comparison booster transformer

81
EMC York 2004 July 1 & 2, 2004 Prof. György Varju e-mail: [email protected] Budapest University of Technology & Economics Comparison of the booster transformer and auto transformer railway feeding systems, Feeding features and induction to telecom lines

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Page 1: Comparison Booster Transformer

EMC York 2004July 1 & 2, 2004

Prof. György Varjue-mail: [email protected]

Budapest University of Technology & Economics

Comparison of the booster transformer and auto transformer railway feeding systems,

Feeding features and induction to telecom lines

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2

Presentation items:

1. Railway feeding voltages and recent alterations of the feeding systems in Europe

2. Qualitative analyses of the ac. feeding systems

3. Modeling and parameters of railway feeding systems

4. Systems comparison

5. Conclusions

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3

1. Railway feeding voltages and recent alterations of the feeding systems in Europe

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4Feeding voltages

in Europe

3000 V dc.1500 V dc.50 Hz 25 kV ac.16 2/3 Hz 16 kV ac.

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5

Recent alterations in feeding systems

• dc. feeding replaced by ac. 50 Hz, 25kV or 2x25 kV– for high speed train (e.g. TGV)– for high density traffic (e.g. Netherlands)

• BT system replaced by AT– for heavy freight train traffic (e.g. Sweden

iron ore transport) – for high speed train

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6

2. Qualitative analyses of the ac. feeding systems

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7

Feeding systems of ac. supply

Simple feeding with rail (+ earth) return: RR

Booster transformer with rail return: BTRR

Booster transformer with return conductor: BTRC

Auto transformer: AT

Combined systems: AT/BTRR

AT/BTRC; ATPF/BTRC; ATPF/SCBT

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8Simple feeding with rail (+ earth) return:

RR system

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9Simple feeding with rail (+ earth) return: RR system

Quantities characterizing the current portion & profiles

Series impedance of the return rail(s)-to-earth loop, as per unit length values:

o ZRR, series impedance of the return rail(s)-to-earth loop,

o ZCR, mutual impedance between the contact line system and return rail system with common earth return,

o GRR the rail-to-earth leakage conductance,

Page 10: Comparison Booster Transformer

10Simple feeding with rail (+ earth) return:

RR systemQuantities characterizing the current portion & profiles

Derived quantities: • rail current portion and screening factor behind the end/effect zones:

Rail current portion: Screening factor

RR

CR

ZZq −=

RR

CR

ZZqk −=+= 11

• length constant of the rail-earth circuit with the approximation, that ωLRR >> RRR:

RRRRGLωατ 21 ≈=

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11Simple feeding with rail (+ earth) return: RR system

Rail current and point screening factorat 50 Hz supply

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12Simple feeding with rail (+ earth) return: RR system

Rail current and point screening factorat 16 2/3 Hz supply

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13

Booster transformer system with rail return: BTRR system

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14Booster transformer system with return conductor:

BTRC system

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15

Booster transformer system with return conductor: BTRC system

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16

Continuity of the current return path BTRC system

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17Auto transformer system

AT (with 2U power source)

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18Auto transformer system :

AT (with 1U power source)

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19Auto transformer system

with increased NF voltageAT [16/25 kV]

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20Auto transformer system

with increased PF and NF voltages:ATPF [16/2x25 kV]

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21Combined feeding system

AT / BTRR

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22Combined feeding system

AT / BTRC

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23Combined feeding systemATPF / BTRC

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24Combined feeding system

ATPF and shunt connected BTATPF / SCBT

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25

3. Modeling and parameters of railway feeding systems

• Multiconductor line representation

• Representation by two phase sequence networks

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26

Multiconductor line representation of railway feeding (AT) system

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27Two phase sequence network representation

BTRC system

Zm ZmZm

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28Two phase sequence network representation

AT system

Ztm Ztm Ztm

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29Two phase symmetrical componentsbasic voltage & current expressions

Phase quantities Symmetrical components:

U U UC = +0 1 ( )PC UUU +=21

0 Voltages:

10 UUU P −= U U UC P112

= −( )

Note: UCP = 2U1

10 IIIC += ( )PC III +=21

0

Currents

10 IIIP −= ( )PC III −=21

1

Notes: current in the balanced loop: IC = -IP = I1

current in the return path (rail+earth): Ireturn = IC + IP = 2 I0

Page 30: Comparison Booster Transformer

30Two phase symmetrical component representation of two coupled lops

Coupled loop circuit Equivalent of the coupled loop

Positive sequence loop Zero sequence loop

CPself ZZZ −=0 CPself ZZZ +=0

( )PPCCself ZZZ +=21

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31Representation of the network elements

Line configuration (Rsi – Svv line)

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32Representation of the network elements

Multiconductor line parametersDistributed series and shunt elements

of the railway line model

Ic(x) ZCC

IR(x) ZRR

IP(x) ZPP

ZCR

ZRP

C

R

P

ZCP

UP(x)

UR(x)

UC(x)

R

C P

CP0

CCP

CCR CRP

CC0GR0 CR0

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33Representation of the network elements

Line system

Multi-conductor network Sequence networks

positive sequence

zero sequence

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34Representation of the network elements

Power supply (converter or transformer station)

Multi-conductor network Sequence networks

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35Representation of the network elements

Traction unit (engine, motor coach)Multi-conductor network Sequence networks

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36View of auto & booster transformers

(Installed at the Kiruna – Råtsi – Svappavaara line in Sweden)

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37

Representation of the network elementsBooster transformer: detailed circuit diagram

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38Representation of the network elements

Booster transformer: magnetizing impedance

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39Representation of the network elements

Booster transformer: simplified circuit diagram

Multi-conductor network Sequence networks

Zm

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40Representation of the network elements

Bond (between RC and RR)

Multi-conductor network Sequence networks

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41Representation of the network elements

Auto transformer: magnetizing impedance neglected

Multi-conductor network Sequence networks

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42

S tudy item s: a) Equivalent im pedance, voltage stability b) System losses c) Power rating of auto transform ers d) Induction effect:

o Inducing earth current profiles o Length-current integrals o Induced longitudina l em f

e) Rail-to-earth potentia l f) Rail-to-ra il potentia l

4. Systems comparison

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43

a) Equivalent impedance, voltage stability

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44Equivalent impedance

vs. train position (spacing 6 km)

BTRR BTRC

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45

Equivalent impedance vs. train positionAT system (spacing 12 km)

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46Comparison of impedances vs. train pos.

for BTRC & AT systems

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47Equivalent impedance vs. train position

AT systems

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48Comparison of voltage drop for AT and BT systems

(Traction power 8 MVA)

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49Comparison of normalized values of

the equivalent impedances forBTRR, BRRC & AT systems

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50Voltage drop, versus train location

for different AT supply options

2U

3U

0

2

4

6

8

10

12

14

16

0 5 10 15 20 25 30 35 40train position, km

∆U[%]

5AT4AT3AT

Train load: 10 MW, cosϕ = 0.8

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51

d) Characterization of the induction effect

o Inducing earth current profiles

o Current-length integrals

o Induced longitudinal emf

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52

Inducing earth current profilesCases studied for demonstration

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53Earth current profiles at different train locationsBTRR system

Spacing: 6 km, G=0.25 S/km, Train current: 500A

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54Earth current profiles at different train locationsBTRC system

Spacing: 6 km, G=0.25 S/km, Train current: 500A

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55Earth current profiles at different train locations

AT systemSpacing: 12 km, G=0.25 S/km, Train current: 500A

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563D surface of the inducing current

BT system

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3D surface of the inducing current BT system

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58

Current-length integralsCalculation principle of the current-length integral

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59

Maximum of the the current-length integralAT system

Integration window: 6 km Integration window: 42 km

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60Maximum of the normalized current-length integrals,

base the current-length integral of the BT systemAT system

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61Current-length integrals for different

feeding systemsParameter: rail-to earth leakage, G

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62Average inducing current for different

feeding systemsParameter: rail-to earth leakage, G

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63

Induced longitudinal emf

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64Map of the measured line(Kiruna – Råtsi – Svappavaara)

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65

C - R short circuit locations, for 16 2/3 Hz measurements

BT system

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66C - R short circuit locations,for 16 2/3 Hz measurements

AT system

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67

Longitudinal voltage measurementsSections of telecommunication cable

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68Induced longitudinal voltage vs. train location

in total cable sectionAT system

0

20

40

60

80

100

120

1.32

9

4.31

4

7.12

8

10.3

30

12.2

22

15.1

74

17.4

23

20.4

12

22.5

72

25.4

90

28.8

10

32.4

24

36.5

00

km

V

calculated G=0.5 S/km

calculated G=0.24 w S/km

measured

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69Induced longitudinal voltage vs. train location

Comparison of BT and AT systemsMeasured cable sections: total

0

20

40

60

80

100

120

1.32

9

2.63

1

5.78

8

7.12

9

10.1

8

11.2

82

12.2

23

15.1

74

17.4

23

19.2

32

21.4

92

23.8

24

25.4

90

28.8

10

30.3

35

34.3

08

36.6

00

k

V AT

BT

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70

e) Rail-to-earth potential

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71Real-to-earth voltage profile vs. length

BTRR systemTrain at 9.01 km

(BT location)Train at 41.99 km

(at the middle of BT spacing)

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72

Maximum rail-to-earth voltages vs. train positionBTRR system, spacing 6 km

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73Real-to-earth voltage profile vs. length

BTRC systemTrain at 2.99 km

(BT location)Train at 39.01 km

(at the middle of BT spacing)

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74

Maximum rail-to-earth voltages vs. train positionBTRC system, spacing 6 km

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75

Real-to-earth voltage profile vs. lengthAT system

Train at 17.90 km(middle of an AT spacing)

Train at 24.01 km(AT location)

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76

Maximum rail-to-earth voltages vs. train positionAT system, spacing 12 km

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77Maximum rail-to-earth voltages for

different feeding systems

BT spacing 3 km BT spacing 6 km

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78

Conclusions

The results of simulation calculations and site experiences

a) The equivalent impedance is significantly (about 3 times) less for the AT

system than that for the BT system. b) Induction to telecommunication lines:

• the BT and AT systems are, practically, identical. • the maximum longitudinal voltage occurred in the whole line length

with the current injection at the Svv end • the induction effect could significantly be reduced by the improvement

of the balance ◊ for BT system balancing the mutual impedances of the catenery

system and the return conductor to rail ◊ for AT system balancing the self impedances of the catenery system

and the inverted feeder

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79

Conclusionscont.

c) The rail potentials in personnel safety point of view, they are also similar in AT and BT supply systems with the following remark:

• in case of AT supply the rail-to-earth voltage can reach higher value in the relatively big AT spacing

• in case of BT supply, the voltages over insulated joints are higher in certain places.

d) Both the induction effect and the rail potential are significantly affected by: • spacing of BT or AT • rail-to-earth leakage conductance, G

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80

Conclusionscont.

Proposals for further study

(1) The feasibility of the use of positive feeder.

(2) The feasibility of the combined feeding systems.

(3) Methods for balancing the AT feeding by: • optimised negative feeder arrangement • use of current unbalance suppression unit (CUS).

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81

Thank you for your attention

?