MIDTERM EXAM 1 SPRING 2014 ECE 422/522 NAME:

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MIDTERM EXAM 1 SPRING 2014
ECE 422/522
NAME:
BE SURE TO SHOW YOUR WORK CLEARLY AND FULLY. SHOWING YOUR THINKIING HELPS
YOU GET MORE POINTS.
All questions are required for both ECE422 and ECE522 students. ECE422 students will receive 10% more
points.
1 and 2 should be finished in class. 3 and 4 are take-home questions due by 12AM midnight today.
1. Load modeling (25 points): Under a steady-state operating condition, a bus has real power load P0=100MW,
reactive power load Q0=50MVAr, voltage magnitude V0=220kV and frequency f0=60Hz. If its real and reactive
power loads, P and Q, under this condition can both be modeled as frequency-dependent ZI (constant
Μ… 0.8, 𝑄̅ /𝑉̅ = 2.7 and 𝑄̅ /𝑓=
Μ… ο€­2.3, where 𝑃̅=P/P0,
impedance and current) loads with 𝑃̅ /𝑉̅ = 1.3, 𝑃̅/𝑓=
Μ… 0.
𝑄̅ =Q/Q0, 𝑉̅ =V/V0 and 𝑓=f/f
a. Represent P and Q as functions of V and f and calculate all coefficients.
b. When f=59.7Hz, draw the characteristics of functions P(V) and Q(V)
a
Μ… = (π‘·πŸ 𝑽
Μ… 𝟐 + π‘·πŸ 𝑽
Μ… )[𝟏 + (𝒇̅ − 𝟏)𝑲𝒑𝒇 ]
𝑷
Μ… = (π‘ΈπŸ 𝑽
Μ… 𝟐 + π‘ΈπŸ 𝑽
Μ… )[𝟏 + (𝒇̅ − 𝟏)𝑲𝒒𝒇 ]
𝑸
8’
𝑽 = π‘½πŸŽ , 𝒇 = π’‡πŸŽ
Μ…
𝝏𝑷
= 𝑲𝒑𝒇 = 𝟎. πŸ–
𝝏𝒇̅
Μ…
𝝏𝑸
= 𝑲𝒒𝒇 = −𝟐. πŸ‘
𝝏𝒇̅
Μ… 𝟎 = π‘·πŸ + π‘·πŸ = 𝟏
𝑷
Μ… 𝟎 = π‘ΈπŸ + π‘ΈπŸ = 𝟏
𝑸
Μ…
𝝏𝑷
= πŸπ‘·πŸ + π‘·πŸ = 𝟏. πŸ‘
Μ…
𝝏𝑽
Μ…
𝝏𝑸
= πŸπ‘ΈπŸ + π‘ΈπŸ = 𝟐. πŸ•
{ 𝝏𝑽
Μ…
π‘·πŸ = 𝟎. πŸ‘
𝑷 = 𝟎. πŸ•
{ 𝟐
π‘ΈπŸ = 𝟏. πŸ•
π‘ΈπŸ = −𝟎. πŸ•
4’
𝑷 = 𝟏𝟎𝟎[𝟎. πŸ‘(
𝑸 = πŸ“πŸŽ[𝟏. πŸ•(
𝑽 𝟐
𝑽
𝒇 − πŸ”πŸŽ
) + 𝟎. πŸ•
](𝟏 +
𝟎. πŸ–)
𝟐𝟐𝟎
𝟐𝟐𝟎
πŸ”πŸŽ
𝑽 𝟐
𝑽
𝒇 − πŸ”πŸŽ
) − 𝟎. πŸ•
](𝟏 +
(−𝟐. πŸ‘))
𝟐𝟐𝟎
𝟐𝟐𝟎
πŸ”πŸŽ
4’
b
f=59.7
𝑷 = πŸ—πŸ—. πŸ”(𝟎. πŸ‘(
𝑽 𝟐
𝑽
) + 𝟎. πŸ•
)
𝟐𝟐𝟎
𝟐𝟐𝟎
𝑸 = πŸ“πŸŽ. πŸ“πŸ•(𝟏. πŸ•(
𝑽 𝟐
𝑽
) − 𝟎. πŸ•
)
𝟐𝟐𝟎
𝟐𝟐𝟎
4’
5’
(Using the exponential model receives up to 10’)
2. True or false? If it is false, explain why briefly (25 points).
a. In NERC’s reliability standards, power system events resulting in the loss of a single element are
referred to the Category A contingencies and events resulting in the loss of two elements belong to the
Category B contingencies.
False. Loss of a single element are referred to the Category B. Loss of two elements belong to the
Category C
(Background - Slides #24~25)
b. Under a steady-state operating condition, all the operating quantities that characterize the condition are
constant.
False. Actually, not constant but treated as constant only for purpose of analysis. (Background – Slide
#29)
c. A bulk power system that has adequate energy resources to support the electrical demands of its
customers does not have reliability problems.
False. Reliability includes adequacy and security. A system without adequacy issue could still have
security issue. (Background – Slide #23)
d. Power system stability is essentially a single problem; Because of high dimensionality and complexity
of stability problems, it helps to make simplifying assumptions to analyze specific types of problems
using an appropriate degree of detail of system representation and appropriate analytical techniques.
Ture. (Background – slide #37)
e. A dynamic load model enables modeling dynamic characteristics of a load with changes of the bus
voltage magnitude and/or frequency at any instant of time. It can be described by algebraic functions of
the bus voltage magnitude and frequency at that instant.
False. Described by differential equations. (Load modeling – slide #10)
NAME:
3. Equivalent Circuits (35 points): Consider the following equivalent circuits for a 483 MVA (3-phase), 24kV
(line-to-line RMS), 0.9 power factor, 60Hz, 3 phase, 2 pole synchronous generator, which has the following
inductance and resistance parameters in per unit values in the Lad–Laq base per unit system and open-circuit time
constants in seconds:
Ld=1.800
Lq=1.720
Ll=0.17
Ra=0.0027
L’d=0.285
L’q=0.490
L”d=0.220
L”q=0.220
T’d0=3.7 s
T’q0=0.48 s T”d0=0.032 s T”q0=0.06 s
The transient and subtransient parameters are based on the classical definitions and unsaturated values of Lad
and Laq.
a. Determine per unit values of fundamental parameters, i.e. all inductances and resistances in the d- and qaxis equivalent circuits
b. Explain why inequalities Ld>L’d>L”d and T’d0 >> T”d0 hold
c. If ifd base (iFbase)=1875A. Determine the following parameters in mH or .
Ll, Ld, Lq, Lad, Laq, MF (i.e. Lafd in Kundur’s book), LF (i.e. Lffd in Kundur’s book), Lfd, Rfd and
Ra
d. Determine transfer function Ld(s)
a (Kundur’s Example 4.1 in Page 153)
𝑳𝒂𝒅 = 𝑳𝒅 − 𝑳𝒍 = 𝟏. πŸ– − 𝟎. πŸπŸ• = 𝟏. πŸ”πŸ‘
𝑳′𝒅 = 𝑳𝒍 +
𝟏
𝟏
𝟏
𝑳𝒂𝒅 + 𝑳𝒇𝒅
= 𝟎. πŸπŸ• +
𝟏
𝟏
𝟏
𝟏. πŸ”πŸ‘ + 𝑳𝒇𝒅
= 𝟎. πŸπŸ–πŸ“
𝑳𝒇𝒅 = 𝟎. πŸπŸπŸ‘πŸ•
𝑳′′𝒅 = 𝑳𝒍 +
𝟏
𝟏
= 𝟎. πŸπŸ• +
= 𝟎. 𝟐𝟐𝟎
𝟏
𝟏
𝟏
𝟏
𝟏
𝟏
𝑳𝒂𝒅 + 𝑳𝒇𝒅 + π‘³πŸπ’…
𝟏. πŸ”πŸ‘ + 𝟎. πŸπŸπŸ‘πŸ• + π‘³πŸπ’…
π‘³πŸπ’… = 𝟎. πŸŽπŸ–πŸ–πŸ“
𝑹𝒇𝒅 =
π‘ΉπŸπ’…
𝑳𝒂𝒅 + 𝑳𝒇𝒅 𝟏. πŸ”πŸ‘ + 𝟎. πŸπŸπŸ‘πŸ•
=
= 𝟎. πŸŽπŸŽπŸπŸπŸ”
𝑻′π’…πŸŽ⁄
πŸ‘. πŸ• ∗ πŸ‘πŸ•πŸ•
𝒕𝒃𝒂𝒔𝒆
𝟏
+ 𝟏⁄𝑳
𝟏
+ π‘³πŸπ’…
+ 𝟎. πŸŽπŸ–πŸ–πŸ“
𝟏⁄
𝟏
𝟏⁄
⁄
+
𝑳𝒂𝒅
𝒇𝒅
𝟎. πŸπŸπŸ‘πŸ•
=
= 𝟏. πŸ”πŸ‘
= 𝟎. πŸŽπŸπŸ”πŸ—
𝑻′′π’…πŸŽ⁄
𝟎. πŸŽπŸ‘πŸ ∗ πŸ‘πŸ•πŸ•
𝒕𝒃𝒂𝒔𝒆
𝑳𝒂𝒒 = 𝑳𝒒 − 𝑳𝒍 = 𝟏. πŸ•πŸπŸŽ − 𝟎. πŸπŸ• = 𝟏. πŸ“πŸ“
𝑳′𝒒 = 𝑳𝒍 +
𝟏
𝟏
𝟏
𝑳𝒂𝒒 + π‘³πŸπ’’
= 𝟎. πŸπŸ• +
𝟏
𝟏
𝟏
+
𝟏. πŸ“πŸ“ π‘³πŸπ’’
= 𝟎. πŸ’πŸ—πŸŽ
π‘³πŸπ’’ = 𝟎. πŸ’πŸŽπŸ‘πŸ‘
𝑳′′𝒒 = 𝑳𝒍 +
𝟏
𝟏
= 𝟎. πŸπŸ• +
= 𝟎. 𝟐𝟐𝟎
𝟏
𝟏
𝟏
𝟏
𝟏
𝟏
+
+
+
+
𝑳𝒂𝒒 π‘³πŸπ’’ π‘³πŸπ’’
𝟏. πŸ“πŸ“ 𝟎. πŸ’πŸŽπŸ‘πŸ‘ π‘³πŸπ’’
π‘³πŸπ’’ = 𝟎. πŸŽπŸ“πŸ—πŸ‘
π‘ΉπŸπ’’ =
π‘ΉπŸπ’’
𝑳𝒂𝒒 + π‘³πŸπ’’ 𝟏. πŸ“πŸ“ + 𝟎. πŸ’πŸŽπŸ‘πŸ‘
=
= 𝟎. πŸŽπŸπŸŽπŸ–
𝑻′π’’πŸŽ
𝟎. πŸ’πŸ– ∗ πŸ‘πŸ•πŸ•
⁄𝒕
𝒃𝒂𝒔𝒆
𝟏
𝟏
+ π‘³πŸπ’’
+ 𝟎. πŸŽπŸ“πŸ—πŸ‘
𝟏⁄
𝟏⁄
𝟏
+
⁄𝟏. πŸ“πŸ“ + 𝟏⁄𝟎. πŸ’πŸŽπŸ‘πŸ‘
𝑳𝒂𝒒
π‘³πŸπ’’
=
=
= 𝟎. πŸŽπŸπŸ”πŸ–
𝑻′′π’’πŸŽ
𝟎. πŸŽπŸ” ∗ πŸ‘πŸ•πŸ•
⁄𝒕
𝒃𝒂𝒔𝒆
10’
b
𝑳𝒅 = 𝑳𝒍 +
𝑳′𝒅 = 𝑳𝒍 +
𝑳′′𝒅 = 𝑳𝒍 +
𝟏
𝟏⁄
𝑳𝒂𝒅
𝟏
𝟏⁄
𝟏
𝑳𝒇𝒅 + ⁄𝑳𝒂𝒅
𝟏
𝟏⁄
𝟏
𝟏
𝑳𝒇𝒅 + ⁄𝑳𝒂𝒅 + ⁄π‘³πŸπ’…
𝑳𝒅 > 𝑳′𝒅 > 𝑳′′𝒅
𝑻′π’…πŸŽ =
𝑻′′π’…πŸŽ =
𝑳𝒂𝒅 + 𝑳𝒇𝒅
𝑹𝒇𝒅
π‘³πŸπ’… + 𝑳𝒂𝒅 //𝑳𝒇𝒅
π‘ΉπŸπ’…
𝑹𝒇𝒅 β‰ͺ π‘ΉπŸπ’… ,
𝑳𝒂𝒅 + 𝑳𝒇𝒅 ≫ π‘³πŸπ’… + 𝑳𝒂𝒅 //𝑳𝒇𝒅
𝑻′π’…πŸŽ ≫ 𝑻′′π’…πŸŽ
2’
c (Kundur’s Example 3.1 in Page 90, slide #48)
𝑬𝑺𝒃𝒂𝒔𝒆 =
πŸπŸ’
√πŸ‘
= πŸπŸ‘. πŸ–πŸ” π’Œπ‘½
𝒆𝑺𝒃𝒂𝒔𝒆 = √πŸπ‘¬π‘Ίπ’ƒπ’‚π’”π’† = πŸπŸ—. πŸ”πŸŽ π’Œπ‘½
𝑰𝑺𝒃𝒂𝒔𝒆 =
𝑽𝑨𝒃𝒂𝒔𝒆
πŸ’πŸ–πŸ‘ ∗ πŸπŸŽπŸ”
=
= 𝟏𝟏. πŸ”πŸ π’Œπ‘¨
πŸ‘π‘¬π‘Ίπ’ƒπ’‚π’”π’† πŸ‘ ∗ πŸπŸ‘. πŸ–πŸ“πŸ” ∗ πŸπŸŽπŸ‘
π’Šπ‘Ίπ’ƒπ’‚π’”π’† = √πŸπ‘°π‘Ίπ’ƒπ’‚π’”π’† = πŸπŸ”. πŸ’πŸ‘ π’Œπ‘¨
𝒆𝑺𝒃𝒂𝒔𝒆
= 𝟏. πŸπŸ—πŸπŸ“ 𝜴
π’Šπ‘Ίπ’ƒπ’‚π’”π’†
𝒁𝑺𝒃𝒂𝒔𝒆 =
𝑳𝑺𝒃𝒂𝒔𝒆 =
𝑳𝒂𝒇𝒅𝒃𝒂𝒔𝒆 (= 𝑴𝑭𝒃𝒂𝒔𝒆 ) =
𝒁𝑺𝒃𝒂𝒔𝒆
= 𝟎. πŸŽπŸŽπŸ‘πŸπŸ” 𝑯
πŽπ’ƒπ’‚π’”π’†
𝑳𝑺𝒃𝒂𝒔𝒆
𝟎. πŸŽπŸŽπŸ‘πŸπŸ”
π’Šπ‘Ίπ’ƒπ’‚π’”π’† =
∗ πŸπŸ”. πŸ’πŸ‘ ∗ πŸπŸŽπŸ‘ = 𝟎. πŸŽπŸπŸ•πŸ• 𝑯
π’Šπ’‡π’…π’ƒπ’‚π’”π’†
πŸπŸ–πŸ•πŸ“
(Generator modeling – slide #36)
𝒆𝒇𝒅𝒃𝒂𝒔𝒆 =
𝑽𝑨𝒃𝒂𝒔𝒆
= πŸπŸ“πŸ•. πŸ” π’Œπ‘½
π’Šπ’‡π’…π’ƒπ’‚π’”π’†
𝒁𝒇𝒅𝒃𝒂𝒔𝒆 =
𝒆𝒇𝒅𝒃𝒂𝒔𝒆
= πŸπŸ‘πŸ•. πŸ‘πŸ— 𝜴
π’Šπ’‡π’…π’ƒπ’‚π’”π’†
𝑳𝒇𝒅𝒃𝒂𝒔𝒆 =
𝒁𝒇𝒅𝒃𝒂𝒔𝒆
= πŸ‘πŸ”πŸ’. πŸ’ π’Žπ‘―
πŽπ’ƒπ’‚π’”π’†
𝑳𝒍 = 𝑳̅𝒍 𝑳𝑺𝒃𝒂𝒔𝒆 = 𝟎. πŸ“πŸ‘πŸ– π’Žπ‘―
𝑳𝒂𝒅 = 𝑳̅𝒂𝒅 𝑳𝑺𝒃𝒂𝒔𝒆 = πŸ“. πŸπŸ“πŸ” π’Žπ‘―
𝑳𝒂𝒒 = 𝑳̅𝒂𝒒 𝑳𝑺𝒃𝒂𝒔𝒆 = πŸ’. πŸ—πŸŽπŸ‘ π’Žπ‘―
𝑳𝒅 = 𝑳𝒂𝒅 + 𝑳𝒍 = πŸ“. πŸ”πŸ—πŸ’ π’Žπ‘―
𝑳𝒒 = 𝑳𝒂𝒒 + 𝑳𝒍 = πŸ“. πŸ’πŸ’πŸ π’Žπ‘―
Μ… 𝑭 = 𝑳̅𝒂𝒅
𝑴
𝑳𝒂𝒇𝒅 (= 𝑴𝑭 ) = 𝑳̅𝒂𝒅 𝑳𝒂𝒇𝒅𝒃𝒂𝒔𝒆 = πŸ’πŸ“. πŸπŸ–πŸ– π’Žπ‘―
Μ… 𝑹 − 𝑳̅𝒂𝒅 = 𝟎
𝑴
Μ… 𝑹 = 𝟏. πŸ•πŸ“πŸ‘πŸ• 𝒑𝒖
𝑳̅𝒇𝒇𝒅 (= 𝑳̅𝑭 ) = 𝑳̅𝒇𝒅 + 𝑴
(Generator modeling – Slide #44)
𝑳𝒇𝒇𝒅 (= 𝑳𝑭 ) = 𝑳̅𝒇𝒇𝒅 𝑳𝒇𝒅𝒃𝒂𝒔𝒆 = πŸ”πŸ‘πŸ—. 𝟏𝟏𝟏 π’Žπ‘―
𝑳𝒇𝒅 = 𝑳̅𝒇𝒅 𝑳𝒇𝒅𝒃𝒂𝒔𝒆 = πŸ’πŸ“. πŸŽπŸ—πŸ π’Žπ‘―
Μ… 𝒂 𝒁𝑺𝑩 = 𝟎. πŸŽπŸŽπŸ‘πŸπŸ 𝜴
𝑹𝒂 = 𝑹
Μ… 𝒇𝒅 𝒁𝒇𝒅𝒃𝒂𝒔𝒆 = 𝟎. πŸπŸ•πŸ‘ 𝜴
𝑹𝒇𝒅 = 𝑹
19’
d
𝑳𝒅 (𝒔) = 𝑳𝒅
(𝟏 + 𝒔𝑻′𝒅 )(𝟏 + 𝒔𝑻′′
𝒅)
′
(𝟏 + π’”π‘»π’…πŸŽ )(𝟏 + 𝒔𝑻′′
π’…πŸŽ )
𝟏
𝟏⁄
𝟏⁄ + 𝑳𝒇𝒅
+
𝑳𝒂𝒅
𝑳𝒍
𝑻′𝒅 =
∗ 𝒕𝒃𝒂𝒔𝒆 = 𝟎. πŸ“πŸ–πŸ” 𝒔
𝑹𝒇𝒅
𝟏
𝟏⁄
𝟏
𝟏⁄ + π‘³πŸπ’…
+
+
⁄
𝑳𝒂𝒅
𝑳𝒇𝒅
𝑳𝒍
𝑻′′𝒅 =
∗ 𝒕𝒃𝒂𝒔𝒆 = 𝟎. πŸŽπŸπŸ’πŸ• 𝒔
π‘ΉπŸπ’…
𝑳𝒅 (𝒔) = 𝟏. πŸ–
(𝟏 + 𝟎. πŸ“πŸ–πŸ”π’”)(𝟏 + 𝟎. πŸŽπŸπŸ’πŸ•π’”)
(𝟏 + πŸ‘. πŸ•π’”)(𝟏 + 𝟎. πŸŽπŸ‘πŸπ’”)
4’
4. Simplified synchronous machine models (15 points): Continuing with Question 1, assume that the
generator is operated with the armature terminal voltage at rated value and its steady-state outputs are
Pt=250MW and Qt=115MVAr. Neglect saturation and saliency (i.e. let Xq=Xd, X’q=X’d and X”q=X”d),
a. Calculate air-gap torque Te in per unit and in Nm.
b. Calculate Eq for the simplified steady-state model, E” for the Voltage behind X” model and E’ for the
classic model.
c. Draw a phasor diagram showing phasors about these quantities: Et, It, jXsIt, RaIt, Eq, E’, jX’dIt, E” and
jX”dIt
a (slide #52, Kundur’s Page 101)
̅𝒕 = 𝟏
𝑬
̅𝒕 =
𝑷
πŸπŸ“πŸŽ
= 𝟎. πŸ“πŸπŸ•πŸ”
πŸ’πŸ–πŸ‘
̅𝒕 =
𝑸
𝑰̃𝒕 = (
πŸπŸπŸ“
= 𝟎. πŸπŸ‘πŸ–
πŸ’πŸ–πŸ‘
̅𝒕
Μ… 𝒕 + 𝒋𝑸
𝑷
)∗ = 𝟎. πŸ“πŸ•πŸŽ∠ − πŸπŸ’. πŸ•πŸŽ°
̅𝒕
𝑬
cos=0.9085
̅𝒆 = 𝑷
̅𝒕 + 𝑹
Μ… 𝒂 π‘°Μ…πŸπ’• = 𝟎. πŸ“πŸπŸ–πŸ“
𝑻
𝑻𝒃𝒂𝒔𝒆 =
πŸ’πŸ–πŸ‘ ∗ πŸπŸŽπŸ”
= 𝟏. πŸπŸ–πŸ ∗ πŸπŸŽπŸ” π‘΅π’Ž
πŸ‘πŸ•πŸ•
̅𝒆 𝑻𝒃𝒂𝒔𝒆 = 𝟎. πŸ”πŸ’πŸ‘ ∗ πŸπŸŽπŸ” π‘΅π’Ž
𝑻𝒆 = 𝑻
6’
b
̃𝒒 = 𝑬
Μƒ 𝒕 + (𝑹𝒂 + 𝒋𝑿𝒅 )𝑰̃𝒕 = 𝟏. πŸ’πŸ‘πŸŽ + π’‹πŸŽ. πŸ—πŸ‘πŸ = 𝟏. πŸ•πŸŽπŸ”∠πŸ‘πŸ‘. πŸŽπŸ”πŸ–°
𝑬
Μƒ =𝑬
Μƒ 𝒕 + (𝑹𝒂 + 𝒋𝑿′𝒅 )𝑰̃𝒕 = 𝟏. πŸŽπŸ”πŸ— + π’‹πŸŽ. πŸπŸ’πŸ• = 𝟏. πŸŽπŸ•πŸ—πŸ‘∠πŸ•. πŸ–πŸπŸ°
𝑬′
Μƒ =𝑬
Μƒ 𝒕 + (𝑹𝒂 + 𝒋𝑿′′𝒅 )𝑰̃𝒕 = 𝟏. πŸŽπŸ“πŸ’ + π’‹πŸŽ. πŸπŸπŸ‘ = 𝟏. πŸŽπŸ“πŸ—πŸ–∠πŸ”. πŸπŸ‘πŸ°
𝑬′′
6’
c
3’
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