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Balance Fault Analysis, Symmetrical Components

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ECE 476 POWER SYSTEM ANALYSIS Lecture 19 Balance Fault Analysis, Symmetrical Components Professor Tom Overbye Department of Electrical and Computer Engineering – PowerPoint PPT presentation

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Title: Balance Fault Analysis, Symmetrical Components


1
ECE 476POWER SYSTEM ANALYSIS
  • Lecture 19
  • Balance Fault Analysis, Symmetrical Components
  • Professor Tom Overbye
  • Department of Electrical andComputer Engineering

2
Announcements
  • Be reading Chapter 8
  • HW 8 is 7.6, 7.13, 7.19, 7.28 due Nov 3 in
    class.
  • Start working on Design Project. Tentatively due
    Nov 17 in class.

3
In the News
  • Earlier this week the Illinois House and Senate
    overrode the Governors veto of the Smart Grid
    Bill it is now law
  • On Tuesday Quinn called it a smart greed plan
  • Law authorizes a ten year, 3 billion project to
    modernization the electric grid in Illinois
  • All ComEd customers and most of Ameren will get
    smart meters
  • Effort will be paid for through rate increases
    over the period ComEd estimated the average
    increase of 36 per year would be offset by
    electricity savings

4
Network Fault Analysis Simplifications
  • To simplify analysis of fault currents in
    networks we'll make several simplifications
  • Transmission lines are represented by their
    series reactance
  • Transformers are represented by their leakage
    reactances
  • Synchronous machines are modeled as a constant
    voltage behind direct-axis subtransient reactance
  • Induction motors are ignored or treated as
    synchronous machines
  • Other (nonspinning) loads are ignored

5
Network Fault Example
For the following network assume a fault on the
terminal of the generator all data is per
unit except for the transmission line reactance
generator has 1.05 terminal voltage supplies
100 MVA with 0.95 lag pf
6
Network Fault Example, cont'd
Faulted network per unit diagram
7
Network Fault Example, cont'd
8
Fault Analysis Solution Techniques
  • Circuit models used during the fault allow the
    network to be represented as a linear circuit
  • There are two main methods for solving for fault
    currents
  • Direct method Use prefault conditions to solve
    for the internal machine voltages then apply
    fault and solve directly
  • Superposition Fault is represented by two
    opposing voltage sources solve system by
    superposition
  • first voltage just represents the prefault
    operating point
  • second system only has a single voltage source

9
Superposition Approach
Faulted Condition
Exact Equivalent to Faulted Condition
Fault is represented by two equal and opposite
voltage sources, each with a magnitude equal to
the pre-fault voltage
10
Superposition Approach, contd
Since this is now a linear network, the faulted
voltages and currents are just the sum of the
pre-fault conditions the (1) component and the
conditions with just a single voltage source at
the fault location the (2) component
Pre-fault (1) component equal to the pre-fault
power flow solution
Obvious the pre-fault fault current is zero!
11
Superposition Approach, contd
Fault (1) component due to a single voltage
source at the fault location, with a magnitude
equal to the negative of the pre-fault voltage at
the fault location.
12
Two Bus Superposition Solution
This matches what we calculated earlier
13
Extension to Larger Systems
However to use this approach we need to first
determine If
14
Determination of Fault Current
15
Determination of Fault Current
16
Three Gen System Fault Example
17
Three Gen Example, contd
18
Three Gen Example, contd
19
Three Gen Example, contd
20
PowerWorld Example 7.5 Bus 2 Fault
21
Problem 7.28
22
Grounding
  • When studying unbalanced system operation how a
    system is grounded can have a major impact on the
    fault flows
  • Ground current does not come into play during
    balanced system analysis (since net current to
    ground would be zero).
  • Becomes important in the study of unbalanced
    systems, such as during most faults.

23
Grounding, contd
  • Voltages are always defined as a voltage
    difference. The ground is used to establish the
    zero voltage reference point
  • ground need not be the actual ground (e.g., an
    airplane)
  • During balanced system operation we can ignore
    the ground since there is no neutral current
  • There are two primary reasons for grounding
    electrical systems
  • safety
  • protect equipment

24
How good a conductor is dirt?
  • There is nothing magical about an earth ground.
    All the electrical laws, such as Ohms law, still
    apply.
  • Therefore to determine the resistance of the
    ground we can treat it like any other resistive
    material

25
How good a conductor is dirt?
26
How good a conductor is dirt?
27
Calculation of grounding resistance
  • Because of its large cross sectional area the
    earth is actually a pretty good conductor.
  • Devices are physically grounded by having a
    conductor in physical contact with the ground
    having a fairly large area of contact is
    important.
  • Most of the resistance associated with
    establishing an earth ground comes within a short
    distance of the grounding point.
  • Typical substation grounding resistance is
    between 0.1 and 1 ohm fence is also grounded,
    usually by connecting it to the substation ground
    grid.

28
Calculation of grounding R, contd
  • Example Calculate the resistance from a
    grounding rod out to a radial distance x from the
    rod, assuming the rod has a radius of r

29
Calculation of grounding R, contd
The actual values will be substantially less
since weve assumed no current flowing downward
into the ground
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