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IMPLICATIONS OF LOAD ANGLE &
EXCITATION ON GENERATOR STABILITY,
    SIGNIFICANCE OF GENERATOR
         CAPABILITY CURVE



          PREPARED BY: -
           KUNAL GUPTA
            DGM(EMD)
WHAT IS LOAD ANGLE ?

• Load Angle δ is the angle between the Generator induced
  E.M.F & Generator terminal voltage.
• Physically, this is the angle by which the reference line
  made on the Generator shaft front deviates from no load-
  to-load condition.
D

              EG               IXS   φ


    δ              V
A                         B              C
    φ


          I

                   FIG – (I)
        Vector Diagram of Generator
          parameters with lagging
                power factor
GENERATOR PARAMETER DETAILS AS
           DEPICTED IN FIG (I)

• AD = EG = Generator Induced E.M.F.
• I = Generator Stator Current.
• AB = V = Generator Terminal Voltage.
• XS = Generator Synchronous Reactance.
• φ = Angle between Generator Terminal Voltage V &
  Stator Current I. (COS φ = p.f).
• δ = Load Angle.
EQUATION OF POWER CURVE

• CD = IX S COS φ = E G SIN δ -------(i)
• Active Power P = VI COS φ = VE G SIN δ (From i
  above)                                  XS
• From above, it becomes clear that the power curve
  with reference to excitation shall be a sinusoidal one
  as EG is proportional to Generator Excitation.
• BC = IX S SIN φ = E G COS δ __ V -------(ii)
• Reactive Power Q = VI SIN φ        = VE G COS δ / XS
  __ V 2 / XS (From ii above)
• It is apparent that Reactive Power Q shall be equal to
  ( __ V 2 / XS ) when EG = 0.
P max at load
                                               angle δ = 90
P (Power )                         P2            Degree.
                           P1




             δ1 δ2
                                    Load Angle δ

                      FIG – (II)
                     Power Curve
POWER CURVE CHARACTERISTICS

• From FIG (II), it becomes evident that with constant
  Excitation, maximum power would be generated at
  δ=900 .
• As the power increases from P1 to P2, the reference
  load angle increases from δ1 to δ2.
• The Generator operates on stable zone up to the
  time dP/dδ is positive, i.e., up to δ=900.
• This is the reason to operate the Generator with load
  angle limiter control, which limits the load in case the
  load angle tends to cross the design value.
P (Power )                          P2


                           P1


             δ1 δ2
                                     Load Angle δ

                      FIG – (III)
                     Power Curve
POWER CURVE CHARACTERISTICS

• From FIG (III), it is quite clear that with constant
  power generation P1, if the excitation is boosted up,
  then load angle shall reduce from δ2 to δ1.
• Also, with same load angle δ2, power generation
  increment is possible from P1 to P2 with boosting up
  of excitation.
• As changing Generator Excitation is done primarily
  by A.V.R, the load angle at which the Generator is
  safe to operate is determined by the A.V.R response.
• With fast acting A.V.R, Generator can be operated at
  higher load angle & vice versa.
• However, boosting up of excitation shall be limited to
  the design value only.
D

                             φ
    EG           I     IXS
        δ

    φ           V
A                                B
            C


                FIG – (IV)
     Vector Diagram of Generator
    parameters with leading power
                factor
EFFECT OF NEGATIVE REACTIVE POWER
           ON GENERATOR

• From FIG (IV), it is evident that EG reduces when
  stator current I leads the terminal voltage V. This is
  the situation when the Generator is subjected to
  negative reactive MVAR.
• In such case, Grid no longer require MVAR from
  Generator, rather it exports MVAR to the connected
  machines, causing reduction of Generator excitation.
• As it is shown in FIG (III) that for constant power,
  reduction of EG means increase in load angle δ, the
  capability of the Generator to absorb reactive MVAR
  at a particular load is subjected to load angle
  limitation.
MW

                                         C
                     F


                                    VI
    EGV / XS
                           φ
A        δ                                   G   MVAR
      V 2 / XS   E        B


                    FIG – (V)
                    Generator
                 Capability Curve
GENERATOR CAPABILITY CURVE
• By multiplying FIG (I) by V / XS, we do arrive at FIG (V).
• EFCG depicts the Generator capability curve.
• Load angle limiter limits the negative reactive MVAR as
  shown by the line EF.
• Rotor current limiter limits the rotor current & is
  depicted by CG which is the arc of AC with A as center
  & is proportional to Generator excitation as well as the
  rotor current.
• Stator current limiter limits the stator current as shown
  by FC, which is the arc of BC with B as center & is
  proportional to stator current.
• All these limiters ensure that the Generator, at any
  point of time, operates within the framework EFCG for
  electrical as well as thermal stability of the machine.
Generator capability curve

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Generator capability curve

  • 1. IMPLICATIONS OF LOAD ANGLE & EXCITATION ON GENERATOR STABILITY, SIGNIFICANCE OF GENERATOR CAPABILITY CURVE PREPARED BY: - KUNAL GUPTA DGM(EMD)
  • 2. WHAT IS LOAD ANGLE ? • Load Angle δ is the angle between the Generator induced E.M.F & Generator terminal voltage. • Physically, this is the angle by which the reference line made on the Generator shaft front deviates from no load- to-load condition.
  • 3. D EG IXS φ δ V A B C φ I FIG – (I) Vector Diagram of Generator parameters with lagging power factor
  • 4. GENERATOR PARAMETER DETAILS AS DEPICTED IN FIG (I) • AD = EG = Generator Induced E.M.F. • I = Generator Stator Current. • AB = V = Generator Terminal Voltage. • XS = Generator Synchronous Reactance. • φ = Angle between Generator Terminal Voltage V & Stator Current I. (COS φ = p.f). • δ = Load Angle.
  • 5. EQUATION OF POWER CURVE • CD = IX S COS φ = E G SIN δ -------(i) • Active Power P = VI COS φ = VE G SIN δ (From i above) XS • From above, it becomes clear that the power curve with reference to excitation shall be a sinusoidal one as EG is proportional to Generator Excitation. • BC = IX S SIN φ = E G COS δ __ V -------(ii) • Reactive Power Q = VI SIN φ = VE G COS δ / XS __ V 2 / XS (From ii above) • It is apparent that Reactive Power Q shall be equal to ( __ V 2 / XS ) when EG = 0.
  • 6. P max at load angle δ = 90 P (Power ) P2 Degree. P1 δ1 δ2 Load Angle δ FIG – (II) Power Curve
  • 7. POWER CURVE CHARACTERISTICS • From FIG (II), it becomes evident that with constant Excitation, maximum power would be generated at δ=900 . • As the power increases from P1 to P2, the reference load angle increases from δ1 to δ2. • The Generator operates on stable zone up to the time dP/dδ is positive, i.e., up to δ=900. • This is the reason to operate the Generator with load angle limiter control, which limits the load in case the load angle tends to cross the design value.
  • 8. P (Power ) P2 P1 δ1 δ2 Load Angle δ FIG – (III) Power Curve
  • 9. POWER CURVE CHARACTERISTICS • From FIG (III), it is quite clear that with constant power generation P1, if the excitation is boosted up, then load angle shall reduce from δ2 to δ1. • Also, with same load angle δ2, power generation increment is possible from P1 to P2 with boosting up of excitation. • As changing Generator Excitation is done primarily by A.V.R, the load angle at which the Generator is safe to operate is determined by the A.V.R response. • With fast acting A.V.R, Generator can be operated at higher load angle & vice versa. • However, boosting up of excitation shall be limited to the design value only.
  • 10. D φ EG I IXS δ φ V A B C FIG – (IV) Vector Diagram of Generator parameters with leading power factor
  • 11. EFFECT OF NEGATIVE REACTIVE POWER ON GENERATOR • From FIG (IV), it is evident that EG reduces when stator current I leads the terminal voltage V. This is the situation when the Generator is subjected to negative reactive MVAR. • In such case, Grid no longer require MVAR from Generator, rather it exports MVAR to the connected machines, causing reduction of Generator excitation. • As it is shown in FIG (III) that for constant power, reduction of EG means increase in load angle δ, the capability of the Generator to absorb reactive MVAR at a particular load is subjected to load angle limitation.
  • 12. MW C F VI EGV / XS φ A δ G MVAR V 2 / XS E B FIG – (V) Generator Capability Curve
  • 13. GENERATOR CAPABILITY CURVE • By multiplying FIG (I) by V / XS, we do arrive at FIG (V). • EFCG depicts the Generator capability curve. • Load angle limiter limits the negative reactive MVAR as shown by the line EF. • Rotor current limiter limits the rotor current & is depicted by CG which is the arc of AC with A as center & is proportional to Generator excitation as well as the rotor current. • Stator current limiter limits the stator current as shown by FC, which is the arc of BC with B as center & is proportional to stator current. • All these limiters ensure that the Generator, at any point of time, operates within the framework EFCG for electrical as well as thermal stability of the machine.