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EPRINSF Workshop presentation 402 Cancun

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Title: EPRINSF Workshop presentation 402 Cancun


1
Instability Monitoring and Control of Power
Systems
Workshop on Open Issues in Analysis and Control
of Power and Energy Processing SystemsIEEE CDC,
December 8, 2003, Maui, HI
Eyad H. Abed Electrical and Computer
Engineering and the Institute for Systems
Research University of Maryland, College Park
20742 abed_at_umd.edu
2
Concepts of Instability Monitoring
  • Detection of (incipient) instability by observing
    a departure from synchronous operation. Use of
    global phasor measurements of system trajectory
    and detection of nature of the trajectory (e.g.,
    concave or convex).
  • Determination of measures of proximity to the
    border of the stability boundary in parameter
    space. (Model based.)
  • Determination of conditions for hitting the
    stability boundary in parameter space. (Model
    based.)
  • Probe signal or inherent noise-based detection of
    impending instability.

3
Problems with Model-Based Instability Monitoring
  • As noted by Hauer (APEx 2000) recurring
    problem of system oscillations and voltage
    collapse is due in part to system behavior not
    well captured by the models used in planning and
    operation studies
  • In the face of component failures, system models
    quickly become mismatched to the physical
    network, and are only accurate if theyre updated
    using a powerful and accurate failure detection
    system.

4
Other Work Related to Probe and Ambient
Noise-Based Instability Monitoring
  • In several papers, Hauer has discussed large
    system experiments using probe signal injection
    and ambient noise effects for stability and
    oscillation studies. This includes HVDC
    modulation at mid-level (125MW) for probing of
    inividual oscillation modes, and low-level
    (20MW) for broadband probing.
  • Earthquake prediction research contains work on
    studying the nature of pre-quake motions.
  • Kevrekidis et al. (recent Phys. Rev. Lett. etc.)
    and Sontag et al. (SCL) are looking for schemes
    for automatically finding bifurcation points in
    uncertain systems.

5
Probe-Based Instability Monitoring Not Entirely
New, However
  • Theres no deep theory at present.
  • Only linearization-based statements are
    available.
  • More comments later on needed work in this area.

6
Noisy Precursors
  • Noisy precursors were studied by Kurt
    Wiesenfeld (1985, J. Stat. Phys.) in the context
    of noise amplification near criticality
    (stability boundary). Wiesenfeld found different
    noisy precursors for different bifurcations,
    assuming a small white noise disturbance.
  • It is important to note that noisy precursors
    also give a nonparametric indicator of impending
    instability.
  • Noisy precursors are observed as rising peaks in
    the power spectral density of a measured output
    signal of a system with a persistent noise
    disturbance --- the rising peak is seen as one or
    more eigenvalues approach the imaginary axis.

7
(a)
(b)
Power spectrum magnitude for Hopf bifurcation
when ?010 for two values of ? (a) ?10, (b)
?0.1 Kim Abed 2000.
8
(a)
(b)
Power spectrum magnitude for stationary
bifurcation for two values of ? (a) ?10, (b)
?0.1 Kim Abed 2000.
9
Application to a Power System Model
Consider a synchronous machine connected to an
infinite bus together with excitation control
Abed Varaiya, 1984. It was shown that this
system undergoes a subcritical Hopf bifurcation
as the control gain in the excitation system is
increased beyond a critical value. The
dynamics of the generator is given by
The dynamics of the generator is given by
10
Output spectrum with noise probe signal, as
instability is approached. (Critical KA 193.7.)
11
Non-noise-based precursors
  • Resonant and nearly resonant (periodic)
    perturbations They can be shown to either delay
    or advance bifurcations (instabilities)
  • Supercritical bifurcations delayed
  • Subcritical bifurcations advanced
  • Chaotic signals containing a resonant frequency
    have a similar effect.
  • White noise can have such an effect, but it is
    less pronounced.

12
Chaotic probe signal
13
(No Transcript)
14
Closed-loop precursor-based monitoring systems
Illustration for closeness to zero eigenvalue
15
Combined model- and signal-based on-line
monitoring
  • The effect of harmonic probe signals to advance a
    subcritical (severe) bifurcations (instability)
    can be very useful in early detection of an
    impending instability.
  • However, this would also introduce the system
    instability into the power system before it would
    otherwise occur (defeating the purpose).
  • To circumvent this problem, the probe can be
    applied to a model that is updated as system
    loading and topology change, and detected
    impending instabilities in the model can be used
    as an alarm to trigger preventive control actions.

16
Model-based instability monitor with periodic
probe signal
17
Example in a Simple Power System Model
Consider the simplified power system model
Venkatasubramanian et al. 1992 with generator,
voltage control, transmission line and matched
load
18
Bifurcation boundaries in parameter space
(subcritical Hopf followed by saddle-node)
LExcitation gain and PLoad
19
Advance of Hopf bifurcation as a function of
probe amplitude two-thirds power law
exhibited (Hassouneh et al., 2002)
20
Severity of Instability/Bifurcation
  • At least two types of severity issues
  • Severity of the nonlinear instability (nature of
    the bifurcation). This depends strongly on system
    nonlinearities.
  • Spatial impact of the instability, which can be
    checked by linear analysis using participation
    factors and needed generalizations.

21
Determining Severity of Instability in Advance
  • Participation factors tell us which physical
    states participate most in a mode (such as an
    unstable mode).
  • Can severity of a bifurcation be linked to
    criteria in terms of participation factors (as
    well as nonlinear calculations)?
  • Is it true that if fewer states are tightly tied
    to a mode then the chance of pervasive
    instability is reduced?
  • Can we use these concepts to build vibration
    absorbers for power networks?

22
Simple Message of this Talk
  • We cant rely totally on models in power system
    instability monitoring the models become less
    reliable as the system is stressed more and more.
  • Signal-based tools need to be developed for
    detecting instability problems before they start.
  • A lot of deep theory needs to be developed to
    make this happen, including ideas for time-space
    propagation of instability.
  • Finding synergies with other areas is needed ---
    self-organized criticality, earthquake
    prediction, lasers, etc.

23
A Related SubjectRevisiting Modal Participation
Factors
  • Participation factors give measures of
    interaction between modes and states
  • These can be useful in placement of controllers
    and sensors
  • A better fundamental understanding of
    participation factors will contribute to health
    monitoring of heavily loaded power systems

24
Participation Factors
  • (Modal) Participation factors are an important
    element of Selective Modal Analysis (SMA)
    (Verghese, Perez-Arriaga and Schweppe, 1982). See
    also books by Sauer and Pai, Kundur, etc.
  • SMA is a very popular tool for system analysis,
    order reduction and actuator placement in the
    electric power systems area. Related concepts
    occur in other engineering disciplines.
  • We have revisited the concept of participation
    factors, and considered why it is useful in
    sensor/actuator placement.

25
Basic Definition
  • Consider a linear time-invariant system
  • dx/dt Ax(t),
  • where x2 Rn, and A is n n with n distinct
    eigenvalues (l1,l2,,ln).
  • It is often desirable to quantify and compare the
    participation of a particular mode (i.e.,
    eigenmode) in state variables. If the states are
    physical variables, this lets us study the
    influence of system modes on physical components.

26
  • Tempting to base the association of modes with
    state variables on the magnitudes of the entries
    in the right eigenvector associated with a mode.
  • Let (r1,r2,,rn) be right eigenvectors of the
    matrix A associated with the eigenvalues
    (l1,l2,,ln), respectively.
  • Using this criterion, one would say that
  • the mode associated with li is significantly
    involved in the state xk if rik is large.

27
  • Two main disadvantages of this approach
  • (i) It requires a complete spectral analysis of
    the system, and is thus computationally
    expensive
  • (ii) The numerical values of the entries of the
    eigenvectors depend on the choice of units for
    the corresponding state variables.
  • Problem (ii) is the more serious flaw. It renders
    the criterion unreliable in providing a measure
    of the contribution of modes to state variables.
    This is true even if the variables are similar
    physically and are measured in the same units.

28
  • In SMA, the entries of both the right and left
    eigenvectors are utilized to calculate
    participation factors that measure the level of
    participation of modes in states and the level of
    participation of states in modes.
  • The participation factors defined in SMA are
    dimensionless quantities that are independent of
    the units in which state variables are measured.
  • Let (l1,l2,,ln) be left (row) eigenvectors of
    the matrix A associated with the eigenvalues
    (l1,l2,,ln), respectively.

29
  • The right and left eigenvectors are taken to
    satisfy the normalization li rj dij (Kronecker
    delta).
  • Verghese, Perez-Arriaga and Schweppe define the
    participation factor of the i-th mode in the k-th
    state xk as the complex number
  • pki lik rik

30
New Approach and New Definitions
  • Reference Abed, Lindsay and Hashlamoun
    (Automatica 2000).
  • The linear system
  • usually represents the small perturbation
    dynamics of a nonlinear system near an
    equilibrium.
  • The initial condition for such a perturbation is
    usually viewed as being an uncertain vector of
    small norm.
  • We have re-defined participation factors using
    deterministic and probabilistic uncertainty
    models.

31
New Approach and New Definitions, Contd.
  • These new definitions involve computing the
    relative participation of a mode in a state
    averaged over the initial condition uncertainty.
  • The averaging can be over a set (set-theoretic
    setting) or with respect to a probability density
    of the initial condition (probabilistic setting).
  • When the uncertainty is symmetric with respect to
    the origin, the new definitions yield the
    original definition as a special case.

32
New Approach and New Definitions, Contd.
  • The new definitions and the old definitions focus
    on behavior around an equilibrium.
  • It would be desirable to extend these concepts to
    the case of transient behavior initiated away
    from equilibrium, such as occurs when in a
    faulted system trajectory.
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