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Transcript
Module B4
Per Unit Analysis
1
B4.1
Per Unit Calculations
2
WHAT IS A PER UNIT VALUE?
• The numerical per-unit value of any quantity is its ratio
to the chosen base quantity of the same dimensions.
• A per-unit quantity is a normalized quantity
with respect to a chosen base value.
ADVANTAGES:
• device parameters tend to fall in a relatively fixed range,
making erroneous values prominent.
• ideal transformers are eliminated as circuit elements, resulting
in large saving in component representation and reduction in
computational burden.
• voltage magnitudes throughout a given normally operating
power system are close to unity, providing a way to perform
“sanity checks” on calculations.
3
How to convert to per unit system?
• Choose voltage base and power base.
• Compute current base, impedance base.
• Divide all actual quantities by the
respective base to get pu quantity, i.,e.
4
V
V pu 
,
Vbase
S
P
Q
S pu 
, Ppu 
, Qpu 
Sbase
Sbase
Sbase
I pu 
I
I base
Always use same
units in numerator
and denominator.
,
Z
Y
1
Z pu 
, (or Ypu 

)
Z base
Ybase Z pu
5
How to choose base voltage and base power?
• Mathematically,
– one voltage can be chosen to be any number
– power base can be chosen to be any number
6
How to choose base voltage and base power?
• Practically,
– one voltage should be chosen corresponding
to nominal voltage of associated part of system.
– power base should be chosen as a multiple
of 10, e.g., 10 kVA, 100 kVA, 1 MVA, 10 MVA, etc.,
depending on “size” of the system.
We will discuss later why we have
emphasized “one voltage”
7
How to compute base current and impedance?
base current, I 
base power S l
base voltage,VLN
base voltage, VLN (base voltage VLN ) 2
base impedance, Z =

base current, I
base power S1
base admittance, Y 
1
base impedance, Z
Use the above for 1 phase or 3 phase circuits.
8
Some comments on per unit in 3 phase circuits:
• For equations on previous page,
– voltages (actual & base) must be line to neutral
– powers (actual & base) must be per phase
– currents (actual & base) must be line current
(there is only a choice if there exists a delta connection)
9
Some comments on per unit in 3 phase circuits:
• We can obtain a line-line base voltage:
base voltage VLL  3 base voltage VLN
• We can obtain a base current for delta:
base current I  
base current I
3
10
More comments on per unit in 3 phase circuits:
• We can obtain a base impedance for delta:
base impedance Z   3 base impedance Z
Use the delta base for delta connected loads and the
Y-base for Y connected loads.
• We can obtain a base power for 3 phase:
base power S 3  3 base power S1
Use the 3-φ base for 3-φ power and the 1-φ base
for 1-φ power.
11
More comments on per unit in 3 phase circuits:
• Base current can also be computed using
line to line voltage:
base current I 
base power S1
base voltage,VLN


base power S 3 / 3
(base voltage VLL ) / 3
base power S 3
3 base voltage VLL
12
More comments on per unit in 3 phase circuits:
• Base impedance can also be computed using
line to line voltage. Recall:
base voltage, VLN (base voltage VLN ) 2
base impedance, Z =

base current, I
base power S1
Then substitution of VLN=VLL/√3 into the numerator
of both expressions yields:
(base voltage, VLL ) / 3 (base voltage VLL / 3) 2
base impedance, Z =

base current, I
base power S1
(base voltage VLL ) 2

3 base power S1
(base voltage VLL ) 2

base power S3
13
More comments on per unit in 3 phase circuits:
• Base current can also be computed using
line to line voltage:
base current I 
base power S1
base voltage,VLN


base power S 3 / 3
(base voltage VLL ) / 3
base power S 3
3 base voltage VLL
14
Please study example B4.1 (module B4),
which illustrates per unit analysis for a
simple single phase system.
We will look at a different example,
for a three phase system, in class. This
example is Problem B4.3 in your text.
This example was worked previously,
using per-phase analysis. It is useful
to compare the two approaches.
15
Refer to example B3.2 (see figure B3.8)
Three balanced three-phase loads are connected in
parallel. Load 1 is Y-connected with an impedance
of 150 + j50 ; load 2 is delta-connected with an impedance
of 900 + j600 ; and load 3 is 95.04 kVA at 0.6 pf leading.
The loads are fed from a distribution line with an
impedance of 3 + j24 . The magnitude of the line-to-neutral
voltage at the load end of the line is 4.8 kV.
Obtain total load current and total power delivered by
the source.
16
Let’s work this problem in per unit!
Choose:
base voltage VLN  4.8 kV  4800 volts,
base power S1  10 kVA  10,000 VA
17
1. Compute:
base voltage VLL  3(base VLN )  3(4800)  8313.8 volts
base power S 3  3(base power S1 )  3(10,000)  30,000 VA
base current I 
base power S 3
3 base voltage VLL
30,000 VA

 2.0833 A
3(8313.8)
(base voltage VLL ) 2 (8313.8) 2
base impedance Z 

 2304 
base power S 3
30,000
2. Convert from SI units into per unit:
ZL
3  j 24

 0.0013  j 0.0104
base impedance Z
2304
Z1
150  j 50
Z1 pu 

 0.0651  j 0.0217
base impedance Z
2304
Z2
300  j 200
Z 2 pu 

 0.1302  j 0.0868
base impedance Z
2304
Z Lpu 
We converted
the delta Z
into a Wye Z.
We could have
also divided
delta Z by
18
deltaZbase.
2. Convert from SI units into per unit (cont):
S3 pu 

S3,3
power base S3
S3,1
power base S1
VLoad , pu


95040(0.6  j 0.8)
 3.168(0.6  j 0.8)
30,000
31680(0.6  j 0.8)
 3.168(0.6  j 0.8)
10,000
VLoad , LN
4800


 1.0
voltage base VLN 4800
VLoad , LL
3(4800)


 1.0
voltage base VLL
8314
You can compute pu powers using 3 phase or per phase quantities.
You can compute pu voltages using LN or LL quantities.
But the numerator and denominator need to be consistent!
19
3. Compute the current into the load in pu.
I L , pu 
I1 pu

I 2 pu

I 3 pu
1.0
1.0
3.168(0.6  j 0.8)



0.0651  j 0.0217 0.1302  j 0.0868
1.0
 13.825  j 4.608  5.317 - j3.545  1.901 j2.534
 21.043  j 5.619 pu  21.780 - 14.951pu
Compare this answer with the one we obtained in
module B3, example B3.2, which was
45.3725 |_ -14.949 amperes. You see that we obtain different
mag, same angle. Let’s convert the pu answer to amps.
I L  I Lpu  base current I  (21.780  14.951)2.0833  45.375  14.951
So it is the same! This only works if bases are chosen
consistently and per-unitization is done correctly.
20
4. Compute losses in distribution line.
2
Ploss , pu  I Lpu RLpu  21.78  0.0013  0.6167 pu
2
2
Qloss , pu  I Lpu X Lpu  21.78  0.0104  4.9334pu
2
Let’s check to see if this is the same. Note carefully
that multiplication by per phase power base gives us
per phase power, and multiplication by 3 phase power
base gives us 3 phase power, which is what we want.
Previously, we obtained 18,528 watts and 148,224 vars.
Ploss  power base S3  Ploss , pu  (30,000)0.6167  18,501 watts
Qloss  power base S3  Qloss , pu  (30,000)4.9334  148,002 vars
There is small difference due to round-off error.
21
This diverges from
solution approach in
5. Let’s compute source voltage.
Ex. B3.2 (there we
computed powers
Van, pu  Vload , pu  I Lpu ( Z Lpu )
in loads), but it is an
 1.00  21.78  14.951(0.0013  j 0.0104) equally valid way to
obtain the power
 1.0858  j 0.2115  1.106211.0245
delivered in either pu
or per phase analysis.
Now we can obtain total source power and total load power.
S
 V ( I )*  1.106211.0245(21.78  14.951)
sending , pu
an , pu
Lpu
 21.659  j10.553 pu
Stotalload , pu  VLpu ( I Lpu )*  1.00(21.78  14.951)
 21.043  5.619 pu
22
6. Convert powers into watts & vars.
S sending ,3  S sending , pu (power base S3 )  (21.659  j10.553)30,000
 649,770  j316,590
Stotalload ,3  Stotalload , pu (power base S3 )  (21.043  5.619)30,000
 631,290  j168,570
Previously, we obtained
sending end power = 649,779+j316,770
receiving end power = 631,251+168,546
So again, difference is very small due to round-off error.
Re-emphasize: answers from pu will agree with answers
from per phase if bases are consistent and quantities have
been per-unitized correctly.
23
Homework problem (not to turn in but may be on quiz)
Choose your voltage base and power base as
base voltage VLN  5 kV  5000 volts,
base power S1  10 kVA  100,000 VA
Rework parts 1-6 of the previous problem.
You will know you have it correct if the
answers in SI units are the same.
Question: Will the per unit values of impedances,
voltages, currents, and powers be the same?
24