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PRESENTED BY:- 
Bhupendra Kumar 
Integrated M.Tech.
Contents 
 Basic concepts and definitions 
 Classification of power system stability 
 Rotor angle stability 
 Transient stability analysis 
 Voltage stability 
 Voltage collapse 
 Factors affecting voltage stability 
 Classification of voltage stability 
 Small signal stability
 Stability of dynamic systems 
 Dynamic stability analysis 
 Effect of excitation system 
 Power system stabilizers 
 Control of PSS 
 Applications of PSS 
 AESOPS algorithm 
 MAM method 
 Characteristics of small signal stability problem 
 References and bibliography
BASIC CONCEPTS AND DEFINITIONS 
 Power system stability may be broadly defined as 
that property of a power system that enables it to 
remain in a state operating equilibirium under normal 
operating conditions and to regain an acceptable 
state of equilibirium after being subjected to a 
disturbance. 
 Instability in a power system may be manifested in 
many different ways depending on the system 
configuration and operating mode. 
 Traditionally ,the stability problem has been one of 
maintaining Synchronus operation.
BASIC CONCEPTS AND 
DEFINITIONS(cont..) 
 Since power system rely on synchronus machines for 
electrical power generation, a necessary condition for 
satisfactory system is that all syn. machines should 
remain in synchronism. 
 This aspect of stability is influenced by the dynamics 
of generators rotor angles and power-angle 
relationships. 
 Instability may also encountered without loss of 
synchronism. For example a system consisting of a 
synchronus generator feeding an induction motor 
load through a transmission line can become 
unstable because of the collapse of load voltage.
BASIC CONCEPTS AND 
DEFINITIONS(cont..) 
 In the evaluation of stability the concern is the behavior of 
the power system when subjected to a transient 
disturbance. The disturbance may be small or large. 
 Small disturbances in the form of load changes take place 
continually, and the system adjusts itself to the changing 
conditions. 
 The system must be able to operate under these changes 
and also be capable of surviving numerous disturbances of 
severe nature, such as short- ckt. on transmission line, loss 
of a large generator or load , or loss of a tie between two 
subsystems.
Classification Of Power 
System Stability
ROTOR ANGLE STABILITY 
 Rotor angle stability is the ability of synchronous 
machines of a power system to remain in 
synchronism. 
 In other words, rotor angle or load angle stability 
denotes the angular displacement between stator 
and rotor speeds. 
 It is directly proportional to the speed of the m/c i.e. 
the load connected to the generator. 
 If the Angle is beyond to liable limit, the system will 
come out of synchronism.
Transient Stability Analysis 
 For transient stability analysis we need to consider 
three systems 
1. Prefault - before the fault occurs the system is 
assumed to be at an equilibrium point 
2. Faulted - the fault changes the system equations, 
moving the system away from its equilibrium point 
3. Post fault - after fault is cleared the system 
hopefully returns to a new operating point
VOLTAGE STABILITY & VOLTAGE 
COLLAPSE 
 Voltage Stability-It refers to the ability of the 
system to maintain a steady frequency, following a 
system drastic change resulting in a significant 
imbalance between generated and demand power 
 Voltage stability margins-
Factors affecting voltage stability 
 Voltage stability is a problem in power systems which are 
heavily loaded, faulted or have a shortage of reactive 
power. 
 The nature of voltage stability can be analyzed by examining 
the production, transmission and consumption of reactive 
power. 
 The reactive characteristics of AC transmission lines, 
transformers and loads restrict the maximum of power 
system transfers. 
 The power system lacks the capability to transfer power 
over long distances or through high reactance due to the 
requirement of a large amount of reactive power at some 
critical value of power or distance.
Scenario of classic voltage collapse 
 The large disturbance causes the network characteristics to 
shrink dramatically. The characteristics of the network and 
load do not intersect at the instability point. A load increase 
beyond the voltage collapse point results in loss of 
equilibrium, and the power system can no longer operate. This 
will typically lead to cascading outages. 
 The load voltage decreases, which in turn decreases the load 
demand and the loading of EHV transmission lines. The 
voltage control of the system, however, quickly restores 
generator terminal voltages by increasing excitation. The 
additional reactive power flow at the transformers and 
transmission lines causes additional voltage drop at these 
components.
PV-curve 
1. Power systems are operated in the upper part of the PV-curve. This 
part of the PV-curve is statically and dynamically stable. 
 The head of the curve is called the maximum loading point. The 
critical point where the solutions unite is the voltage collapse point. 
The maximum loading point is more interesting from the practical 
point of view than the true voltage collapse point, because the 
maximum of power system loading is achieved at this point. The 
maximum loading point is the voltage collapse point when constant 
power loads are considered, but in general they are different. 
 The voltage dependence of loads affects the point of voltage collapse. 
The power system becomes voltage unstable at the voltage collapse 
point. Voltages decrease rapidly due to the requirement for an infinite 
amount of reactive power.
PV-curve 
 The lower part of the PV-curve (to the left of the voltage collapse point) is 
statically stable, but dynamically unstable. The power system can only 
operate in stable equilibrium so that the system dynamics act to restore 
the state to equilibrium when it is perturbed. 
V1=400 kV and X=100 Ohm
Classification of Voltage stability 
Small-disturbance Voltage Stability- this category 
considers small perturbations such as an incremental 
change in system load. 
 It is the load characteristics and voltage control 
devices that determine the system capability to 
maintain its steady-state bus voltages. 
 This problem is usually studied using power-flow-based 
tools (steady state analysis). 
 In that case the power system can be linearised 
around an operating point and the analysis is typically 
based on eigenvalue and eigenvector techniques
Large-disturbance Voltage Stability 
 Here, the concern is to maintain a steady bus voltages 
following a large disturbance such as system faults, 
switching or loss of load, or loss of generation. 
 This ability is determined by the system and load 
characteristics, and the interactions between the different 
voltage control devices in the system. 
 Large disturbance voltage stability can be studied by using 
non-linear time domain simulations in the short-term time 
frame and load-flow analysis in the long-term time frame 
(steady-state dynamic analysis) 
 The voltage stability is. however, a single problem on which 
a combination of both linear and non-linear tools can be 
used.
Short-term voltage stability 
 Short-term voltage stability is characterized by 
components such as induction motors, excitation of 
synchronous generators, and electronically controlled 
devices such as HVDC and static var compensator. 
The time scale of short-term
Long-term voltage stability 
 The analysis of long-term voltage stability requires 
detailed modeling of long-term dynamics 
 Two types of stability problems emerge in the long-term 
time scale: 
1. Frequency problems may appear after a major 
disturbance resulting in power system islanding. 
Frequency instability is related to the active power 
imbalance between generators and loads. An island 
may be either under or over-generated when the 
system frequency either declines or rises. 
2. Voltage problems
Small Signal Stability 
 Small signal stability refers to the system’s ability to 
maintain steady voltages when subjected to small 
perturbations such as incremental changes in system load. 
 This form of stability is influenced by the characteristics of 
loads, continuous controls, and discrete controls at a given 
instant of time. 
 This concept is useful in determining, at any instant, 
how the system voltages will respond to small system 
changes.
Forms of Instability 
Two forms of Instability 
occur under these 
conditions: 
 Steady Increase in Rotor 
Angle due to lack of 
sufficient Synchronising 
Torque 
 Rotor oscillations of 
increasing amplitude due 
to lack of sufficient 
damping torque
Small-Signal Stability of Multi-machine 
Systems 
 Analysis of practical power systems involves the 
simultaneous solution of equations representing the 
following: 
 Synchronous machines, and the associated excitation 
systems and prime movers. 
 Interconnecting transmission network. 
 Static and dynamic (motor) loads 
 Other devices such as HVDC converters, static var 
compensators
• For system stability studies it is appropriate to 
neglect the transmission network and machine stator 
transients. 
• The dynamics of machine rotor circuits, excitation 
systems, prime mover and other devices are 
represented by differential equations. 
• The result is that the complete system model 
consists of a large number of ordinary differential 
and algebraic equations.
Stability of a Dynamic System 
 The stability of a linear system is entirely independent 
of the input, and the state of the stable system with 
zero input will always will return to the origin of the 
state space, independent of the finite initial state. 
 In contrast stability of the non linear system depends 
on the type and magnitude of input, and the initial 
state.
 In control system theory, it is common to classify 
nonlinear stability into following categories:- 
 Local Stability 
 Finite Stability 
 Global Stability
Local problems 
 Associated with rotor angle oscillations of a single 
generator or a single plant against the rest of the power 
system. Such oscillations are called local plant mode 
oscillations. 
 Most commonly encountered small-signal stability 
problems are of this category. 
 Local problems may also be associated with oscillations 
between the rotors of a few generators close to each 
other.
 Such oscillations are called inter-machine or inter-plant 
mode oscillations. 
 The local plant mode and interplant mode oscillations 
have frequencies in the range of 0.7 to 2.0 Hz. 
 Analysis of local small-signal stability problems requires 
a detailed representation of a small portion of the 
complete interconnected power system.
Finite Stability 
 If state of a system remains within a finite region R, it 
is said to be stable within R. if further, the state of the 
system returns to the equilibrium point from any 
point within R, it is asymptotically stable within finite 
region R.
Global Stability Problems 
 Global small-signal stability problems are caused by 
interactions among large groups of generators and 
have widespread effects. 
 They involve oscillations of a group of generators in 
one area swinging against a group of generators in 
another area. Such oscillations are called inter-area 
mode oscillations.
Eigen value And Stability 
• Stability of the linearized system is described by the 
eigenvalues of the state matrix 
• A real eigen value, or a pair of complex eigenvalues, is 
usually referred to as a mode
• For a complex mode =j, two quantities are of main 
interest: 
 Frequency (in Hz) :f=ω/2π 
 Damping ratio (in %):ξ=100×σ/√(σ^2+ω^2) 
• The system is unstable if  is negative 
• To ensure the acceptable performance, a damping margin 
in the range of 3%-5% is normally required
Model Characteristics 
• While an eigenvalue indicates the stability, its right 
and left eigenvectors give much more information on 
the characteristics of the mode 
• The right eigenvector shows the mode shape, i.e., the 
observability of the mode 
 A mode should be observable from generator 
rotor oscillations if the generator is high in its 
mode shape
• A weighted left eigenvector shows the participation 
factors, i.e., the controllability of the mode 
 A mode should be controllable from generator if the 
generator is high in its participation factors 
• A generator which is high in the mode shape of a 
mode is not necessarily high in the participation 
factor of the same mode
DYNAMIC STABILITY ANALYSIS 
 The analysis of dynamic stability can be performed by 
deriving a linearized state space model of the system 
in the following form 
p X = A X + B u 
 Where the matrices A and B depend on the system 
parameters and the operating conditions. 
 The Eigen values of the system matrix A determine 
the stability of the operating point.
 The Eigen value analysis can be used not only for the 
determination of the stability regions, but also for the 
design of the controllers in the system.
Small Signal Stability of Single M/C 
Infinite Bus System 
 In this section we study the small signal performance of a 
single machine connected to a large system through 
transmission lines. 
 A general system configuration is shown as- 
 Fig. a reduced as fig. b using Thevenin’s Equivalent such 
as virtually there is no change in voltage & frequency of 
Thevenin’s voltage E. 
 Such a voltage source of constt. Voltage & frequency is 
referred as Infinite Bus.
 For any given system condition, the magnitude of the 
infinite bus voltage E remains constt. when the 
machine is perturbed. However as the steady state 
system conditions change, magnitude of E may 
change, representing a changed operating condition of 
external network.
Effects of Excitation System 
 In this section we extend the state space model & block 
diagram to include the excitation system. 
 Fast excitation-systems are usually acknowledged to be 
beneficial to transient stability. 
 These fast excitation changes are not necessarily 
beneficial in damping the oscillations that follow the first 
swing.
 They sometimes contribute growing oscillations several 
seconds after the occurrence of a large disturbance. 
 With proper design and compensation, a fast exciter can 
be an effective means of enhancing stability in the 
dynamic range as well as in the first few cycles after a 
disturbance.
Some General Comments on the 
Effect of Excitation on Stability 
 For less severe transients, the effect of modern fast 
excitation systems on first swing transients is marginal. 
 For more severe transients or for transients initiated by 
faults of longer duration, these modern exciters can have 
a more pronounced effect.
 Their effects on damping torques are small; but in the 
cases where the system exhibits negative damping 
characteristics, the voltage regulator usually 
aggravates the situation by increasing the negative 
damping. 
 Supplementary signals to introduce artificial 
damping torques and to reduce inter machine and 
intersystem oscillations have been used with great 
success.
 Large interconnected power systems experience 
negative damping at very low frequencies of 
oscillations. The parameters of the PSS for a 
particular generator must be adjusted after careful 
study of the power system dynamic performance.
POWER SYSTEM STABILIZERS 
 The dynamic stability of a system can be improved by 
providing suitably tuned power system stabilizers on 
selected generators. to provide damping to critical 
oscillatory modes. 
 Suitably tuned Power System Stabilizers (PSS), will 
introduce a component of electrical torque in phase 
with generator rotor speed deviations resulting in 
damping of low frequency power oscillations in which 
the generators are participating.
 The input to stabilizer signal may be one of the locally 
available signal such as changes in rotor speed, rotor 
frequency, accelerating power or any other suitable 
signal.
CONTROL OF PSS 
A Typical Control Schematic Diagram of 
Power System Stabilizer
APPLICATIONS OF PSS
STRUCTURE OF COMPLETE POWER 
SYSTEM MODEL 
 For system stability it is appropriate to neglect the 
transmission network and machine stator transients. 
 The dynamics of machine rotor ckts., excitation 
systems, prime movers and other devices 
represented by differential equations. 
 Result in that the complete system model consists of 
a large no. of ordinary differential and algebric 
equation.
SPECIAL TECNIQUES FOR ANALYSIS 
OF VERY LARGE SYSTEMS 
 Two methods have been found to be efficient, and, 
they complement each other in meeting the 
requirements of small-signal stability- 
 1. the AESOPS algorithm 
 2. the Modified Arnoldi Method(MAM)
THE AESOPS ALGORITHM 
 The AESOPS algorithm is a type of selective eigen 
value analysis method and it is found very effective in 
computing modes. 
 This allows the efficient studies of local modes without 
the need to reduce the system model
. THE MODIFIED ARNOLDI METHOD
CHARACTERISTICS OF SMALL 
SIGNAL STABILITY PROBLEM 
In large power systems, small signal 
stability problem may be either local or 
global in nature.
LOCAL PROBLEMS 
 Local problems involve a small party of the system. 
 They may be associated with rotor angle oscillations 
of a single generator or a single plant against the rest 
of power system. 
 Such oscillations are called local plant mode 
oscillations. 
 the stability problems related to such oscillations 
are similar to infinite bus system.
 Local problems may also associated with oscillations 
between the rotors of a few generators close to each 
other. 
 Such oscillation are called inter-machine or interplant 
mode oscillations. 
 Other possible local; problems include instability of 
modes associated with controls of equipments such as 
generator excitation system, HVDC converters, and 
static var compensators.
GLOBAL PROBLEMS
is in order of 0.1 to 0.3 Hz. 
Higher frequency modes involving subgroups of 
generators swinging against each other. 
The frequency of these oscillations is typically in the 
range of 0.4 to 0.7 Hz.
References and Bibliography 
 Prabha Kundur , Power System Stability and Control , TMH 
Publication,2008. 
 Kimbark E W, Power System Stability, Volume I, III, Wiley 
publication. 
 C. Radhakrishna : “Stability Studies of AC/DC Power Systems” , 
Ph. D. Thesis , submitted to Indian Institute of Technology 
Kanpur, India, 1980. 
 Presentation on Voltage collapse- M.H.Sadegi 
 Small Signal Stability Analysis Study: 
study prepared by Powertech Labs Inc. for ERCOT 
 www.Google.com
Small signal stability analysis

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Small signal stability analysis

  • 1. PRESENTED BY:- Bhupendra Kumar Integrated M.Tech.
  • 2. Contents  Basic concepts and definitions  Classification of power system stability  Rotor angle stability  Transient stability analysis  Voltage stability  Voltage collapse  Factors affecting voltage stability  Classification of voltage stability  Small signal stability
  • 3.  Stability of dynamic systems  Dynamic stability analysis  Effect of excitation system  Power system stabilizers  Control of PSS  Applications of PSS  AESOPS algorithm  MAM method  Characteristics of small signal stability problem  References and bibliography
  • 4. BASIC CONCEPTS AND DEFINITIONS  Power system stability may be broadly defined as that property of a power system that enables it to remain in a state operating equilibirium under normal operating conditions and to regain an acceptable state of equilibirium after being subjected to a disturbance.  Instability in a power system may be manifested in many different ways depending on the system configuration and operating mode.  Traditionally ,the stability problem has been one of maintaining Synchronus operation.
  • 5. BASIC CONCEPTS AND DEFINITIONS(cont..)  Since power system rely on synchronus machines for electrical power generation, a necessary condition for satisfactory system is that all syn. machines should remain in synchronism.  This aspect of stability is influenced by the dynamics of generators rotor angles and power-angle relationships.  Instability may also encountered without loss of synchronism. For example a system consisting of a synchronus generator feeding an induction motor load through a transmission line can become unstable because of the collapse of load voltage.
  • 6. BASIC CONCEPTS AND DEFINITIONS(cont..)  In the evaluation of stability the concern is the behavior of the power system when subjected to a transient disturbance. The disturbance may be small or large.  Small disturbances in the form of load changes take place continually, and the system adjusts itself to the changing conditions.  The system must be able to operate under these changes and also be capable of surviving numerous disturbances of severe nature, such as short- ckt. on transmission line, loss of a large generator or load , or loss of a tie between two subsystems.
  • 7. Classification Of Power System Stability
  • 8.
  • 9.
  • 10. ROTOR ANGLE STABILITY  Rotor angle stability is the ability of synchronous machines of a power system to remain in synchronism.  In other words, rotor angle or load angle stability denotes the angular displacement between stator and rotor speeds.  It is directly proportional to the speed of the m/c i.e. the load connected to the generator.  If the Angle is beyond to liable limit, the system will come out of synchronism.
  • 11.
  • 12.
  • 13.
  • 14.
  • 15.
  • 16.
  • 17. Transient Stability Analysis  For transient stability analysis we need to consider three systems 1. Prefault - before the fault occurs the system is assumed to be at an equilibrium point 2. Faulted - the fault changes the system equations, moving the system away from its equilibrium point 3. Post fault - after fault is cleared the system hopefully returns to a new operating point
  • 18. VOLTAGE STABILITY & VOLTAGE COLLAPSE  Voltage Stability-It refers to the ability of the system to maintain a steady frequency, following a system drastic change resulting in a significant imbalance between generated and demand power  Voltage stability margins-
  • 19. Factors affecting voltage stability  Voltage stability is a problem in power systems which are heavily loaded, faulted or have a shortage of reactive power.  The nature of voltage stability can be analyzed by examining the production, transmission and consumption of reactive power.  The reactive characteristics of AC transmission lines, transformers and loads restrict the maximum of power system transfers.  The power system lacks the capability to transfer power over long distances or through high reactance due to the requirement of a large amount of reactive power at some critical value of power or distance.
  • 20. Scenario of classic voltage collapse  The large disturbance causes the network characteristics to shrink dramatically. The characteristics of the network and load do not intersect at the instability point. A load increase beyond the voltage collapse point results in loss of equilibrium, and the power system can no longer operate. This will typically lead to cascading outages.  The load voltage decreases, which in turn decreases the load demand and the loading of EHV transmission lines. The voltage control of the system, however, quickly restores generator terminal voltages by increasing excitation. The additional reactive power flow at the transformers and transmission lines causes additional voltage drop at these components.
  • 21. PV-curve 1. Power systems are operated in the upper part of the PV-curve. This part of the PV-curve is statically and dynamically stable.  The head of the curve is called the maximum loading point. The critical point where the solutions unite is the voltage collapse point. The maximum loading point is more interesting from the practical point of view than the true voltage collapse point, because the maximum of power system loading is achieved at this point. The maximum loading point is the voltage collapse point when constant power loads are considered, but in general they are different.  The voltage dependence of loads affects the point of voltage collapse. The power system becomes voltage unstable at the voltage collapse point. Voltages decrease rapidly due to the requirement for an infinite amount of reactive power.
  • 22. PV-curve  The lower part of the PV-curve (to the left of the voltage collapse point) is statically stable, but dynamically unstable. The power system can only operate in stable equilibrium so that the system dynamics act to restore the state to equilibrium when it is perturbed. V1=400 kV and X=100 Ohm
  • 23. Classification of Voltage stability Small-disturbance Voltage Stability- this category considers small perturbations such as an incremental change in system load.  It is the load characteristics and voltage control devices that determine the system capability to maintain its steady-state bus voltages.  This problem is usually studied using power-flow-based tools (steady state analysis).  In that case the power system can be linearised around an operating point and the analysis is typically based on eigenvalue and eigenvector techniques
  • 24. Large-disturbance Voltage Stability  Here, the concern is to maintain a steady bus voltages following a large disturbance such as system faults, switching or loss of load, or loss of generation.  This ability is determined by the system and load characteristics, and the interactions between the different voltage control devices in the system.  Large disturbance voltage stability can be studied by using non-linear time domain simulations in the short-term time frame and load-flow analysis in the long-term time frame (steady-state dynamic analysis)  The voltage stability is. however, a single problem on which a combination of both linear and non-linear tools can be used.
  • 25. Short-term voltage stability  Short-term voltage stability is characterized by components such as induction motors, excitation of synchronous generators, and electronically controlled devices such as HVDC and static var compensator. The time scale of short-term
  • 26. Long-term voltage stability  The analysis of long-term voltage stability requires detailed modeling of long-term dynamics  Two types of stability problems emerge in the long-term time scale: 1. Frequency problems may appear after a major disturbance resulting in power system islanding. Frequency instability is related to the active power imbalance between generators and loads. An island may be either under or over-generated when the system frequency either declines or rises. 2. Voltage problems
  • 27. Small Signal Stability  Small signal stability refers to the system’s ability to maintain steady voltages when subjected to small perturbations such as incremental changes in system load.  This form of stability is influenced by the characteristics of loads, continuous controls, and discrete controls at a given instant of time.  This concept is useful in determining, at any instant, how the system voltages will respond to small system changes.
  • 28. Forms of Instability Two forms of Instability occur under these conditions:  Steady Increase in Rotor Angle due to lack of sufficient Synchronising Torque  Rotor oscillations of increasing amplitude due to lack of sufficient damping torque
  • 29. Small-Signal Stability of Multi-machine Systems  Analysis of practical power systems involves the simultaneous solution of equations representing the following:  Synchronous machines, and the associated excitation systems and prime movers.  Interconnecting transmission network.  Static and dynamic (motor) loads  Other devices such as HVDC converters, static var compensators
  • 30. • For system stability studies it is appropriate to neglect the transmission network and machine stator transients. • The dynamics of machine rotor circuits, excitation systems, prime mover and other devices are represented by differential equations. • The result is that the complete system model consists of a large number of ordinary differential and algebraic equations.
  • 31.
  • 32.
  • 33.
  • 34.
  • 35. Stability of a Dynamic System  The stability of a linear system is entirely independent of the input, and the state of the stable system with zero input will always will return to the origin of the state space, independent of the finite initial state.  In contrast stability of the non linear system depends on the type and magnitude of input, and the initial state.
  • 36.  In control system theory, it is common to classify nonlinear stability into following categories:-  Local Stability  Finite Stability  Global Stability
  • 37. Local problems  Associated with rotor angle oscillations of a single generator or a single plant against the rest of the power system. Such oscillations are called local plant mode oscillations.  Most commonly encountered small-signal stability problems are of this category.  Local problems may also be associated with oscillations between the rotors of a few generators close to each other.
  • 38.  Such oscillations are called inter-machine or inter-plant mode oscillations.  The local plant mode and interplant mode oscillations have frequencies in the range of 0.7 to 2.0 Hz.  Analysis of local small-signal stability problems requires a detailed representation of a small portion of the complete interconnected power system.
  • 39. Finite Stability  If state of a system remains within a finite region R, it is said to be stable within R. if further, the state of the system returns to the equilibrium point from any point within R, it is asymptotically stable within finite region R.
  • 40. Global Stability Problems  Global small-signal stability problems are caused by interactions among large groups of generators and have widespread effects.  They involve oscillations of a group of generators in one area swinging against a group of generators in another area. Such oscillations are called inter-area mode oscillations.
  • 41. Eigen value And Stability • Stability of the linearized system is described by the eigenvalues of the state matrix • A real eigen value, or a pair of complex eigenvalues, is usually referred to as a mode
  • 42. • For a complex mode =j, two quantities are of main interest:  Frequency (in Hz) :f=ω/2π  Damping ratio (in %):ξ=100×σ/√(σ^2+ω^2) • The system is unstable if  is negative • To ensure the acceptable performance, a damping margin in the range of 3%-5% is normally required
  • 43. Model Characteristics • While an eigenvalue indicates the stability, its right and left eigenvectors give much more information on the characteristics of the mode • The right eigenvector shows the mode shape, i.e., the observability of the mode  A mode should be observable from generator rotor oscillations if the generator is high in its mode shape
  • 44. • A weighted left eigenvector shows the participation factors, i.e., the controllability of the mode  A mode should be controllable from generator if the generator is high in its participation factors • A generator which is high in the mode shape of a mode is not necessarily high in the participation factor of the same mode
  • 45. DYNAMIC STABILITY ANALYSIS  The analysis of dynamic stability can be performed by deriving a linearized state space model of the system in the following form p X = A X + B u  Where the matrices A and B depend on the system parameters and the operating conditions.  The Eigen values of the system matrix A determine the stability of the operating point.
  • 46.  The Eigen value analysis can be used not only for the determination of the stability regions, but also for the design of the controllers in the system.
  • 47. Small Signal Stability of Single M/C Infinite Bus System  In this section we study the small signal performance of a single machine connected to a large system through transmission lines.  A general system configuration is shown as-  Fig. a reduced as fig. b using Thevenin’s Equivalent such as virtually there is no change in voltage & frequency of Thevenin’s voltage E.  Such a voltage source of constt. Voltage & frequency is referred as Infinite Bus.
  • 48.  For any given system condition, the magnitude of the infinite bus voltage E remains constt. when the machine is perturbed. However as the steady state system conditions change, magnitude of E may change, representing a changed operating condition of external network.
  • 49.
  • 50. Effects of Excitation System  In this section we extend the state space model & block diagram to include the excitation system.  Fast excitation-systems are usually acknowledged to be beneficial to transient stability.  These fast excitation changes are not necessarily beneficial in damping the oscillations that follow the first swing.
  • 51.  They sometimes contribute growing oscillations several seconds after the occurrence of a large disturbance.  With proper design and compensation, a fast exciter can be an effective means of enhancing stability in the dynamic range as well as in the first few cycles after a disturbance.
  • 52. Some General Comments on the Effect of Excitation on Stability  For less severe transients, the effect of modern fast excitation systems on first swing transients is marginal.  For more severe transients or for transients initiated by faults of longer duration, these modern exciters can have a more pronounced effect.
  • 53.  Their effects on damping torques are small; but in the cases where the system exhibits negative damping characteristics, the voltage regulator usually aggravates the situation by increasing the negative damping.  Supplementary signals to introduce artificial damping torques and to reduce inter machine and intersystem oscillations have been used with great success.
  • 54.  Large interconnected power systems experience negative damping at very low frequencies of oscillations. The parameters of the PSS for a particular generator must be adjusted after careful study of the power system dynamic performance.
  • 55. POWER SYSTEM STABILIZERS  The dynamic stability of a system can be improved by providing suitably tuned power system stabilizers on selected generators. to provide damping to critical oscillatory modes.  Suitably tuned Power System Stabilizers (PSS), will introduce a component of electrical torque in phase with generator rotor speed deviations resulting in damping of low frequency power oscillations in which the generators are participating.
  • 56.  The input to stabilizer signal may be one of the locally available signal such as changes in rotor speed, rotor frequency, accelerating power or any other suitable signal.
  • 57. CONTROL OF PSS A Typical Control Schematic Diagram of Power System Stabilizer
  • 58.
  • 60. STRUCTURE OF COMPLETE POWER SYSTEM MODEL  For system stability it is appropriate to neglect the transmission network and machine stator transients.  The dynamics of machine rotor ckts., excitation systems, prime movers and other devices represented by differential equations.  Result in that the complete system model consists of a large no. of ordinary differential and algebric equation.
  • 61.
  • 62. SPECIAL TECNIQUES FOR ANALYSIS OF VERY LARGE SYSTEMS  Two methods have been found to be efficient, and, they complement each other in meeting the requirements of small-signal stability-  1. the AESOPS algorithm  2. the Modified Arnoldi Method(MAM)
  • 63. THE AESOPS ALGORITHM  The AESOPS algorithm is a type of selective eigen value analysis method and it is found very effective in computing modes.  This allows the efficient studies of local modes without the need to reduce the system model
  • 64. . THE MODIFIED ARNOLDI METHOD
  • 65. CHARACTERISTICS OF SMALL SIGNAL STABILITY PROBLEM In large power systems, small signal stability problem may be either local or global in nature.
  • 66. LOCAL PROBLEMS  Local problems involve a small party of the system.  They may be associated with rotor angle oscillations of a single generator or a single plant against the rest of power system.  Such oscillations are called local plant mode oscillations.  the stability problems related to such oscillations are similar to infinite bus system.
  • 67.  Local problems may also associated with oscillations between the rotors of a few generators close to each other.  Such oscillation are called inter-machine or interplant mode oscillations.  Other possible local; problems include instability of modes associated with controls of equipments such as generator excitation system, HVDC converters, and static var compensators.
  • 69. is in order of 0.1 to 0.3 Hz. Higher frequency modes involving subgroups of generators swinging against each other. The frequency of these oscillations is typically in the range of 0.4 to 0.7 Hz.
  • 70. References and Bibliography  Prabha Kundur , Power System Stability and Control , TMH Publication,2008.  Kimbark E W, Power System Stability, Volume I, III, Wiley publication.  C. Radhakrishna : “Stability Studies of AC/DC Power Systems” , Ph. D. Thesis , submitted to Indian Institute of Technology Kanpur, India, 1980.  Presentation on Voltage collapse- M.H.Sadegi  Small Signal Stability Analysis Study: study prepared by Powertech Labs Inc. for ERCOT  www.Google.com