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Lecture 10
Transformers, Generators, Load, Ybus
Professor Tom Overbye
Department of Electrical and
Computer Engineering
ECE 476
POWER SYSTEM ANALYSIS
1
Announcements
 Be reading Chapter 6.
 HW 3 is due now.
 HW 4 is 3.4, 3.10, 3.14, 3.19, 3.23, 3.60; due September 29
in class.
 First exam is October 11 during class. Closed book, closed
notes, one note sheet and calculators allowed
2
Load Tap Changing Transformers
 LTC transformers have tap ratios that can be varied
to regulate bus voltages
 The typical range of variation is 10% from the
nominal values, usually in 33 discrete steps
(0.0625% per step).
 Because tap changing is a mechanical process, LTC
transformers usually have a 30 second deadband to
avoid repeated changes.
 Unbalanced tap positions can cause "circulating
vars"
3
LTCs and Circulating Vars
slack
1 1.00 pu
2 3
40.2 MW
40.0 MW
1.7 Mvar
-0.0 Mvar
1.000 tap 1.056 tap
24.1 MW
12.8 Mvar
24.0 MW
-12.0 Mvar
A
MVA
1.05 pu
0.98 pu
24 MW
12 Mvar
64 MW
14 Mvar
40 MW
0 Mvar
0.0 Mvar
80%
A
MVA
4
Phase Shifting Transformers
 Phase shifting transformers are used to control the
phase angle across the transformer
 Since power flow through the transformer depends
upon phase angle, this allows the transformer to
regulate the power flow through the transformer
 Phase shifters can be used to prevent inadvertent
"loop flow" and to prevent line overloads.
5
Phase Shifter Example 3.13
slack
Phase Shifting Transformer
345.00 kV 341.87 kV
0.0 deg
216.3 MW 216.3 MW
283.9 MW 283.9 MW
1.05000 tap
39.0 Mvar 6.2 Mvar
93.8 Mvar
125.0 Mvar
500 MW
164 Mvar 500 MW
100 Mvar
6
ComED Control Center
7
ComED Phase Shifter Display
8
Phase Shifting Transformer Picture
230 kV 800 MVA Phase Shifting
Transformer During factory testing
Source: Tom Ernst, Minnesota Power
Costs about $7 million,
weighs about 1.2
million pounds
9
Autotransformers
 Autotransformers are transformers in which the
primary and secondary windings are coupled
magnetically and electrically.
 This results in lower cost, and smaller size and
weight.
 The key disadvantage is loss of electrical isolation
between the voltage levels. Hence auto-
transformers are not used when a is large. For
example in stepping down 7160/240 V we do not
ever want 7160 on the low side!
10
Could it Happen Tomorrow?
 Geomagnetic disturbances (GMDs) impact the
power grid by causing geomagenetic induced dc
currents (GICs) that can push the transformers into
saturation.
 Saturated
transformers
have high
harmonics which
leads to high
reactive losses and
heating
Image from Ed Schweitzer June 2011 JASON Presentation
11
Could It Happen Tomorrow?
• A 1989 storm caused a major blackout in Quebec.
Much larger storms have occurred in the past, such
as in 1859, which knocked out much of the
telegraph system in the Eastern US
• A 2010 Metatech Report
indicated an 1859 type
event could destroy
hundreds of EHV
transformers, crippling
our grid for months!
Metatech R-319, Figure 4.11
12
Load Models
 Ultimate goal is to supply loads with electricity at
constant frequency and voltage
 Electrical characteristics of individual loads matter,
but usually they can only be estimated
– actual loads are constantly changing, consisting of a large
number of individual devices
– only limited network observability of load characteristics
 Aggregate models are typically used for analysis
 Two common models
– constant power: Si = Pi + jQi
– constant impedance: Si = |V|2 / Zi
13
Generator Models
 Engineering models depend upon application
 Generators are usually synchronous machines
 For generators we will use two different models:
– a steady-state model, treating the generator as a constant
power source operating at a fixed voltage; this model
will be used for power flow and economic analysis
– a short term model treating the generator as a constant
voltage source behind a possibly time-varying reactance
14
Power Flow Analysis
 We now have the necessary models to start to
develop the power system analysis tools
 The most common power system analysis tool is the
power flow (also known sometimes as the load flow)
– power flow determines how the power flows in a network
– also used to determine all bus voltages and all currents
– because of constant power models, power flow is a
nonlinear analysis technique
– power flow is a steady-state analysis tool
15
Linear versus Nonlinear Systems
A function H is linear if
H(a1m1 + a2m2) = a1H(m1) + a2H(m2)
That is
1) the output is proportional to the input
2) the principle of superposition holds
Linear Example: y = H(x) = c x
y = c(x1+x2) = cx1 + c x2
Nonlinear Example: y = H(x) = c x2
y = c(x1+x2)2 ≠ (cx1)2 + (c x2)2
16
Linear Power System Elements
Resistors, inductors, capacitors, independent
voltage sources and current sources are linear
circuit elements
1
V = R I V = V =
Such systems may be analyzed by superposition
j L I I
j C


17
Nonlinear Power System Elements
Constant power loads and generator injections are
nonlinear and hence systems with these elements can
not be analyzed by superposition
Nonlinear problems can be very difficult to solve,
and usually require an iterative approach
18
Nonlinear Systems May Have
Multiple Solutions or No Solution
Example 1: x2 - 2 = 0 has solutions x = 1.414…
Example 2: x2 + 2 = 0 has no real solution
f(x) = x2 - 2 f(x) = x2 + 2
two solutions where f(x) = 0 no solution f(x) = 0
19
Multiple Solution Example 3
The dc system shown below has two solutions:
where the 18 watt
load is a resistive
load
2
2
Load
Load
Load
The equation we're solving is
9 volts
I 18 watts
1 +R
One solution is R 2
Other solution is R 0.5
Load Load
R R
 
 
 

 
 
 
What is the
maximum
PLoad?

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ECE4762011_Lect10.ppt

  • 1. Lecture 10 Transformers, Generators, Load, Ybus Professor Tom Overbye Department of Electrical and Computer Engineering ECE 476 POWER SYSTEM ANALYSIS
  • 2. 1 Announcements  Be reading Chapter 6.  HW 3 is due now.  HW 4 is 3.4, 3.10, 3.14, 3.19, 3.23, 3.60; due September 29 in class.  First exam is October 11 during class. Closed book, closed notes, one note sheet and calculators allowed
  • 3. 2 Load Tap Changing Transformers  LTC transformers have tap ratios that can be varied to regulate bus voltages  The typical range of variation is 10% from the nominal values, usually in 33 discrete steps (0.0625% per step).  Because tap changing is a mechanical process, LTC transformers usually have a 30 second deadband to avoid repeated changes.  Unbalanced tap positions can cause "circulating vars"
  • 4. 3 LTCs and Circulating Vars slack 1 1.00 pu 2 3 40.2 MW 40.0 MW 1.7 Mvar -0.0 Mvar 1.000 tap 1.056 tap 24.1 MW 12.8 Mvar 24.0 MW -12.0 Mvar A MVA 1.05 pu 0.98 pu 24 MW 12 Mvar 64 MW 14 Mvar 40 MW 0 Mvar 0.0 Mvar 80% A MVA
  • 5. 4 Phase Shifting Transformers  Phase shifting transformers are used to control the phase angle across the transformer  Since power flow through the transformer depends upon phase angle, this allows the transformer to regulate the power flow through the transformer  Phase shifters can be used to prevent inadvertent "loop flow" and to prevent line overloads.
  • 6. 5 Phase Shifter Example 3.13 slack Phase Shifting Transformer 345.00 kV 341.87 kV 0.0 deg 216.3 MW 216.3 MW 283.9 MW 283.9 MW 1.05000 tap 39.0 Mvar 6.2 Mvar 93.8 Mvar 125.0 Mvar 500 MW 164 Mvar 500 MW 100 Mvar
  • 9. 8 Phase Shifting Transformer Picture 230 kV 800 MVA Phase Shifting Transformer During factory testing Source: Tom Ernst, Minnesota Power Costs about $7 million, weighs about 1.2 million pounds
  • 10. 9 Autotransformers  Autotransformers are transformers in which the primary and secondary windings are coupled magnetically and electrically.  This results in lower cost, and smaller size and weight.  The key disadvantage is loss of electrical isolation between the voltage levels. Hence auto- transformers are not used when a is large. For example in stepping down 7160/240 V we do not ever want 7160 on the low side!
  • 11. 10 Could it Happen Tomorrow?  Geomagnetic disturbances (GMDs) impact the power grid by causing geomagenetic induced dc currents (GICs) that can push the transformers into saturation.  Saturated transformers have high harmonics which leads to high reactive losses and heating Image from Ed Schweitzer June 2011 JASON Presentation
  • 12. 11 Could It Happen Tomorrow? • A 1989 storm caused a major blackout in Quebec. Much larger storms have occurred in the past, such as in 1859, which knocked out much of the telegraph system in the Eastern US • A 2010 Metatech Report indicated an 1859 type event could destroy hundreds of EHV transformers, crippling our grid for months! Metatech R-319, Figure 4.11
  • 13. 12 Load Models  Ultimate goal is to supply loads with electricity at constant frequency and voltage  Electrical characteristics of individual loads matter, but usually they can only be estimated – actual loads are constantly changing, consisting of a large number of individual devices – only limited network observability of load characteristics  Aggregate models are typically used for analysis  Two common models – constant power: Si = Pi + jQi – constant impedance: Si = |V|2 / Zi
  • 14. 13 Generator Models  Engineering models depend upon application  Generators are usually synchronous machines  For generators we will use two different models: – a steady-state model, treating the generator as a constant power source operating at a fixed voltage; this model will be used for power flow and economic analysis – a short term model treating the generator as a constant voltage source behind a possibly time-varying reactance
  • 15. 14 Power Flow Analysis  We now have the necessary models to start to develop the power system analysis tools  The most common power system analysis tool is the power flow (also known sometimes as the load flow) – power flow determines how the power flows in a network – also used to determine all bus voltages and all currents – because of constant power models, power flow is a nonlinear analysis technique – power flow is a steady-state analysis tool
  • 16. 15 Linear versus Nonlinear Systems A function H is linear if H(a1m1 + a2m2) = a1H(m1) + a2H(m2) That is 1) the output is proportional to the input 2) the principle of superposition holds Linear Example: y = H(x) = c x y = c(x1+x2) = cx1 + c x2 Nonlinear Example: y = H(x) = c x2 y = c(x1+x2)2 ≠ (cx1)2 + (c x2)2
  • 17. 16 Linear Power System Elements Resistors, inductors, capacitors, independent voltage sources and current sources are linear circuit elements 1 V = R I V = V = Such systems may be analyzed by superposition j L I I j C  
  • 18. 17 Nonlinear Power System Elements Constant power loads and generator injections are nonlinear and hence systems with these elements can not be analyzed by superposition Nonlinear problems can be very difficult to solve, and usually require an iterative approach
  • 19. 18 Nonlinear Systems May Have Multiple Solutions or No Solution Example 1: x2 - 2 = 0 has solutions x = 1.414… Example 2: x2 + 2 = 0 has no real solution f(x) = x2 - 2 f(x) = x2 + 2 two solutions where f(x) = 0 no solution f(x) = 0
  • 20. 19 Multiple Solution Example 3 The dc system shown below has two solutions: where the 18 watt load is a resistive load 2 2 Load Load Load The equation we're solving is 9 volts I 18 watts 1 +R One solution is R 2 Other solution is R 0.5 Load Load R R              What is the maximum PLoad?