGDTF Meeting9 BUSNUMBus Number SUBNUM Substation Number. This is a substation number to which bus “BUSNUM” belongs to. The following restrictions apply: Two buses connected by a transmission line (non-transformer branch) must be in different substations. Two buses connected by a two winding transformer must be in same substation. Three buses connected by a three winding transformer must be in same substation. Two buses connected by zero impedance line must have same substation number.

Bus Substation Data Michael Juricek – 3/21/2016 PGDTF Meeting10

Bus Substation Data Michael Juricek – 3/21/2016 PGDTF Meeting11

12 Source: Siemens PTI 2012 Substation Data Example Michael Juricek - 3/21/2016 PGDTF Meeting

13 Source: Siemens PTI 2012 Bus Substation Data Michael Juricek - 3/21/2016 PGDTF Meeting

Transformer Data I, J, K, CKT, WRI, WRJ, WRK, GICBDI, GICBGJ, GICBDK, VECGRP, CORE, KFACTOR, GRDWRI, GRDWRJ, GRDWRK, TMODEL Where: Michael Juricek – 3/21/2016 PGDTF Meeting 14 IWinding Bus Number 1 JWinding Bus Number 2 KWinding Bus Number 3 CKTAlphanumeric Circuit Identifier WRIDC Resistance of Winding 1 in ohms/phase. When WRI is not specified, load flow data resistance is used. WRJDC Resistance of Winding 2 in ohms/phase. When WRJ is not specified, load flow data resistance is used. WRKDC Resistance of Winding 3 in ohms/phase. When WRK is not specified, load flow data resistance is used. GICBDIGIC blocking device in neutral of Winding 1 GICBDJGIC blocking device in neutral of Winding 2 GICBDKGIC blocking device in neutral of Winding 3 VECGRPAlphanumeric identifier specifying vector group based on transformer winding grounding connections and phase angles. CORENumber of cores. This data used to calculate transformer reactive power loss from GIC flowing in winding KFACTORFactor to calculate transformer reactive power loss from GIC flowing through winding (MVAR/AMP) GRDWRIWinding 1 grounding DC resistance in ohms GRDWRJWinding 2 grounding DC resistance in ohms GRDWRKWinding 3 grounding DC resistance in ohms TMODELTransformer Model in GIC DC Network

Bus Fixed Shunt Data I, ID, R, RG Where: Michael Juricek – 3/21/2016 PGDTF Meeting15 IBus Number IDAlphanumeric shunt identifier RDC resistance in ohm/phase. RGGrounding DC resistance in ohms

16 Source: Siemens PTI 2012 Transformer MVAR Scaling Factors Michael Juricek - 3/21/2016 PGDTF Meeting

17 Source: Siemens PTI 2012 Transformer Data Example Michael Juricek - 3/21/2016 PGDTF Meeting

Branch Data I, J, CKT, RBRN, INDVP, INDVQ Where: Michael Juricek – 3/21/2016 PGDTF Meeting18 IBranch from bus number JBranch to bus number CKTAlphanumeric branch circuit identifier RBRNBranch DC resistance in ohms/phase. When RBRN is not specified, load flow data branch resistance is used as is. INDVPReal part of total branch GMD induced electric field in volts. INDVQImaginary part of total branch GMD induced electric field in volts.

User Earth Model Data NAME, BETAFTR, DESC, RESISTIVITY1, THICKNESS1, RESISTIVITYn, THICKNESSn Where: Michael Juricek – 3/21/2016 PGDTF Meeting19 NAMEAlphanumeric identifier assigned to this earth model. BETAFTREarth Model scaling factor used when calculating branch induced electric field for Benchmark GMD event. DESCDescription of the earth model. RESISTIVITY1Layer 1 Resistivity in ohm-m. THICKNESS1Layer 1 Thickness in km. RESISTIVITYnNth Layer Resistivity in ohm-m. Up to 25 layers allowed. THICKNESSnNth Layer Thickness in km. Up to 25 layers allowed.

Default Data Versus Actual Data Software developer used actual data to develop default data which is assumed conservative data Default data may produce higher GICs and reactive loading than actual data Experienced TSPs highly recommend actual data Consultants highly recommend actual data PGDTF has decided to use actual data, where possible Michael Juricek – 3/21/2016 PGDTF Meeting20

Proposed Modeling Schedule June 1 – TSPs and REs start providing data to ERCOT November 1 – All data must be submitted to ERCOT Michael Juricek – 3/21/2016 PGDTF Meeting21

Questions and Answers 22Michael Juricek – 3/21/2016 PGDTF Meeting

Appendix Michael Juricek - 3/21/2016 PGDTF Meeting23

FERC March 1, 2016 Technical Conference FERC commissioners and staff participated Benchmark GMD event and geomagnetic fields Earth conductivity model Harmonics and vibrational effects during benchmark GMD events Selection of 75 Ampere threshold for thermal assessments Modeling capabilities regarding transformer thermal assessments Non-uniform geoelectric fields Corrective action plans Current state of monitoring Potential for additional monitoring Improvement in modeling and analysis tools Michael Juricek – 3/21/2016 PGDTF Meeting24

FERC March 1, 2016 Technical Conference continued Comments Adopt standard as proposed and revise as better data and analysis techniques indicate Make benchmark event more severe in standard Lower GIC threshold for transformer thermal assessment such as 15 Amperes in standard Use actual GIC data to validate benchmark event Increase monitoring of GIC geomagnetic fields and geoelectric fields Improve earth models Provide real-time GIC readings to control rooms Study multiple GMD scenarios to determine the system’s strength Share GIC measurements with public Michael Juricek – 3/21/2016 PGDTF Meeting25