Method for measuring the resistance and the inductance of a line

Abstract

The method described here makes it possible to determine the impedance of a line (1) by measuring the voltage (u) applied across the line and the time derivative of the current (i) flowing through the line. The measured values of the differentiated current are not integrated in this case, but rather are substituted directly, together with the measured voltage values, into an equation system from which the values of the inductance (L) and the resistance (R) of the line (1) can be estimated. In this way, integration of the values of the differentiated current is obviated.

Description

FIELD OF THE INVENTION

[0001] The invention relates to a method for measuring the resistance and the inductance of a line according to the preamble of claim 1. Such methods are used e.g. for short circuit detection in electricity supply lines.

BACKGROUND OF THE INVENTION

[0002] In order to measure the impedance and, in particular, the resistance and the inductance of a line, the current flowing in it and the voltage applied across it are generally measured in a time-resolved fashion and converted into the required values by computation. For the measurement of currents, especially in the case of electrical power lines, use has also recently been made of a Rogowski coil, i.e. a coil that extends around the line carrying the current and measures the derivative of the current with respect to time. In order to find the current, this derivative needs to be integrated with respect to time. This necessitates additional numerical calculation and can lead to inaccuracies (clipping effects, phase offset).

SUMMARY OF THE INVENTION

[0003] It is therefore an object of the invention to provide a method of the type mentioned in the introduction, which gives a maximally accurate and simple way of measuring the inductance and the resistance.

[0004] This object is achieved by the method as claimed in claim 1. Instead of integrating the values from the Rogowski coil, the measured values are hence substituted directly into an equation system that delivers the desired results.

[0005] Preferably, a sizeable number of measurements are used, so that the equation system is over-determined. The resistance and the inductance can then be found by adjustment computation. The method of least squares is preferably employed, which can be done by means of simple matrix inversion or recursively.

BRIEF DESCRIPTION OF THE DRAWING

[0006] Further configurations, advantages and applications of the invention are contained in the dependent claims and from the following description with reference to FIG. 1. The figure shows an equivalent circuit diagram of a line to be measured.

[0007] FIG. 1 shows the equivalent circuit diagram of a line 1 with a resistance R and inductance L. It may, for example, be an electrical power line that is short-circuited at a point 2.

[0008] In order to measure the voltage u(t) across the line 1, a voltmeter 3 is provided. It may, for example, be an electro-optical voltage transformer that is capable of reproducing the value of the voltage u(t) directly (possibly to within a known calibration constant). In order to measure the current i(t) in the line 1, a current differential meter 4 is used. This comprises a Rogowski coil 5, which produces a voltage proportional to the time derivative ∂/∂t of i(t). Accordingly, the current differential meter 4 produces measurements that correspond (to within a known calibration constant) to the value ∂i(t)/∂t.

[0009] The meters 3, 4 are operated at a sampling rate ƒA=1/TA and deliver a series of voltage values u0, u1, . . . and a series of values l0, l1, . . . lN of the differentiated current, with uk=u(kTA) and lk=∂l/∂t|t=kTA. The resistance R and the inductance L are to be determined from these values.

[0010] For the voltage u(t), the following applies: 1$\begin{array}{cc}u\left(t\right)=R·i\left(t\right)+L·\frac{\partial }{\partial t}i\left(t\right)& \left(1\right)\end{array}$

[0011] Using the Rogowski coil, the time derivative of the current i(t) is measured, i.e. the quantity 2$\begin{array}{cc}i\left(t\right)=\frac{\partial }{\partial t}i\left(t\right)& \left(2\right)\end{array}$

[0012] The current i(t) can be calculated by integrating (2). Substitution into (1) hence leads to:

u (t)=R·∫l(τ)dτ+L·i(t)  (3)

[0013] Equation (3) can be converted into a discretized form. Preferably, the Laplace transform u(p) is formed, and a bilinear transformation p=A·(z−1)/(z+1), where A takes the value A≅2/TA in the case of the Tustin (bilinear) approximation. A can more accurately be described as 3$\begin{array}{cc}A={\omega }_0·\cot \left(\frac{{\omega }_0}{2}·\frac{T_A}{2}\right),& \text{(3a)}\end{array}$

[0014] where ω0 is the frequency at which the digital approximation is to agree with the analog values. When formula (3a) is used instead of A=2/TA, the approximation by the digital model agrees accurately with the analog model at the angular frequency ω0. In practice, w0=2πƒN is selected, where ƒN is the mains frequency of the voltage along the line to be surveyed.

[0015] Discretization of Equation (3) approximately leads to:

u n =u n−1 +α0·ln+α1·ln−1  (4)

[0016] where un and un−1 are two successively sampled voltage values and ln and ln−1 are two successively sampled values of the differentiated current. The parameters α0 and α1 are given by 4$\begin{array}{cc}{\alpha }_0=\frac{R}{A}+L{\alpha }_1=\frac{R}{A}-L& \left(5\right)\end{array}$

[0017] Equation (4) provides a basis for finding the required values R and L, or the parameters α0 and α1. To that end, N measurements of the voltage {u1, u2, . . . uN} and of the differentiated current {l1, l2, . . . lN}, with N≧3, are needed in order to set up, from (4), an equation system with N−1 equations for a0 and a1, so that the parameters can be calculated. This procedure has the advantage that direct integration of Equation (3) can be circumvented.

[0018] From the parameters α0 and α1, the resistance R and the inductance L can then be determined from 5$\begin{array}{cc}R=A·\frac{\left({\alpha }_0+{\alpha }_1\right)}{2}L=\frac{{\alpha }_0-{\alpha }_1}{2}& \left(6\right)\end{array}$

[0019] Preferably, N>3, i.e. more than two equations are set up, so that over-determination of the equation system is obtained. The parameter values can, in this case, be determined with high accuracy by means of adjustment computation.

[0020] For example, the parameters α0 and α1, can be determined by applying the method of least squares to the linear equations (4) for n=1. . . N, which in vector notation leads to the following solution: 6$\begin{array}{cc}\Theta =\left(\begin{array}{c}{\alpha }_0\\ {\alpha }_1\end{array}\right)={\left[\sum _{n=1}^N{m}_n{m}_n^T\right]}^{-1}·\sum _{n=1}^N{m}_n{y}_n\mathrm{with}{m}_n=\left(\begin{array}{c}{i}_n\\ i_{n-1}\end{array}\right)& \left(7\right)\end{array}$

[0021] and yn=(un−un−1)

[0022] In this, the first multiplicand on the right-hand side of Equation (7) is the inverse of a 2×2 matrix produced from the values lk of the differentiated current, while the second multiplicand is a sum of vectors comprising the values lk of the differentiated current weighted with differences between consecutive voltage values uk.

[0023] The equation system (4) can also be solved by means of recursive parameter estimation methods or Kalman filters. An iterative method may, e.g. for each vector pair mn, yn, calculate a new approximation Θn for the parameter vector Θ from the preceding approximation Θn−1, by means of the recursion formula

K=P n−1 ·m n ·(λ+mnT·Pn−1·mn)−1

Θn=Θn−1+K·(yn−mnT·Θn−1)

[0024] 7 $$ K = P n - 1 · m n · ( λ + m n T · P n - 1 · m n ) - 1 Θ n = Θ n - 1 + K · ( y n - m n T · Θ n - 1 ) P n = ( E - K · m n T ) ⁢ P n - 1 λ ( 8 )

[0025] In this, E is the unit matrix, λ is a weighting factor between 0.8 and 0.9 and Pn is the so-called precision matrix (start value e.g. 103·E or 105·E). K is referred to as a correction factor.

[0026] List of references

[0027] 1 : line

[0028] 2 : short circuit point

[0029] 3 : voltmeter

[0030] 4 : current differential meter

[0031] 5 : Rogowski coil

[0032] A: factor

[0033] E: unit matrix

[0034] ƒA: sampling rate

[0035] i(t): time-varying current

[0036] K: correction factor

[0037] L: inductance

[0038] N: number of measurements within the observation window

[0039] R: resistance

[0040] TA: time interval between measurements

[0041] u(t): voltage

[0042] uk: voltage values

[0043] l(t): time-differentiated current

[0044] lk: values of the time-differentiated current

[0045] α0, α1: parameter values

[0046] λ: weighting factor

[0047] Θ: parameter vector

Claims

1. A method for measuring the resistance R and the inductance L of a line, in which a voltage u across the line and a time derivative i of the current through the line are measured at a rate 1/TA in order to obtain a series of N voltage values u0, u1, . . . uN and a series of N values i0, i1, . . . iN of the differentiated current, [characterized in that] wherein N≧3 and the voltage values and the values of the differentiated current are substituted into an equation system with N−1 equations of the form

2. The method as claimed in claim 1, [characterized in that] wherein N≧3, and [in that] wherein the resistance R and the inductance L are found by adjustment computation.

3. The method as claimed in claim 2, [characterized in that] wherein the resistance R and the inductance L are found by solving

4. The method as claimed in [one of claims 1-3] claim 1, [characterized in that] wherein the equation system is solved iteratively by calculating, for a plurality of n, an approximation Θn for

5. The method as claimed in [one of the preceding claims] claim 1, [characterized in that] wherein the first derivative of the current is measured using a Rogowski coil.

6. The method as claimed in [one of the preceding claims] claim 1, [characterized in that] wherein A=2/TA.

7. The method as claimed in [one of claims 1-5] claim 1, [characterized in that] wherein

8. The use of the method as claimed in [one of the preceding claims] claim 1 for measuring the impedance of an electrical power line.