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Distribution Voltage Regulation
The voltage at every customer’s service
  entrance must remain within acceptable
  tolerances. Common methods of regulating
  the voltage are:
  1. Step- type voltage regulators
  2. Load tap changing transformers and
  3. Shunt Capacitors.
Two Winding Transformer Theory




Standard Markings:        High Voltage Side: H1, H2
                          Low Voltage Side: X1, X2
s.t. (a) at no load, Vs is in phase with VL
   (b) under s.s. load conditions I1 in phase with I2
Referring the leakage impedance to the secondary, we have:




 The total leakage impedance is now given by:
         Zt = nt2 Z1 + Z2         … (1)
 where nt = N2/N1

 For an ideal transformer:
          E2 = N2/N1E1 = ntE1             … (2)
          I1 = N2/N1I2 = ntI2             … (3)
 Applying KVL to the secondary:
          E2 = VL + I2Zt                  … (4)
 But      VS = E1 = 1 E2 = 1 VL + Zt I2   … (5)
Equation (5) can be written as:
       VS = a.VL + b.I2         … (6)
where a = 1 and                 … (7)
           nt
       b = Zt                   … (8)
           nt
Also, IS = Ym.VS + I1                  … (9)
Sub (3) and (5) into (9)
        IS = Ym. 1 [ VL + ZtI2 ] + nt.I2
                 nt
        IS = Ym VL + [ YmZt + nt ] I2 … (10)
             nt          nt
In general form, (10) can be rewritten as
        IS = c. VL + d. I2      … (11)
where c = Ym                    … (12)
             nt
        d = Y .Z + n            … (13)
We now have a model of a 1Φ transformer as a two port device:
i.e.:
         VS = a.VL + b. I2          … (6)
         IS = c. VL + d. I2         … (11)
where the a, b, c, d constants are:
         a=1 ;              c = Ym
             nt                 nt
         b = Zt ;           d = Ym.Zt + nt
              nt                 nt
If the O/P voltage is needed, then (6) can be rewritten as:
         VL = 1/a VS – b/a I2              … (14)
Sub. for a and b in (14) we get
         VL = AVS – BI2             … (15)
where A = 1/a = nt                  … (16)
∴        B = b/a = Zt               … (17)
    VL = ntVS – ZtI2
Example:
A 1Φ transformer is rated 75kVA 2400/240 V. The
transformer has the following impedances and shunt
admittances:
Z1 = (0.612 + j1.2) Ω (HV)
Z2 = (0.0061 + j0.0115) Ω (LV)
Ym = (1.92x10-4 – j8.52x10-4) s (referred to HV side)

Determine the generalized a, b, c, d constants as well as
the A and B constants for the transformer. What should
be the primary Voltage and Current at rated kVA and 0.9
p.f. lag.
Solution:
Nt = N2 = 240 = 0.1
      N1 2400
Equivalent impedance of transformer referred to L.V.
           Zt = Z2 + nt2.Z1 = 0.0122 + j0.0235
The generalized constants are:
a = 1/nt = 10         ;         b = Zt/nt = 0.122 + j0.235
c = Ym/nt = 0.0019 – j0.0085
d = Ym.Zt + nt = 0.1002 – j0.0001
       nt
A = nt = 0.1          ;         B = Zt = 0.0122 + j0.0235

   VL = 240 ∠ 0
Assuming that transformer operating at 75kVA, 240 V 0.9 lag (Rated)

    I2 = 75 x 1000 ∠ -25.84 = 312.5 ∠-25.84
           240

   VS = aVL + bI2 = 2466.9 ∠ 1.15 V
Applying the values of a, b, c and d parameters:

    IS = cVL + dI2 = 32.67 ∠ -28.75 A
Two Winding Auto-Transformer (Buck/
               Boost Transformer)
        • The two winding transformer can be
          connected as an autotransformer.
STEP
 UP
        • This is done by connecting X2 to H1 and
          taking the output from X1H2 for step up.
 STEP
DOWN    • Connect X1 to H1 and output is X2H2.
        • LV winding is referred to as the “series”
          winding and the HV winding as the “shunt”
          winding (in relation to the Load).
STEP- UP AUTO TRANSFORMER
In this case, the total equivalent impedance is referred to the “series”
winding.
(Boost Transformer) Applying KVL to secondary circuit:
        E1 + E2 = VL + Zt.I2                     … (1)
Or      E1 + ntE1 = (1 +nt)E1 = VL + Zt.I2 … (2)
From the circuit: VS = E1 and I2 = IL            … (3)

Sub (3) into (2)
         VS = 1 VL + Zt . I L                             … (4)
              1+nt      1+nt
Or       VS = a’.VL + b’.IL                               … (5)
where a’ = 1                and   b’ = Zt
             1+nt                     1+nt

Applying KCL to node X2
       IS = I1 + I2 + Iex                                 … (7)
       IS = (1+nt)I2 + Iex
          = (1+nt)I2 + YmVs                               … (8)
Sub (4) into (8) gives:

                           1             Zt       
 I S = (1 + nt ).I 2 + Ym        .VL +       .I 2 
                          1 + nt       1 + nt 


              Ym            Ym .Z t          
      I S=           .VL +          + 1 + nt  I 2      … (9)
           (1 + nt )        1 + nt           
But       I2 = IL
Or        IS = c’.VL + d’.IL                             … (10)

where      c’ = Ym             and   d’ = YmZt +1 + nt   … (11)
               (1+nt)                    (1+nt)
Step Down Auto-Transformer
           (X1 connected to H1)




In this case for KVL => E1- E2 = VL + I2Zt
If the analysis is continued as before we get;
         VS = aVL + bIL                           … (12)
          IS = cVL + dIL                          … (13)


                                             }
where a = 1               b = Zt
              1-nt            1-nt                  (14)
         c = Ym           d = YmZt + 1 –nt
  ∴           1-nt             1-nt
[ the only difference is the sign of the turns ratio.]
 ∴
    Generalized Constants for Auto-Transformer can be defined as:
         a= 1
              1±nt
         c = Ym
              1±nt
                          b = Zt
                              1±nt
                          d = YmZt + 1 ± nt
                              1±nt
                                             }      (15)




From (12)     VL = 1/a.VS – b/a.IL             ... (16)
Or            VL = A.VS – BIL
where A = 1/a = 1±n     ;      B = b/a = Z     … (17)
The generalized equations for the auto-

transformer are of exactly the same form as

was derived for the two winding transformer

as well as for a transmission line. (In terms of

a, b, c, d constants). These single phase

values will be expanded to a 3x3 matrix for

the 3Φ transformer.
Rating of Autotransformer
The rating is given by: VSIS or VLIL
Let:    kVAxfm = kVA rating of two winding transformer
        kVAauto = kVA “        “ autotransformer
        Vrated1 = E1 = rated source voltage
        Vrated1 = E2 = rated load voltage
        Vauto S = rated source voltage of autotransformer
        Vauto L = rated load voltage autotransformer

Neglecting voltage drop across Zt
        Vauto L = E1 ± E2 = (1 ± nt)E1   … (18)
∴       kVAauto = Vauto L . I2 = (1 ± nt)E1I2 … (19)
But I1 = ntI2
    ∴ kVAauto = (1 ± nt) . E1. I1               … (20)
                       nt
But E1I1 = kVAxfm
    ∴
           kVAauto = (1 ± nt) kVAxfm            … (21)
                         nt
Fundamental Equations for Buck/Boost transformer:
(1)       Vauto L = (1 ± nt) E1
          kVAauto = (1 ± nt) kVAxfm
                         nt
where nt = N2
              N1
Example:
The 75kVA 2400/240V transformer given before is connected as a step-up auto
transformer.
1.Determine the kVA rating and voltage output of this arrangement.
2.If the auto transformer is supplying rated kVA at rated voltage at 0.9 lag,
determine source voltage and current.
nt = 0.1       ; kVAxfm = 75         2400/240
  ∴
1. ∴ kVAauto = ( + 0.1 ) 75 = 825 kVA
                1
                   0.1
        V1 = VS = 2400

           Vauto L = (1 + n) E1
                     = (1.1)(2400) = 2640 V
                      = (V1 + V2) = (2400 + 240)
                          = 2640V
(2)          VL = 2640 ∠0 V

      I2 = 825 x 103 ∠ -25.84 = 312.5 ∠ -25.84 A
            2640 /0

       ∴ a = 1/(1+0.1) = 0.9091
              b = 0.0122 + j0.0235 = (0.0111 + j0.0214)
                      1 + 0.1
 ∴      c = (1.92 – j8.52) x 10-4 = (1.7364 – j7.7455) x 10-4
                 1 + 0.1

∴       [                                         ]
      d = (1.92 – j8.52)(0.0122 + j0.0235) x 10-4 + 1 + 0.1
                            1 + 0.1

            = (1.1002 – j0.000005)
But     VS = aVL + bIL
         IS = cVL + dIL



        VS = (a)2560 ∠ 0 + b(312.5 ∠ -25.84)
Sub for a, b, c and d we get:


           = 2406 ∠ 0.1 V
        IS = (c)(2640 ∠ 0) + d(312.5 ∠ -25.84)
           = 345.06 ∠ -26.11

Check VL = AV –BIL

where A = 1 + nt = 1.1
      B = Zt = 0.0111 + j0.0235

        VL = (1.1)(2406 ∠ 0.1) – (0.0111 + j0.0235)(312.5 ∠ -25.84)
           = 2640 ∠ 0
Step Voltage Regulators
1. A step voltage regulator consists of an auto
   transformer and a load tap changing mechanism.
2. Voltage changes obtained by changing taps in series
   winding.
3. The position of tap controlled by a control unit
   called the line drop compensator.
4. Regulator has a reversing switch enabling a ± 10%
   regulating range typically in 32 steps.
5. On a 120V basis this yields 0.75V per step.
6. As per ANSI/IEEE C57-1986 standard there are two
   types: Type A and Type B. (Type B more common)
CONTROL SETTINGS

a.Voltage Level -: Voltage to be maintained.

b.Bandwidth -: Deadband.
     If (a) = 122V and Bandwidth = 2V then voltage is
between 121-123.

c.Time Delay -: Wait time before execution of a tap
change.

d.Line Drop Compensator -: Used to compensate for Vdrop
due to line impedance.
TYPE B Step- Voltage Regulator
TYPE A Regulator
Note:   In type B regulator, the core excitation is constant because the
        shunt winding is connected to the control circuit i.e. the
regulated line drop compensator.
Diagram gives Regulator in Raise (step up) connection (R). For Lower (L) (step
down) the switch is moved to ‘L’.
Voltage Equations                              Current Equations
E1 = E2                                        N1I1 = N2I2                          … (1)
N1      N2
VS = E1 – E2                                   IL = IS – I1                 … (2)
VL = E1                                        I2 = IS                              … (3)
E2 = N2 E1 = N2 VL                             I1 = N2 I2 = N2 IS           … (4)
        N1          N1                               N1            N1
VS =    [1 – N ]V
                2        L                          [
                                               IL = 1 – N2         ]I   s   … (5)
               N1                                             N1
VS = ar . VL        where    ar = 1 – N2 IL = ar . IS                       … (6)   … (7)
                                 (    N1
                                           )
When the switch is placed on L (Lower or step down) only equation (2)
changes -: VS = E1 + E2 ; IL = IS + I1

This again gives equation (6) but in this case
         a r = 1 + N2                                          … (8)
                   N1
If N2/N1 is not known but we know the tap change is 0.75V.
∴Effective regulator ratio for type B regulator:
    On 120V ; 0.75V = 0.00625 p.u.
   ∴ effective ratio   = ar = 1 ± (0.00625)(# tap)             … (9)
        where:     -   = raise
                   +   = lower
Generalized Constants (a, b, c, d)
For Type A and Type B regulators we have:
  Type A:        VS = 1 VL    ;   IS = arIL
                       ar
  Type B:        VS = arVL    ;   IS = 1 IL
                                        ar
                  Effective ratio

                                              }
with             Type A           Type B          For
                                                  equation
        raise        +                 -          (9)
        lower         -                +
∴Generalized Constants for 1Φ step-voltage regulator are:
 Type A:      a = 1/ar   b=0     c=0     d = ar      … (10)

 Type B:      a = ar     b=0     c=0     d = 1/ ar   … (11)

 where ar is given by (9) with sign given by table before.
Line Drop Compensator
The changing of the taps on a regulator is controlled by the line drop
  compensator.




                        Line Drop Compensator
a) The current transformer ratio is specified as CTp:CTs where the
   primary rating (CTp) is typically the rated current for the circuit
   (or feeder).

b) The compensator is an analog circuit i.e. it is a scale model
   (R’ + jX’) of the line impedance (RL + jXL).
   (R’ + jX’ -: scale model; replica impedance; analog of the line)

c) R’ + jX’ is calibrated in volts

d) ZL pu = Zcomp pu
Table of Base Values
Base                    Line Cct                Compensator Cct
Voltage                 VLN                     VLN/Npt
Current                 CTp                     CTs
Zbase                   VLN/CTp                 VLN/( Npt . CTs)
   From this we can derive R’ & X’ (Compensator)
           Rpu + jXpu = RL + jXL
                         Zbline
        ∴ R + jX = (R + jX ) CT              … (1)
            pu     pu    L      L  p
                                  VLN
   For the compensator to function, ZL pu = Zcomp pu.
        ∴
          (Rcomp + jXcomp)Ω = (Rpu + jXpu)Zbase comp
        ∴
            (Rcomp + jXcomp)Ω = (RL + jXL) CTp . VLN
                                            VLN (Npt . CTs)
   Or       (Rcomp + jXcomp)Ω = (RL + jXL) CTp . 1        … (2)
Equation (2) gives the ohmic value of the compensator.
To obtain the R and X settings in Volt we multiply the ohmic value by
the rated current:
        (R’ + jX’) volt = (Rcomp + jXcomp). CTs
        (R’ + jX’) volt = (RL + jXL) CTp. CTs
                                     Npt. CTs
     ∴ (R’ + jX’) volt = (R + jX ) CT           volt   … (3)
                           L    L     p
                                     Npt

Example:
For the compensator circuit given before, the regulator (transformer)
rated 5000kVA, 115 delta- 4.16kV grounded wye and the equivalent
line impedance from the Regulator to the load centre is (0.3 + j0.9)Ω.
a) Determine the VT and CT ratings for the compensator cct.
b) Determine the R and X setting of the compensator in Ω and volts.
Solution:
a)     VLG = 4160/ √3 = 2401.8 V.
         For a 120V compensator operation (Normal voltage)
                  Npt = 2401.8 ≈ 20
                          120
         Rated current of Regulator = 5000 = 693.9 A
                                          √3. x 4.16
     ∴        Select primary rating of CT as 700A
         Assuming compensator secondary = 5A
      CT = CTp = 700 = 140
                CTs        5
b)         (R’ + jX’) volts = (RL + jXL) CTp
                                         Npt
                            = (0.3 + j0.9) 700 /20 = (10.5 + j31.5) V
         The R and X setting in Ω is obtained by dividing the volt settings by CTs
         (current rating)
                           (RΩ +jXΩ) compensator = (10.5 + j31.5)/5
                                                   = (2.1 + j6.3) Ω
         Remember that the compensator is set in volts i.e. at (10.5 + j31.5) V.
Example:
Assume the regulator is supplying 2500kVA at 4.16kV, 0.9 p.f. lag. If the voltage
level at the load centre is to be 120V of bandwidth 2V, determine the tap
setting of the regulator.

Solution:
As calculated before:
      Setting of regulator = R’ + jX’ = (10.5 + j31.5) V

   ∴ IL = 2500 ∠ -25.84 = 346.97 ∠-25.84 A
      VL = 120 ± 1


   ∴ Icomp = 346.97 ∠ θ = 2.4783 ∠ -25.84 A
              √3 x 4.16


Input voltage to regulator = 4160 ∠ 0 = 120.09 ∠ 0
                  140

                                √3 x 20

         Vdrop = (2.1 + j6.3)(2.4783 ∠-25.84) = 16.458 ∠ 45.72 V
Voltage drop in compensator cct = (Zcomp)Ω (Icomp).

∴
        VR = Vreg – Vdrop = (120.09 ∠ 0) – (Vdrop)
    Voltage across compensator relay = VR

     ∴
NB:
VR represents the voltage expected at the load centre due to the
voltage drop across the line (RL + jXL)
The min. value for this voltage should be 119V.
 ∴ the regulator has to raise Taps.
Recall for a typical regulator, on tap ≡ 0.75V
  ∴ # of taps required = 119 – 109.24     = 13.02
                                0.75
  ∴ for a Type B regulator in raise position the effective ratio is:
                ar = 1 - (0.00625)(# of taps)
                   = 1 – (0.00625)(13)          (for Type B “raise”)
                   = 0.9188
  ∴ the generalized constants for modeling this regulator for
this operating condition are:
       a = ar = 0.9188                  c=0
       b=0                              d = 1/ar = 1.0884
Example Continued:
For the system given before, calculated the actual voltage at the load centre
assuming that 2500kVA at 4160 is measured at the substation transformer low-
voltage terminals.

Solution:

  ∴ VL = (4160 0 /√3) 1/0.9188 = 2614.2 ∠ 0 V
Recall VL = VS / ar            ; IL = arIS

          IL = arIS = (0.9188)(346.97 ∠-25.84)
             = 318.77 ∠ -25.84 A
Also
∴
   Actual voltage at load centre is:

               = (2614.2 ∠ 0) – (0.3 + j0.9)(318.77 ∠ -25.84)
          VLC = VL – ZLIL

               = 2412.8 ∠ -5.15 V

          VLC 120 = VLC = 2412.8 ∠ -5.15 = 120.6 ∠ -5.15
On a base 120Vbase, load centre voltage is:

∴                    Npt      20
   the +13 tap has produced the result needed.


        VL = 2614.2 ∠ 0 and         IL = 318.77 ∠ -25.84
** Recheck with the previous example for

                           Find V .
Three Phase Step Voltage Regulators
Three 1Φ step-voltage regulators can be
 connected externally to form a 3Φ regulator.
 In this case each regulator has its own
 compensator circuit and can be tapped
 independently.
Normally only one compensator regulator is
 used and the tapping on all 3 phases is
 ganged.
In this case, it is left to the engineer to decide
 the phase to sample.
Wye Connected Regulator (Type B)




       Regulator shown in “Raise” Position
Voltage Equations
       VAN  aRa       0          0  Van 
       V  =  0                                      … (1)
        BN           aRb         0  Vbn 
                                        
       VCN   0
                      0         aRc  Vcn 
                                        
where aRabc = effective turns ratio of the 3 single phase regulators.
Normally aRa = aRb = aRc
We can rewrite (1) in matrix format
      [VLN ABC   ] = [a].[V ] + [b].[ I ]
                         LN abc              abc       … (2)

Also the current equations become:
      1                                       
                              0           0 
 I     a
 A   Ra                                      Ia 
                                                
  0                        1
 I   =
B                                       0  I b  … (3)
                                                
                                                 
                             a Rb              
C                                             
 I
 
      0                                   1  Ic 
                                               
                                                
                               0
      
                                         a Rc 
                                               


OR
      [ I ABC ] = [c].[VLG   abc
                                   ] + [d ][ I ]
                                             abc       … (4)
Where:
                 aRa       0      0 
           [a] =  0
                          aRb     0  
                  0
                           0     a Rc 
                                       
           [b] =[c ] =[0]
                   1                    
                            0       0 
                   a Ra                 
                            1
           [d ] =  0
                  
                                     0 
                                         
                           a Rb
                                    1 
                   0        0           
                  
                                   a Rc 
                                         
For the typical 120 V base regulator with 0.75V / step:
                0.9 ≤ aRabc ≤ 1.1 in 32 steps

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ECNG 3013 D

  • 1. D
  • 2. Distribution Voltage Regulation The voltage at every customer’s service entrance must remain within acceptable tolerances. Common methods of regulating the voltage are: 1. Step- type voltage regulators 2. Load tap changing transformers and 3. Shunt Capacitors.
  • 3. Two Winding Transformer Theory Standard Markings: High Voltage Side: H1, H2 Low Voltage Side: X1, X2 s.t. (a) at no load, Vs is in phase with VL (b) under s.s. load conditions I1 in phase with I2
  • 4. Referring the leakage impedance to the secondary, we have: The total leakage impedance is now given by: Zt = nt2 Z1 + Z2 … (1) where nt = N2/N1 For an ideal transformer: E2 = N2/N1E1 = ntE1 … (2) I1 = N2/N1I2 = ntI2 … (3) Applying KVL to the secondary: E2 = VL + I2Zt … (4) But VS = E1 = 1 E2 = 1 VL + Zt I2 … (5)
  • 5. Equation (5) can be written as: VS = a.VL + b.I2 … (6) where a = 1 and … (7) nt b = Zt … (8) nt Also, IS = Ym.VS + I1 … (9) Sub (3) and (5) into (9) IS = Ym. 1 [ VL + ZtI2 ] + nt.I2 nt IS = Ym VL + [ YmZt + nt ] I2 … (10) nt nt In general form, (10) can be rewritten as IS = c. VL + d. I2 … (11) where c = Ym … (12) nt d = Y .Z + n … (13)
  • 6. We now have a model of a 1Φ transformer as a two port device: i.e.: VS = a.VL + b. I2 … (6) IS = c. VL + d. I2 … (11) where the a, b, c, d constants are: a=1 ; c = Ym nt nt b = Zt ; d = Ym.Zt + nt nt nt If the O/P voltage is needed, then (6) can be rewritten as: VL = 1/a VS – b/a I2 … (14) Sub. for a and b in (14) we get VL = AVS – BI2 … (15) where A = 1/a = nt … (16) ∴ B = b/a = Zt … (17) VL = ntVS – ZtI2
  • 7. Example: A 1Φ transformer is rated 75kVA 2400/240 V. The transformer has the following impedances and shunt admittances: Z1 = (0.612 + j1.2) Ω (HV) Z2 = (0.0061 + j0.0115) Ω (LV) Ym = (1.92x10-4 – j8.52x10-4) s (referred to HV side) Determine the generalized a, b, c, d constants as well as the A and B constants for the transformer. What should be the primary Voltage and Current at rated kVA and 0.9 p.f. lag.
  • 8. Solution: Nt = N2 = 240 = 0.1 N1 2400 Equivalent impedance of transformer referred to L.V. Zt = Z2 + nt2.Z1 = 0.0122 + j0.0235 The generalized constants are: a = 1/nt = 10 ; b = Zt/nt = 0.122 + j0.235 c = Ym/nt = 0.0019 – j0.0085 d = Ym.Zt + nt = 0.1002 – j0.0001 nt A = nt = 0.1 ; B = Zt = 0.0122 + j0.0235 VL = 240 ∠ 0 Assuming that transformer operating at 75kVA, 240 V 0.9 lag (Rated) I2 = 75 x 1000 ∠ -25.84 = 312.5 ∠-25.84 240 VS = aVL + bI2 = 2466.9 ∠ 1.15 V Applying the values of a, b, c and d parameters: IS = cVL + dI2 = 32.67 ∠ -28.75 A
  • 9. Two Winding Auto-Transformer (Buck/ Boost Transformer) • The two winding transformer can be connected as an autotransformer. STEP UP • This is done by connecting X2 to H1 and taking the output from X1H2 for step up. STEP DOWN • Connect X1 to H1 and output is X2H2. • LV winding is referred to as the “series” winding and the HV winding as the “shunt” winding (in relation to the Load).
  • 10. STEP- UP AUTO TRANSFORMER
  • 11. In this case, the total equivalent impedance is referred to the “series” winding. (Boost Transformer) Applying KVL to secondary circuit: E1 + E2 = VL + Zt.I2 … (1) Or E1 + ntE1 = (1 +nt)E1 = VL + Zt.I2 … (2) From the circuit: VS = E1 and I2 = IL … (3) Sub (3) into (2) VS = 1 VL + Zt . I L … (4) 1+nt 1+nt Or VS = a’.VL + b’.IL … (5) where a’ = 1 and b’ = Zt 1+nt 1+nt Applying KCL to node X2 IS = I1 + I2 + Iex … (7) IS = (1+nt)I2 + Iex = (1+nt)I2 + YmVs … (8)
  • 12. Sub (4) into (8) gives:  1 Zt  I S = (1 + nt ).I 2 + Ym  .VL + .I 2  1 + nt 1 + nt  Ym  Ym .Z t  I S= .VL +  + 1 + nt  I 2 … (9) (1 + nt )  1 + nt  But I2 = IL Or IS = c’.VL + d’.IL … (10) where c’ = Ym and d’ = YmZt +1 + nt … (11) (1+nt) (1+nt)
  • 13. Step Down Auto-Transformer (X1 connected to H1) In this case for KVL => E1- E2 = VL + I2Zt
  • 14. If the analysis is continued as before we get; VS = aVL + bIL … (12) IS = cVL + dIL … (13) } where a = 1 b = Zt 1-nt 1-nt (14) c = Ym d = YmZt + 1 –nt ∴ 1-nt 1-nt [ the only difference is the sign of the turns ratio.] ∴ Generalized Constants for Auto-Transformer can be defined as: a= 1 1±nt c = Ym 1±nt b = Zt 1±nt d = YmZt + 1 ± nt 1±nt } (15) From (12) VL = 1/a.VS – b/a.IL ... (16) Or VL = A.VS – BIL where A = 1/a = 1±n ; B = b/a = Z … (17)
  • 15. The generalized equations for the auto- transformer are of exactly the same form as was derived for the two winding transformer as well as for a transmission line. (In terms of a, b, c, d constants). These single phase values will be expanded to a 3x3 matrix for the 3Φ transformer.
  • 16. Rating of Autotransformer The rating is given by: VSIS or VLIL Let: kVAxfm = kVA rating of two winding transformer kVAauto = kVA “ “ autotransformer Vrated1 = E1 = rated source voltage Vrated1 = E2 = rated load voltage Vauto S = rated source voltage of autotransformer Vauto L = rated load voltage autotransformer Neglecting voltage drop across Zt Vauto L = E1 ± E2 = (1 ± nt)E1 … (18)
  • 17. kVAauto = Vauto L . I2 = (1 ± nt)E1I2 … (19) But I1 = ntI2 ∴ kVAauto = (1 ± nt) . E1. I1 … (20) nt But E1I1 = kVAxfm ∴ kVAauto = (1 ± nt) kVAxfm … (21) nt Fundamental Equations for Buck/Boost transformer: (1) Vauto L = (1 ± nt) E1 kVAauto = (1 ± nt) kVAxfm nt where nt = N2 N1 Example: The 75kVA 2400/240V transformer given before is connected as a step-up auto transformer. 1.Determine the kVA rating and voltage output of this arrangement. 2.If the auto transformer is supplying rated kVA at rated voltage at 0.9 lag, determine source voltage and current.
  • 18. nt = 0.1 ; kVAxfm = 75 2400/240 ∴ 1. ∴ kVAauto = ( + 0.1 ) 75 = 825 kVA 1 0.1 V1 = VS = 2400 Vauto L = (1 + n) E1 = (1.1)(2400) = 2640 V = (V1 + V2) = (2400 + 240) = 2640V
  • 19. (2) VL = 2640 ∠0 V I2 = 825 x 103 ∠ -25.84 = 312.5 ∠ -25.84 A 2640 /0 ∴ a = 1/(1+0.1) = 0.9091 b = 0.0122 + j0.0235 = (0.0111 + j0.0214) 1 + 0.1 ∴ c = (1.92 – j8.52) x 10-4 = (1.7364 – j7.7455) x 10-4 1 + 0.1 ∴ [ ] d = (1.92 – j8.52)(0.0122 + j0.0235) x 10-4 + 1 + 0.1 1 + 0.1 = (1.1002 – j0.000005)
  • 20. But VS = aVL + bIL IS = cVL + dIL VS = (a)2560 ∠ 0 + b(312.5 ∠ -25.84) Sub for a, b, c and d we get: = 2406 ∠ 0.1 V IS = (c)(2640 ∠ 0) + d(312.5 ∠ -25.84) = 345.06 ∠ -26.11 Check VL = AV –BIL where A = 1 + nt = 1.1 B = Zt = 0.0111 + j0.0235 VL = (1.1)(2406 ∠ 0.1) – (0.0111 + j0.0235)(312.5 ∠ -25.84) = 2640 ∠ 0
  • 21. Step Voltage Regulators 1. A step voltage regulator consists of an auto transformer and a load tap changing mechanism. 2. Voltage changes obtained by changing taps in series winding. 3. The position of tap controlled by a control unit called the line drop compensator. 4. Regulator has a reversing switch enabling a ± 10% regulating range typically in 32 steps. 5. On a 120V basis this yields 0.75V per step. 6. As per ANSI/IEEE C57-1986 standard there are two types: Type A and Type B. (Type B more common)
  • 22. CONTROL SETTINGS a.Voltage Level -: Voltage to be maintained. b.Bandwidth -: Deadband. If (a) = 122V and Bandwidth = 2V then voltage is between 121-123. c.Time Delay -: Wait time before execution of a tap change. d.Line Drop Compensator -: Used to compensate for Vdrop due to line impedance.
  • 23. TYPE B Step- Voltage Regulator
  • 25. Note: In type B regulator, the core excitation is constant because the shunt winding is connected to the control circuit i.e. the regulated line drop compensator. Diagram gives Regulator in Raise (step up) connection (R). For Lower (L) (step down) the switch is moved to ‘L’. Voltage Equations Current Equations E1 = E2 N1I1 = N2I2 … (1) N1 N2 VS = E1 – E2 IL = IS – I1 … (2) VL = E1 I2 = IS … (3) E2 = N2 E1 = N2 VL I1 = N2 I2 = N2 IS … (4) N1 N1 N1 N1 VS = [1 – N ]V 2 L [ IL = 1 – N2 ]I s … (5) N1 N1 VS = ar . VL where ar = 1 – N2 IL = ar . IS … (6) … (7) ( N1 )
  • 26. When the switch is placed on L (Lower or step down) only equation (2) changes -: VS = E1 + E2 ; IL = IS + I1 This again gives equation (6) but in this case a r = 1 + N2 … (8) N1 If N2/N1 is not known but we know the tap change is 0.75V. ∴Effective regulator ratio for type B regulator: On 120V ; 0.75V = 0.00625 p.u. ∴ effective ratio = ar = 1 ± (0.00625)(# tap) … (9) where: - = raise + = lower
  • 27. Generalized Constants (a, b, c, d) For Type A and Type B regulators we have: Type A: VS = 1 VL ; IS = arIL ar Type B: VS = arVL ; IS = 1 IL ar Effective ratio } with Type A Type B For equation raise + - (9) lower - +
  • 28. ∴Generalized Constants for 1Φ step-voltage regulator are: Type A: a = 1/ar b=0 c=0 d = ar … (10) Type B: a = ar b=0 c=0 d = 1/ ar … (11) where ar is given by (9) with sign given by table before.
  • 29. Line Drop Compensator The changing of the taps on a regulator is controlled by the line drop compensator. Line Drop Compensator
  • 30. a) The current transformer ratio is specified as CTp:CTs where the primary rating (CTp) is typically the rated current for the circuit (or feeder). b) The compensator is an analog circuit i.e. it is a scale model (R’ + jX’) of the line impedance (RL + jXL). (R’ + jX’ -: scale model; replica impedance; analog of the line) c) R’ + jX’ is calibrated in volts d) ZL pu = Zcomp pu
  • 31. Table of Base Values Base Line Cct Compensator Cct Voltage VLN VLN/Npt Current CTp CTs Zbase VLN/CTp VLN/( Npt . CTs) From this we can derive R’ & X’ (Compensator) Rpu + jXpu = RL + jXL Zbline ∴ R + jX = (R + jX ) CT … (1) pu pu L L p VLN For the compensator to function, ZL pu = Zcomp pu. ∴ (Rcomp + jXcomp)Ω = (Rpu + jXpu)Zbase comp ∴ (Rcomp + jXcomp)Ω = (RL + jXL) CTp . VLN VLN (Npt . CTs) Or (Rcomp + jXcomp)Ω = (RL + jXL) CTp . 1 … (2)
  • 32. Equation (2) gives the ohmic value of the compensator. To obtain the R and X settings in Volt we multiply the ohmic value by the rated current: (R’ + jX’) volt = (Rcomp + jXcomp). CTs (R’ + jX’) volt = (RL + jXL) CTp. CTs Npt. CTs ∴ (R’ + jX’) volt = (R + jX ) CT volt … (3) L L p Npt Example: For the compensator circuit given before, the regulator (transformer) rated 5000kVA, 115 delta- 4.16kV grounded wye and the equivalent line impedance from the Regulator to the load centre is (0.3 + j0.9)Ω. a) Determine the VT and CT ratings for the compensator cct. b) Determine the R and X setting of the compensator in Ω and volts.
  • 33. Solution: a) VLG = 4160/ √3 = 2401.8 V. For a 120V compensator operation (Normal voltage) Npt = 2401.8 ≈ 20 120 Rated current of Regulator = 5000 = 693.9 A √3. x 4.16 ∴ Select primary rating of CT as 700A Assuming compensator secondary = 5A  CT = CTp = 700 = 140 CTs 5 b) (R’ + jX’) volts = (RL + jXL) CTp Npt = (0.3 + j0.9) 700 /20 = (10.5 + j31.5) V The R and X setting in Ω is obtained by dividing the volt settings by CTs (current rating) (RΩ +jXΩ) compensator = (10.5 + j31.5)/5 = (2.1 + j6.3) Ω Remember that the compensator is set in volts i.e. at (10.5 + j31.5) V.
  • 34. Example: Assume the regulator is supplying 2500kVA at 4.16kV, 0.9 p.f. lag. If the voltage level at the load centre is to be 120V of bandwidth 2V, determine the tap setting of the regulator. Solution: As calculated before: Setting of regulator = R’ + jX’ = (10.5 + j31.5) V ∴ IL = 2500 ∠ -25.84 = 346.97 ∠-25.84 A VL = 120 ± 1 ∴ Icomp = 346.97 ∠ θ = 2.4783 ∠ -25.84 A √3 x 4.16 Input voltage to regulator = 4160 ∠ 0 = 120.09 ∠ 0 140 √3 x 20 Vdrop = (2.1 + j6.3)(2.4783 ∠-25.84) = 16.458 ∠ 45.72 V Voltage drop in compensator cct = (Zcomp)Ω (Icomp). ∴ VR = Vreg – Vdrop = (120.09 ∠ 0) – (Vdrop) Voltage across compensator relay = VR ∴
  • 35. NB: VR represents the voltage expected at the load centre due to the voltage drop across the line (RL + jXL) The min. value for this voltage should be 119V. ∴ the regulator has to raise Taps. Recall for a typical regulator, on tap ≡ 0.75V ∴ # of taps required = 119 – 109.24 = 13.02 0.75 ∴ for a Type B regulator in raise position the effective ratio is: ar = 1 - (0.00625)(# of taps) = 1 – (0.00625)(13) (for Type B “raise”) = 0.9188 ∴ the generalized constants for modeling this regulator for this operating condition are: a = ar = 0.9188 c=0 b=0 d = 1/ar = 1.0884
  • 36. Example Continued: For the system given before, calculated the actual voltage at the load centre assuming that 2500kVA at 4160 is measured at the substation transformer low- voltage terminals. Solution: ∴ VL = (4160 0 /√3) 1/0.9188 = 2614.2 ∠ 0 V Recall VL = VS / ar ; IL = arIS IL = arIS = (0.9188)(346.97 ∠-25.84) = 318.77 ∠ -25.84 A Also ∴ Actual voltage at load centre is: = (2614.2 ∠ 0) – (0.3 + j0.9)(318.77 ∠ -25.84) VLC = VL – ZLIL = 2412.8 ∠ -5.15 V VLC 120 = VLC = 2412.8 ∠ -5.15 = 120.6 ∠ -5.15 On a base 120Vbase, load centre voltage is: ∴ Npt 20 the +13 tap has produced the result needed. VL = 2614.2 ∠ 0 and IL = 318.77 ∠ -25.84 ** Recheck with the previous example for Find V .
  • 37. Three Phase Step Voltage Regulators Three 1Φ step-voltage regulators can be connected externally to form a 3Φ regulator.  In this case each regulator has its own compensator circuit and can be tapped independently. Normally only one compensator regulator is used and the tapping on all 3 phases is ganged. In this case, it is left to the engineer to decide the phase to sample.
  • 38. Wye Connected Regulator (Type B) Regulator shown in “Raise” Position
  • 39. Voltage Equations VAN  aRa 0 0  Van  V  =  0 … (1)  BN   aRb 0  Vbn    VCN   0    0 aRc  Vcn    where aRabc = effective turns ratio of the 3 single phase regulators. Normally aRa = aRb = aRc We can rewrite (1) in matrix format [VLN ABC ] = [a].[V ] + [b].[ I ] LN abc abc … (2) Also the current equations become: 1   0 0  I a  A   Ra  Ia     0 1 I = B   0  I b  … (3)    a Rb  C     I   0 1  Ic    0   a Rc   OR [ I ABC ] = [c].[VLG abc ] + [d ][ I ] abc … (4)
  • 40. Where: aRa 0 0  [a] =  0  aRb 0    0  0 a Rc   [b] =[c ] =[0]  1   0 0   a Ra  1 [d ] =  0  0   a Rb  1   0 0    a Rc   For the typical 120 V base regulator with 0.75V / step: 0.9 ≤ aRabc ≤ 1.1 in 32 steps