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Open Physics

formerly Central European Journal of Physics

Editor-in-Chief: Seidel, Sally

Managing Editor: Lesna-Szreter, Paulina

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Volume 16, Issue 1

Issues

Volume 13 (2015)

Multivariable polynomial fitting of controlled single-phase nonlinear load of input current total harmonic distortion

Roman Sikora / Przemysław Markiewicz
  • Corresponding author
  • Lodz University of Technology, Institute of Power Engineering, Łódź, Poland
  • Other articles by this author:
  • De Gruyter OnlineGoogle Scholar
/ Wiesława Pabjańczyk
Published Online: 2018-04-18 | DOI: https://doi.org/10.1515/phys-2018-0021

Abstract

The power systems usually include a number of nonlinear receivers. Nonlinear receivers are the source of disturbances generated to the power system in the form of higher harmonics. The level of these disturbances describes the total harmonic distortion coefficient THD. Its value depends on many factors. One of them are the deformation and change in RMS value of supply voltage. A modern LED luminaire is a nonlinear receiver as well. The paper presents the results of the analysis of the influence of change in RMS value of supply voltage and the level of dimming of the tested luminaire on the value of the current THD. The analysis was made using a mathematical model based on multivariable polynomial fitting.

Keywords: curve fitting; total harmonics distortion; single-phase nonlinear loads; LED luminaire

PACS: 88.05.-b; 88.05.Tg

1 Introduction

Nonlinear receivers are the source of many negative phenomena occurring in the power system. They receive the distorted currents from the power system which, when flowing by the power systems elements, result in voltage drops caused by higher harmonics of current. Consequently, this causes distortion of the supply voltage. The distorted current causes increased heating of wires and other power systems elements, as well as insulation aging, increased power losses, increased probability of resonance, and many more. In three-phase systems, another problem concern the occurrence of current in neutral conductor.

Nowadays, more devices are equipped with SMPS power supplies. Such devices are receivers with nonlinear current-voltage characteristics e.g. LED luminaires that are equipped with SMPS power supplies. Modern luminaire solutions allow to control of the luminous flux. This is accomplished by controlling the current or output voltage of the power supply. Usually, most of power supplies are equipped with PFC systems which are used to improve the power factor. They are generally designed for increasing the rated power of the power supply. In the case of power supplies, the influence of the level of control on the generated disturbances is observed. With the decrease of the dimming level of control gear, THD coefficient of the current increases and the power factor decreases. In addition, the THDI is influenced by a number of factors: the power supply design and algorithm, the level of the supply voltage distortion and its RMS value, the control level.

The voltage and current THD coefficients are described by (1) and (2).

THDU=UHU1=UU121(1)

THDI=IHI1=II121(2)

According to standard [23] for steady-state and non-sinusoidal currents and voltages, the RMS values of voltage U and current I have two components:

U2=U02+UH2(3)

I2=I02+IH2(4)

A component with a lower index 0 denotes a constant component. For other components, the index is the actual harmonic or voltage number.

UH2=U02+H1UH2=U2U12(5)

IH2=I02+H1IH2=I2I12(6)

A new problem with the generation of harmonics is the fact that increasingly responsible for this phenomenon are the receivers with low power although present in large quantities. In particular, it concerns adjustable light sources and luminaires dimmed light sources and luminaires.

Many analytical methods are used to evaluate this effect. One method uses a simplified schematic diagram of a nonlinear load described by time differential equations based on the knowledge of basic electrical laws [1]. Another method include replacing the nonlinear receiver with a nonlinear resistance [4]. In the literature [12, 17, 19], a method of creating a mathematical model of a nonlinear equipment based on measurements is presented. It is based on accepting the input and output quantities which characterize the given nonlinear equipment in the studied phenomena. The method described was used to assess the impact of computer power supplies on the quality of electricity in the mains [12, 14, 17, 18, 20].

As a tested object the LED luminaire with controlled power and light flux was selected. For the analysis, the methods described in [6, 7, 8] using the measurement results of a real object were used. Using these methods a mathematical model was developed. Input values of the model are the RMS value of the supply voltage and the control level. The output value of the model is the value of the THDI. Mathematical model is a n-th degree polynomial of two input variables. The model was developed using the Curve Fitting Toolbox available in MATLAB.

2 Laboratory results

LED luminaire equipped with power supply with analogue control input made of standard 1 - 10V has been subjected to the laboratory tests. This luminaire has rated power equal to 32W. The RMS value of the supply voltage was varied in the range 230V ± 10% (from 207 to 253 V). The limits of voltage variations aredescribed in EN 50160 [21] for acceptable voltage changes in low voltage networks. The second input values was the input control level of the luminaire, determined by the value of the control voltage from 1V to 10V, with a step equal to 1 volt. The output value was the value of the THDI coefficient. Measurements were made using the FLUKE 1760 which is anelectrical power quality analyzer. The laboratory power supply as a source of DC control voltage was used.

Figure 1 shows the relation of the power of the lighting fitting as a function of the control voltage UC and of the supply voltage US. When analyzing its waveform, it can be seen that in the range of UC voltage from 1V to 8V the dependency is linear. In the range of 8V to 10V it can be assumed that the luminaire is working at full power. Table 1 summarizes the results of the measurement of the power of the luminaire P as a function of the control voltage UC. For the tested luminaire, 1V of control voltage ofthe luminaire is achievedat 19.32% of the rated power. This corresponds to the lower limit of regulation, at which the luminaire achieves a minimum power of 6.28W.

Relation of the power of the lighting fixture P as a function of the supply voltage US and control voltage UC
Figure 1

Relation of the power of the lighting fixture P as a function of the supply voltage US and control voltage UC

Table 1

Relation between the luminaire power P and control voltage Uc

In Figure 2 the relationship between the THDI of the US supply voltage and the UC control voltage is presented. Figure 2 shows two different areas of variation. For control voltages greater than approx. 5V, the THDI value of the supply current varies in a small range. In the control voltage range of 1V to 5V, the THDI coefficient shows a strong upward trend.


Relation of THDI coefficient as a function of supply voltage US and control voltage UC
Figure 2

Relation of THDI coefficient as a function of supply voltage US and control voltage UC

The presented dependence is characteristic for the tested luminaire. Other types of luminaires with control systems may had different dependencies whilethe general nature of the dependency changes are similar.

For the illuminated luminaire, the characteristics of the THDI coefficient are described by two polynomials according to (7):

THDI=THDI15UC,USUC1;5US207;253THDI510UC,USUC5;10US207;253(7)

Polynomials THDI–15 and THDI–510 are presented as the sum of the product of the supply voltage US, the control voltage UC and the coefficients aij and bij (8) (9), respectively:

THDI15UC,US=i=0mj=0maijUCiUSj(8)

THDI510UC,US=i=0mj=0mbijUCiUSj(9)

The coefficients aij and bij can be written in matrix form as A and B (4):

A=a00a01a02a03a04a05a10a11a12a13a140a20a21a22a2300a30a31a32000a40a410000000000m×mB=b00b01b02b03b04b05b10b11b12b13b140b20b21b22b2300b30b31b32000b40b410000b5000000m×m(10)

For the study, the luminaire coefficients aij and bij take the following values.

A=5.9091051.306104115.400.50980.0011279.97107179263.240.68360.36714.2221060123520.340.099580.00015270083.910.36710.00013710006.3220.025640000000000B=1.63910536.3632.170.1420.00031272.749107136120.320.12160.00031843.284106056.740.32980.0014367.035107004.7820.0010314.3911050000.33670.000614200000.0130400000

The polynomials THDI–15 and THDI–510 from the dependence (1) were obtained using the two-variable polynomial fitting method to the measurement results using the Curve Fitting Toolbox [7]. The proposed tool for data vectors US, UC and THDI have found the vector of polynomial coefficients of the assumed degrees. Polynomial coefficients were selected to obtain a minimum value of the mean square deviation between the given function THDI = f(US, UC), and approximating polynomial THDI–15(US, UC) for US ∈ 〈1;5) and THDI–510(US, UC) for US ∈ 〈5;10〉.

For the obtained approximating polynomials (Figures 3 and 4) the mean square errors were respectively 0.95 and 0.99.

Graph presenting the approximating polynomial THDI–15(US,UC)
Figure 3

Graph presenting the approximating polynomial THDI–15(US,UC)

Graph presenting the approximating polynomial THDI–510(US,UC)
Figure 4

Graph presenting the approximating polynomial THDI–510(US,UC)

Verification of the correctness of the model has been made in order to determine the error values at the calculation points. The calculation results are shown in Figure 5 for the THDI–15 polynomial approximation and Figure 6 for the THDI–510 polynomial.

Graph presenting the polynomial approximation error of THDI–15(US,UC)
Figure 5

Graph presenting the polynomial approximation error of THDI–15(US,UC)

Graph presenting polynomial approximation error of THDI–510(US,UC)
Figure 6

Graph presenting polynomial approximation error of THDI–510(US,UC)

Due to the high nonlinearity according to THDI = f(US, UC) in range of the control voltage from 1V to 5V the error values are within the range of 0.10% to 26.73%.

The maximum error value occurred for UC = 3V and US = 245V. An error graph is shown in Figure 5. Within the control voltage range of 5 to 10V, the maximum error value is 2.52%, as illustrated in Figure 6.

3 Computational example designation of THDI coefficient

The proposed method of estimating the value of THDI of the power supply was used to calculate this factor for the tested luminaire and the assumed daily schedule of its operation. The luminaire works at full power from 16.00 to 23.00 and from 5.00 to 7.00. At night from 23.00 to 5.00 in the morning it is operated at 50% of the rated power. In order to implement the adopted work schedule of luminaire, it is necessary to know the power P depending on the input value UC. This relationship is shown in Figure 7 and it is practically linear. For analytical purposes according to UC = f(P) it may therefore take advantage of the approximation as a linear function.

Graph presenting the approximating polynomial UC(P)
Figure 7

Graph presenting the approximating polynomial UC(P)

The obtained approximation function UC = f(P) is represented by the expression (11) and obtained for the mean square error is equal to 0.9984.

UCP=10forP=1pu8.541P0.4562for0.1932P<1pu(11)

For the further calculations it is assumed that in order to achieve the full power of the luminaire UC = 10V and for the remaining control levels, the UC value is calculated from the relationship (11). The dependence (11) allows to determine the value of the UC control voltage to obtain the assumed power of the luminaire in any schedule of its operation.

The second input value (supply voltage US) was derived from measurements made in an existing lighting installation.

Figure 8 shows the time dependent waveforms of RMS supply voltage from measurements and the THDI values obtained from the calculations. These results correspond to a full daylight cycle with a scheduled power reduction. For the full power of the luminaire, the predicted THDI value 14%. The reduction of the power of the luminaire causes it to increase to a range of 15.5 to 17%. This corresponds to a 19% increase in THDI.

Results of calculations using the model
Figure 8

Results of calculations using the model

4 Conclusions

The problem of the quality of electricity is one of the most important aspects related to the operation of power devices. According to EN 61000-3-2 [21], class C receivers cannot generate harmonic currents exceeding their limit values. One of the indicators of the level of disturbances generated to the power supply in the form of higher harmonic current is the total harmonic distortion factor THDI. On the basis of the measurements it was proved that for the LED luminaire with power regulation its value depends on the level of control and the value of the supply voltage. From an operational point of view, it is important to predict THDI, values under given power conditions at a given level of control.

The applied mathematical model of the nonlinear receiver based on the results of the measurements allows for accurate estimation of the THDI level of the given receiver. The knowledge of the THDI characteristics as a function of changes in the input values allows to determine permissible changes of these values to maintain the current deformation at a given level. For the tested luminaire, this method determined the acceptable range of power regulation and luminous flux. The analysis can be carried out for the assumed range of voltage supply variations, ranging from 230V ± 10% (from 207V to 253V and full range of power P control).

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About the article

Received: 2017-11-02

Accepted: 2017-11-12

Published Online: 2018-04-18


Citation Information: Open Physics, Volume 16, Issue 1, Pages 137–142, ISSN (Online) 2391-5471, DOI: https://doi.org/10.1515/phys-2018-0021.

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© 2018 R. Sikora et al.. This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License. BY-NC-ND 4.0

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