Measurement of the frequency dependent impedance of a

  • Slides: 20
Download presentation
Measurement of the frequency dependent impedance of a thin wire with ground return Magnus

Measurement of the frequency dependent impedance of a thin wire with ground return Magnus Akke 2004 -04 -115 Industriell Elektroteknik och Automation magnus. akke@iea. lth. se

Outline – Introduction – Measurements – Comparison with models – Discussion and conclusion 2

Outline – Introduction – Measurements – Comparison with models – Discussion and conclusion 2

Motivation for measurements • • Relay testing Transient based fault location Insulation coordination Power

Motivation for measurements • • Relay testing Transient based fault location Insulation coordination Power line carrier 3

Decouple 3 -phase line has one ground mode and two aerial modes. Focus on

Decouple 3 -phase line has one ground mode and two aerial modes. Focus on ground mode. 4

Task 1: Measure impedance vs frequency for 1500 meter wire with ground return Task

Task 1: Measure impedance vs frequency for 1500 meter wire with ground return Task 2: Compare with models 1500 m 3 2 Ch. A Ch. B Scope 1 4 5 6 5

What to expect? Quick and dirty, use handbook TEFYMA Approximate inductance with two lines.

What to expect? Quick and dirty, use handbook TEFYMA Approximate inductance with two lines. Return line is the mirror image. Distance between wire and mirror image is 2 m. Resistance from DC-measurement. 6

TEFYMA model – Impedance vs Frequency 7

TEFYMA model – Impedance vs Frequency 7

Measurement setup 1500 m 3 2 Ch. A Ch. B Scope 4 5 6

Measurement setup 1500 m 3 2 Ch. A Ch. B Scope 4 5 6 1 8

Measurement execution 9

Measurement execution 9

Measured and expected result 10

Measured and expected result 10

Transmission line theory References: Hallén, E. , Elektricitetslära, Almqvist & Wiksells, 1953. Claesson, I.

Transmission line theory References: Hallén, E. , Elektricitetslära, Almqvist & Wiksells, 1953. Claesson, I. , et al, Analoga kretsar och signaler, Studentlitteratur, 1993. 11

Transmission line theory cont. Re-write and let Calculation using Laplace gives where 12

Transmission line theory cont. Re-write and let Calculation using Laplace gives where 12

Transmission line with load Line model 13

Transmission line with load Line model 13

Transmission line model with fixed parameters 14

Transmission line model with fixed parameters 14

Frequency dependent parameters • Fixed parameters works well with metallic return, but fails when

Frequency dependent parameters • Fixed parameters works well with metallic return, but fails when ground is used as the current’s return path. • Carson (1926) used Maxwell’s equation to make a line model where the effect of ground losses and current distribution are embedded in frequency dependent line parameters R and L. 15

Model with Carson’s frequency dependent parameters 16

Model with Carson’s frequency dependent parameters 16

Frequency dependence by Carson and ad-hoc grounding model 17

Frequency dependence by Carson and ad-hoc grounding model 17

Discussion • Model with lumped inductance and resistance is only valid at • Transmission

Discussion • Model with lumped inductance and resistance is only valid at • Transmission line model with fixed parameters is insufficient. Results in poor model and inefficient simulation • Carson’s model is reasonable up to 100 k. Hz. 18

Relevance for typical transmission line? Height=15 m, area=500 mm 2, length=300 km, R_flt=5 ohm

Relevance for typical transmission line? Height=15 m, area=500 mm 2, length=300 km, R_flt=5 ohm 19

Conclusion • Theory and measurements are needed to verify and develop models. • Measurement

Conclusion • Theory and measurements are needed to verify and develop models. • Measurement shows un-modeled dynamics. • Further work – High frequency modeling of line – Include dynamics of connection between line and ground, e. g, ground rod or fault – Bounded line length 20