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EE1352 POWER SYSTEM ANALYSIS R.KALAIVANI EEE DEPARTMENT RAJALAKSHMI ENGINEERING COLLEGE RAJALAKSHMI NAGAR,THANDALAM 602 105
UNIT I ,[object Object]
Power system network
SINGLE LINE DIAGRAM ,[object Object]
COMPONENTS OF A POWER SYSTEM ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
MODELLING OF GENERATOR AND SYNCHRONOUS MOTOR 1 Φ  equivalent circuit of generator 1 Φ  equivalent circuit of synchronous motor
MODELLING OF TRANSFORMER =Equivalent resistance referred to 1 o =Equivalent reactance referred to 1 o
MODELLING OF TRANSMISSION LINE Π   type T  type
MODELLING OF INDUCTION MOTOR =Resistance representing load =Equivalent resistance referred to stator =Equivalent reactance referred to stator
per unit=actual value/base value Let KVA b =Base KVA kV b =Base voltage Z b =Base impedance in  Ω
Changing the base of per unit quantities ,[object Object],[object Object],Let   represent old base values represent new base values
 
ADVANTAGES OF PER UNIT CALCULATIONS ,[object Object],[object Object],[object Object],[object Object]
IMPEDANCE DIAGRAM ,[object Object],[object Object],[object Object],[object Object],[object Object]
REACTANCE DIAGRAM ,[object Object],[object Object],[object Object],[object Object]
REACTANCE DIAGRAM FOR THE GIVEN POWER SYSTEM NETWORK
PROCEDURE TO FORM REACTANCE DIAGRAM FROM SINGLE DIAGRAM ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
p.u. calculation of 3 winding transformer Zp=Impedance of primary winding Zs’=Impedance of secondary winding Zt’=Impedance of tertiary winding Short circuit test conducted to find out the above 3 impedances
= Leakage impedance measured in 1 o  with 2 o  short circuited and tertiary open.  = Leakage impedance measured in 1 o  with tertiary short circuited and 2 o  open.  = Leakage impedance measured in 2 o  with tertiary short circuited and 1 o  open and referred to primary
[object Object],[object Object]
PRIMITIVE NETWORK   ,[object Object]
BUS ADMITTANCE(Y BUS) MATRIX Y BUS can be formed by 2 methods 1.Inspection method 2.Singular transformation Y BUS =
INSPECTION METHOD ,[object Object],[object Object],[object Object]
SINGULAR TRANSFORMATION METHOD ,[object Object],[object Object],[object Object]
BUS CLASSIFICATION ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
ITERATIVE METHOD ,[object Object],[object Object],[object Object],[object Object],[object Object]
GAUSS SEIDAL METHOD For load bus   calculate |V| and  δ  from V p k+1  equation   For generator bus calculate Q from Q P K+1  equation
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
NEWTON RAPHSON METHOD
[object Object],[object Object],[object Object]
FAST DECOUPLED METHOD ,[object Object]
[object Object],[object Object],[object Object]
COMPARISION BETWEEN ITERATIVE METHODS ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
NEWTON – RAPHSON METHOD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
FAST DECOUPLED METHOD ,[object Object],[object Object],[object Object],[object Object],[object Object]
UNIT III ,[object Object]
[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object]
Procedure for calculating short circuit capacity and fault current ,[object Object],[object Object],[object Object]
ALGORITHM FOR SHORT CIRCUIT ANALYSIS USING BUS IMPEDANCE MATRIX ,[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object]
 
ALGORITHM FOR FORMATION OF THE BUS IMPEDANCE MATRIX ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
UNIT IV ,[object Object]
INTRODUCTION ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
FUNDAMENTALS OF SYMMETRICAL COMPONENTS ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
RELATIONSHIP BETWEEN UNBALANCED VECTORS AND SYMMETRICAL COMPONENTS Similarly we can obtain for currents also
SEQUENCE IMPEDANCE ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
SEQUENCE NETWORK ,[object Object],positive sequence network negative sequence network Zero sequence network
SEQUENCE NETWORK FOR TRANSMISSION LINE positive sequence network negative sequence network Zero sequence network
SEQUENCE NETWORK FOR TRANSFORMER positive sequence network negative sequence network Zero sequence network
SEQUENCE NETWORK FOR LOAD positive sequence network negative sequence network Zero sequence network
SINGLE LINE TO GROUND FAULT Consider a fault between phase a and ground through an impedance z f
LINE TO LINE (LL) FAULT Consider a fault between phase b and c through an impedance z f
DOUBLE LINE TO GROUND (LLG) FAULT Consider a fault between phase b and c  through an impedance z f  to ground
UNBALANCED FAULT ANALYSIS USING BUS IMPEDANCE MATRIX ,[object Object],[object Object],[object Object],For a fault at bus k the symmetrical components of fault current
LINE TO LINE (LL) FAULT Consider a fault between phase b and c through an impedance z f
DOUBLE LINE TO GROUND (LLG) FAULT Consider a fault between phase b and c  through an impedance z f  to ground
BUS VOLTAGES AND LINE CURRENTS DURING FAULT
[object Object],[object Object]
[object Object],[object Object],[object Object]
CLASSIFICATION OF STABILITY ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object]
Swing Equation for Single Machine Infinite Bus System ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object]
δ  and  ω s  are in electrical radian p.u p.u H=machine inertia constant
Swing Equation for Multimachine System p.u =machine rating(base) =system base
Rotor Angle Stability ,[object Object],[object Object],[object Object],[object Object]
Voltage Stability ,[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Equal Area Criterion ,[object Object],[object Object]
Factors Affecting Transient Stability ,[object Object],[object Object],[object Object]
Numerical Integration methods  ,[object Object],[object Object],[object Object]
EULER’S METHOD ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
MODIFIED EULER’S METHOD ,[object Object],[object Object],[object Object],[object Object]
Numerical Solution of the swing equation   ,[object Object],[object Object],[object Object]
The swing equation Applying Modified Eulers method to above equation
[object Object],The corrected value
Runge-Kutta Method ,[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]

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Newton Raphson

  • 1. EE1352 POWER SYSTEM ANALYSIS R.KALAIVANI EEE DEPARTMENT RAJALAKSHMI ENGINEERING COLLEGE RAJALAKSHMI NAGAR,THANDALAM 602 105
  • 2.
  • 4.
  • 5.
  • 6. MODELLING OF GENERATOR AND SYNCHRONOUS MOTOR 1 Φ equivalent circuit of generator 1 Φ equivalent circuit of synchronous motor
  • 7. MODELLING OF TRANSFORMER =Equivalent resistance referred to 1 o =Equivalent reactance referred to 1 o
  • 8. MODELLING OF TRANSMISSION LINE Π type T type
  • 9. MODELLING OF INDUCTION MOTOR =Resistance representing load =Equivalent resistance referred to stator =Equivalent reactance referred to stator
  • 10. per unit=actual value/base value Let KVA b =Base KVA kV b =Base voltage Z b =Base impedance in Ω
  • 11.
  • 12.  
  • 13.
  • 14.
  • 15.
  • 16. REACTANCE DIAGRAM FOR THE GIVEN POWER SYSTEM NETWORK
  • 17.
  • 18. p.u. calculation of 3 winding transformer Zp=Impedance of primary winding Zs’=Impedance of secondary winding Zt’=Impedance of tertiary winding Short circuit test conducted to find out the above 3 impedances
  • 19. = Leakage impedance measured in 1 o with 2 o short circuited and tertiary open. = Leakage impedance measured in 1 o with tertiary short circuited and 2 o open. = Leakage impedance measured in 2 o with tertiary short circuited and 1 o open and referred to primary
  • 20.
  • 21.
  • 22. BUS ADMITTANCE(Y BUS) MATRIX Y BUS can be formed by 2 methods 1.Inspection method 2.Singular transformation Y BUS =
  • 23.
  • 24.
  • 25.
  • 26.
  • 27. GAUSS SEIDAL METHOD For load bus calculate |V| and δ from V p k+1 equation For generator bus calculate Q from Q P K+1 equation
  • 28.
  • 30.
  • 31.
  • 32.
  • 33.
  • 34.
  • 35.
  • 36.
  • 37.
  • 38.
  • 39.
  • 40.
  • 41.
  • 42.
  • 43.  
  • 44.
  • 45.
  • 46.
  • 47.
  • 48.
  • 49.
  • 50.
  • 51. RELATIONSHIP BETWEEN UNBALANCED VECTORS AND SYMMETRICAL COMPONENTS Similarly we can obtain for currents also
  • 52.
  • 53.
  • 54. SEQUENCE NETWORK FOR TRANSMISSION LINE positive sequence network negative sequence network Zero sequence network
  • 55. SEQUENCE NETWORK FOR TRANSFORMER positive sequence network negative sequence network Zero sequence network
  • 56. SEQUENCE NETWORK FOR LOAD positive sequence network negative sequence network Zero sequence network
  • 57. SINGLE LINE TO GROUND FAULT Consider a fault between phase a and ground through an impedance z f
  • 58. LINE TO LINE (LL) FAULT Consider a fault between phase b and c through an impedance z f
  • 59. DOUBLE LINE TO GROUND (LLG) FAULT Consider a fault between phase b and c through an impedance z f to ground
  • 60.
  • 61. LINE TO LINE (LL) FAULT Consider a fault between phase b and c through an impedance z f
  • 62. DOUBLE LINE TO GROUND (LLG) FAULT Consider a fault between phase b and c through an impedance z f to ground
  • 63. BUS VOLTAGES AND LINE CURRENTS DURING FAULT
  • 64.
  • 65.
  • 66.
  • 67.
  • 68.
  • 69.
  • 70. δ and ω s are in electrical radian p.u p.u H=machine inertia constant
  • 71. Swing Equation for Multimachine System p.u =machine rating(base) =system base
  • 72.
  • 73.
  • 74.
  • 75.
  • 76.
  • 77.
  • 78.
  • 79.
  • 80.
  • 81. The swing equation Applying Modified Eulers method to above equation
  • 82.
  • 83.
  • 84.