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3-Per Unit System

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ELEC-1104 Lecture 3: Lecture 3: Per Unit Systems Per Unit Systems
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  • ELEC-1104

    Lecture 3:Lecture 3:

    Per Unit SystemsPer Unit Systems

  • Basic Units

    The 4 basic electrical quantities are:Voltage V (volt)Current I (amp)Current I (amp)Impedance Z (ohm)P S (VA)Power S (VA)

    For single-phase circuits,V(volt) = Z(ohm) I(amp);S (VA) = V(volt) I(amp)*S (VA) V(volt) I(amp)

  • Per unit notation

    In per unit notation, the physical quantity isIn per unit notation, the physical quantity is expressed as a fraction of the reference value, i.e.va ue, .e.per unit value = actual value/base value in the same unitthe same unit.e.g. V(in per unit) = V(in kV)/V base (in kV)

    where the base value is a reference value for magnitude.magnitude.

  • Base QuantitiesQ

    In per unit notation we would like to keep the basic relations:

    Vpu = Zpu Ipu; Spu = Vpu Ipu*pu pu pu; pu pu pu Hence the base quantities should be chosen

    such thatsuch thatBase voltage (VB) =

    b i d (Z ) b t (I )base impedance (ZB) base current (IB)Base power (SB) =

    b l (V ) b (I )base voltage (VB) base current(IB)

  • Base QuantitiesQ

    Thus only two of the base quantities can beThus only two of the base quantities can be arbitrarily chosen, the other two will follow directly.d ect y. It is common practice to specify

    b (S ) d b lt (V )base pwer (SB) and base voltage (VB) Then it follows

    base current IB = SB/VBbase impedance ZB = VB/IB =VB2/SBp B B B B B

  • Percentage Valuesg

    An equivalent way to express the per unitAn equivalent way to express the per unit value is the percentage value where

    Percentage value = per unit value 100%

    However, percentage values are not so convenient to use sinceconvenient to use since

    Vpercent Zpercent Ipercent

  • Example 1p

    Given V = 10030oGiven V 10030Z = 3 + j4 = 553.1o

    Fi d t Find currentactive, reactive, & apparent powerpower factor

    I ZI

    VV

  • Solution 1

    Take (for example)( p )Base power SB = 1 kVA Base voltage V = 100 VBase voltage VB 100 V

    ThenBase current I = S /V = 10 ABase current IB = SB/VB = 10 ABase impedance ZB = VB/IB = 10

    Given V = 100 30o V = 1.0 30o p.u.Z 553 1o 0 553 1oZ = 553.1o = 0.553.1o p.u.

  • Solution 1 (cont)( )

    Current I = V/Z = 2.0 -23.1o p.u

    = 2 010-23 1o A = 20-23 1o A 2.010 23.1 A 20 23.1 A Complex power

    S = VI* = 2 0 53 1o p u = 1 2 + j1 6 p u S = VI* = 2.0 53.1o p.u = 1.2 + j1.6 p.u. Apparent power S = 2.01 = 2 kVA

    Acti e po er P 1 21 1 2 kW Active power P = 1.21 = 1.2 kW Reactive power Q = 1.61 = 1.6 kVAr

    P f t f P/S 1 2/2 0 0 6 Power factor p.f. = P/S = 1.2/2.0 = 0.6

  • Base Value for 3-phase systemsp y

    For 3-phase systems it is common practiceFor 3 phase systems it is common practice to describe system operation with:

    total 3-phase power S = Stotal 3-phase power S = S3-line voltage V = Vlineline current I = Ilineequivalent impedance/phase Z = Zphp

    with (in magnitude)V = 3ZI; S = 3VIV 3ZI; S 3VI.

  • Base Value for 3-phase systemsp y

    Hence if base values are chosen for:Hence if base values are chosen for:total 3-phase power SBli lt Vline voltage VB

    Thenbase line current

    IB = SB/ 3VBB SB VBbase impedance

    Z V / 3I V 2/SZB = VB/ 3IB = VB2/SB

  • Example 2p

    Supply: 400 V, 50 Hz, 3-phaseSupply: 400 V, 50 Hz, 3 phase Load: 3 identical coils with Z = 20+j15

    in star connectionin star connection.

    Find: line currentpower suppliedpower factor.

  • Solution 2

    Take (for example)( p )Base power (total 3-phase) SB = 10 kVABase voltage (line-to-line) V = 400 VBase voltage (line-to-line) VB 400 V

    ThenBase current I = S /3V = 14 43 ABase current IB = SB/3VB = 14.43 ABase impedance ZB = VB2/SB = 16

    Given V = 400 V = 1.0 p.u.Z 2536 9o 1 562536 9oZ = 2536.9o = 1.562536.9o p.u.

  • Solution 2 (cont)( )

    Current/ 1 0 /1 62 0 64I = V/Z = 1.0 /1.5625 p.u. = 0.64 p.u.

    = 0.6414.43 A = 9.235 A Apparent power

    S = VI = 1.00.64 = 0.64 p.u. = 6.4 kVA Power factor

    p.f. = cos 36.9o = 0.8p Active power

    P = VI pf = 0.64 0.8 p.u = 0.512 p.u.p p p= 0.512 10 = 5.12 kW

  • Choice of Base values

    For a connected circuit, it is obvious that the same ,bases should be used for the whole network such that the normal circuit theorems would also apply to per unit values, e.g.Kirchhoff laws

    At a given node, i(Ipu)i = 0Around a mesh i(Vpu)i = 0

    Impedance in series Zpu = (Zpu)1+ (Zpu)2Admittance in parallel Ypu = (Ypu)1+ (Ypu)2

  • Base values for a transformer

    In a transformer, two circuits are not directlyIn a transformer, two circuits are not directly connected but magnetically coupled. The voltages of the windings are in the ratio of vo tages o t e w d gs a e t e at o oturns and currents in inverse ratio.

    For the coupled circuit we should then chooseFor the coupled circuit, we should then choose The same base power Base voltages in the ratio of turns Base voltages in the ratio of turns.

    This will ensure Spu, Vpu, Ipu, to remain unchanged when passing through an ideal transformerwhen passing through an ideal transformer

  • Base values for a transformer

    LetLet n1,n2 be the number of turns in primary and

    secondary windingsecondary winding.Z1, Z2 be the primary and secondary winding

    impedance.impedance.Then total impedance referred to primary

    Z 1 = Z1 + (n1/n2)2Z2ZT1 Z1 + (n1/n2) Z2and total impedance referred to secondary

    Z = Z + (n /n )2Z = (n /n )2ZZT2 = Z2 + (n2/n1)2Z1 = (n2/n1)2ZT1

  • Base values for a transformer

    If base values were chosen for the transformer:If base values were chosen for the transformer:SB1 = SB2; VB1 = (n1/n2)VB2

    ThThenIB1 = (n2/n1)IB2 ; ZB1 = (n1/n2)2ZB2

    Thus per unit impedance of transformerZpu = ZT1/ZB1 = ZT2/ZB2pu T1 B1 T2 B2

    is the same whether we use the total impedance referred to primary or secondaryimpedance referred to primary or secondary.

  • Equivalent circuit for transformerq

    In the per unit representation, the equivalentIn the per unit representation, the equivalent circuit of a transformer is a simple winding impedance Zpu (with excitation branch peda ce pu (w t e c tat o b a cignored)

    (I ) (I )

    (V ) (V2)pu

    (I1)pu (I2)pu

    (Z)pu(V1)pu (V2)pu

  • Base Conversion

    If the per unit values are given based on SB1If the per unit values are given based on SB1and VB1 which are different from the chosen base SB2 and VB2 for analysis, the given per base SB2 a d VB2 o a a ys s, t e g ve peunit values must be modified before they can be used. Thusc be used. us

    (Vpu)2 = V/VB2 = (Vpu)1VB1/VB2(Spu)2 = S/SB2 = (Spu)1SB1/SB2

  • Base Conversion

    SimilarlySimilarly(Ipu)2 = I/IB2 = (Ipu)1IB1/IB2

    = (Ipu)1VB2/VB1 SB1/SB2(Z ) = Z/Z = (Z ) Z /Z(Zpu)2 = Z/ZB2 = (Zpu)1ZB1/ZB2

    = (Zpu)1(VB1/VB2)2 SB2/SB1

  • Examplep

    Given a 50 MVA, 3.3 kV generator has aGiven a 50 MVA, 3.3 kV generator has a synchronous impedance of 10%. Find the per unit impedance on a base ofFind the per unit impedance on a base of

    100 MVA and 5 kV.

    Zp.u. = 0.1 x (3.3/5.0)2 x (100/50)= 0.087 p.u.

  • Examplep

    Choose base powerpSbase = 20 MVA

    Base voltages G1 G220MVAX=15%

    40MVAX=20%

    ase vo tagesVbase1 = 11 kVVbase2 = 33 kV

    1 2

    11 kVbase2

    ThenXG1 = 0.15pu

    11/33kV60MVAX=12%

    11 kV

    33 kV

    TXG1 0.15puXG2 = 0.20x20/40=0.10puXT = 0.12x20/60=0.04pu

    33 kV

    T

  • Advantages of Per Unit Systemg y

    Normally we are dealing with numericsNormally we are dealing with numerics near unity rather than over a wide range. Provides a more meaningful comparison ofProvides a more meaningful comparison of

    parameters of machines with different ratingsratings. As the per unit values of parameters of a

    hi f i d i ll f llmachine of a given design normally falls within a certain range, a typical value can be sed if s ch parameters are not pro idedbe used if such parameters are not provided.


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