T2 C Power Flow Control

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    Power Flow Control Using

    Distributed Saturable Inductors

    Aleks Dimitrovski

    ORNL

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    Power System Flows

    ,S SP Q

    /S

    V 0/R

    V Z jX

    2 cossinS R S S RS S

    V V V V V P Q

    X X

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    Simple Example

    3 x 150 MVA lines supply 250 MW load

    All lines: z= 0.125 + j0.52 /mi, y= j6.8 S/mi

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    Simple Example

    Uncontrolled Power Flow

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    Uncontrolled Flows Cause Problems

    Overloading of lines and transformers

    Reduced security margins

    Power exchange contractual violations

    Increased fault levels beyond rating

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    and Inefficiencies

    Increased system losses

    Reduced power transfer capabilities

    Opposite reactive power flows

    Loop flows

    loop flow,reactive power

    actual realpower transfer

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    Limited Flow Control

    Switching elements on/off Regulating Transformers

    Off-nominal turns ratio

    Phase-shifters

    Switchable shunt/series capacitors andinductors

    FACTS - Flexible AC Transmission SystemDevices

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    FACTS Devices Expensive and Bulky

    100 MVAr

    STATCOM

    84 MVArCap Bank

    TVA Sullivan S/S near Johnson City

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    Air-Core Inductors Cheaper but Coarse

    PNM Norton S/S near LANL

    15 Air-CoreSeries Inductor

    14,500 lbs

    7 ft

    6 ft

    10 ft

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    Cost Comparison

    Norton air-core inductor,120 MVA:~ $1,000,000 (current estimate)

    Equivalent FACTS device:

    > $10,000,000

    This proposal:

    ~ $100,000

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    Simple Example

    Inductor Controlled Power Flow

    24.9 (66 mH)

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    Simple Example

    Different Load Distribution inductor On

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    Simple Example

    Different Load Distribution inductor Off

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    Simple Example

    Different Load Distribution inductor Changed

    14.8 (39 mH)

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    Iac Nac

    l

    Ndc

    DC Source

    Power line

    (controlled circuit)

    Idc

    dc bias flux

    control circuit

    A

    mdcac

    Magnetic Amplifier

    2

    ( )

    acac

    dc

    N AL constl

    f I

    m m

    m

    ac circuit inductance :

    controlled by dc circuit current :

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    BH Curve of Ferromagnetic Core

    1~2 T

    B

    H

    small

    Idc1 < Idc2

    large

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    Iac

    ac

    Nac/2

    Ndc/2

    DC Source

    Idc

    Nac/2

    Ndc/2

    acdc dc

    Symmetrical Connection

    Equal performance in both half-cycles

    Cancellation of the induced voltage in the dc circuit

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    Iac

    ac

    Nac/2

    DC Source

    Idc

    Nac/2

    Ndc dc

    Single-Core Symmetrical Connection

    Three-legged core

    No induced voltage in the dc circuit

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    Iac

    ac

    Ndc/2

    DC Source

    Idc

    Ndc/2Nac

    dc gaps

    Single-Core with Swapped Windings

    Exclusive path for ac flux instead of dc through the middle leg

    Bias dc flux not impeded by gaps in the core

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    Local DC Saturation

    Iac

    Nacl

    Ndc/2

    Idc

    dc

    ac

    Ndc/2

    gaps

    DCS

    ource

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    Conclusions

    Magnetic amplifier based device for continuouspower flow control

    Combination of proven and familiar conceptswith new technology

    Cheap enough for system-wide deploymentand comprehensive power flow control

    Makes the grid part smart in smart grid,besides generation and load