lecture sc

Upload: fedilino-p-fornolles

Post on 02-Apr-2018

215 views

Category:

Documents


0 download

TRANSCRIPT

  • 7/27/2019 Lecture Sc

    1/8

  • 7/27/2019 Lecture Sc

    2/8

    5

    Symmetrical short circuit transienton a transmission line

    Resulting currents

    6

    New features in this course

    9 DC components

    Top values

    Modeling of synchronous machines

    Other types of faults

    7

    Maximum current (R is small)

    Resulting currents

    2 2peak x y ac RMSI I I I = + =

    8

    Maximum RMS current (R is small)

    2 2

    RMS ac RMS dc RMSI I I = +

    2

    dc RMS Y Y I I I = =

    2

    2 2 2 31 322 2

    X XRMS Y X X ac RMSI II I I I I

    = + = + = =

  • 7/27/2019 Lecture Sc

    3/8

    9

    Different fault angles in differentphases => Maximum not in allphases at the same time

    10

    New features in this course

    9 DC components

    9 Top values

    Modeling of synchronous machines

    Other types of faults

    11

    Short circuit ona synchronousmachine

    12

    Short circuit on a synchronous machine

  • 7/27/2019 Lecture Sc

    4/8

    13

    Short circuit on a synchronous machine

    14

    New features in this course

    9 DC components

    9 Top values

    9 Modeling of synchronous machines

    Other types of faults

    15

    Differentfaulttypes

    16

    Single line-to-ground fault, SLGF

  • 7/27/2019 Lecture Sc

    5/8

    17

    Double line-to-ground faults

    18

    Symmetrical components (basic course)

    The transformation matrix for symmetrical

    components

    19

    Example 12.4

    Find the subtransient currents and the line-to-line voltages at the fault under subtransientconditions when a double line-to-ground fault

    with Zf=0 occurs at the terminals of machine 2in the system below. Assume that the system isunloaded and operating at rated voltage whenthe fault occurs. Neglect resistance.

    20

    1. Build an impedance diagram each for the positive-, negativeand zero-sequence systems, for the entire network except for

    the un-symmetrical load.2. Calculate the Thvenin-equivalent for the positive-,negative-

    and zero-sequences at the bus where the un-symmetricalload is located.

    3. Calculate the positive-, negative- and zero- sequencecurrents through the load.

    4. Calculate the positive-, negative- and zero- sequencevoltages at the locations that are of interest

    5. Calculate the positive-, negative- and zero-sequence currentsthrough components that are of interest

    6. Transform those symmetrical components to phase-quantities that are asked for.

    Analysis of a network with one un-symmetrical load (basic course)

  • 7/27/2019 Lecture Sc

    6/8

    21

    Example12.4

    Pos. seq.

    Zero seq.

    Neg. seq.= pos. -Vf

    22

    Example12.4

    Pos. seq.

    Zero seq.

    Neg. seq.= pos. -Vf

    23

    Considerations regardingneutral grounding

    Fault currents Voltage on healthy phases

    Suppression of arcing faults

    Interference with communication (EMC)

    24

    Assume a grid

    Z=?

    YZ

    Loads

    Z=?

  • 7/27/2019 Lecture Sc

    7/8

    25

    Neutral grounding

    Isolated neutral (no grounding)

    Grounding through resistor

    Grounding through reactor (Petersen coil)

    Solidly grounded

    26

    Isolated NeutralResistor grounded

    Very high Z

    1

    1 2

    33

    1shU

    I j CU

    Z Zj C

    = + +

    YZ

    Long lines => large C => large capacitive Ish-1

    C

    Resistor grounded => identify faulty part

    Healthy phases 3 phaseU U=

    Ua=0

    27

    Isolated Neutral (Resistorgrounded)

    Small systems Small fault current (SLGF)

    High voltages on healthy phases at faults(SLGF)

    28

    Petersen coilZ = jX

    0

    1 13

    1

    3

    Z j Xj C

    j CjX

    = = = +

    &

    YZ

    Long lines => large C

    C

    if

    Healthy phases 3 phaseU U=

    1 1

    3 3C X

    X C

    = =

  • 7/27/2019 Lecture Sc

    8/8

    29

    Grounded through reactor(Petersen coil)

    Distribution networks

    Arcing faults could be clearedautomatically

    Small fault currents (SLGF)

    High voltages on healthy phases (SLGF)

    30

    Solidly groundedZ = 0

    YZ

    Long lines => large C

    C

    Healthy phasesphase

    U U=

    1

    1 21 2

    3 3

    1(3 0 )

    sh

    TT

    U UI

    Z Z ZZ Z Z

    j C

    = =+ ++ + +&

    = large

    31

    Solidly grounded systems

    Subtransmission and transmission systems

    Large fault currents (SLGF)

    Voltages on healthy phases limited (SLGF)