phd thesis abstract - utcluj.roold.utcluj.ro/download/doctorat/rezumat_adina_racasan.pdf ·...
TRANSCRIPT
FACULTY OF ELECTRICAL ENGINEERING
Eng. Nicoleta Adina RĂCĂŞAN
PhD THESIS ABSTRACT
CONTRIBUTIONS TO THE IMPROVEMENT OF THE CONDUCTED ELECTROMAGNETIC INTERFERENCE
FILTERS PERFORMANCES
PhD Evaluation Commission:
PRESIDENT: Prof.dr.eng. Radu CIUPA – Dean, Faculty of Electrical Engineering,
Technical University of Cluj-Napoca
SUPERVISOR: Prof.dr.eng. Călin MUNTEANU – Faculty of Electrical Engineering, Technical University of Cluj-Napoca
MEMBERS: Prof.dr.eng. Daniel IOAN – Faculty of Electrical Engineering, „Politehnica” University of Bucharest
Prof.dr.eng. Mihai IORDACHE – Faculty of Electrical Engineering, „Politehnica” University of Bucharest
Prof.dr.eng. Vasile ŢOPA – Faculty of Electrical Engineering, Technical University of Cluj-Napoca
The PhD Thesis public defense takes place Friday 1st of October 2010 at 1000 on “Aula Domşa”, str. C. Daicoviciu 15, Technical University of Cluj-Napoca
2
Chapter 1, entitled Introduction to EMI Filters, shows the most important elements resulted
from the specialty literature analysis regarding the general topic of the research realized in the PhD
thesis. So, we start from fundamental principles about electromagnetic compatibility pointing out on
the aspects regarding the susceptibility and immunity problems of the perturbations in the electric-
power-supply network. It is outlined the actual standards and limits of electromagnetic emissions
imposed at international level. There are detailed the test methods of the perturbations induced in
the electric-power-supply network, and the fundamental characteristic elements of this signals
respectively. In the second part of the chapter it is presented the actual stage of the research in the
electromagnetic interference filters’ domain, generic named EMI filters. Are presented the
characteristic elements of the filters realized in the classical technology, by discrete components,
outlining the advantages and disadvantages of this technical solution. In the last part of the chapter
it is presented the functional limits of the electronic passive elements that compose the classical
EMI filters emphasizing the mechanism of parasitic effects that appear in these devices.
Concluding, taking account of the actual demands of limiting the perturbation emissions induced in
the electric-power-supply network, the improvement of the EMI filters performances by
introduction of a new implementation technology able to throw away the technological and
performances barriers impose by the used devices in the classical filters represent a research topic
very actual and important on the international plan.
Chapter 2, entitled EMI Filters and the magnetic planar technology, outlines the
fundamental principles that are the base of the magnetic planar technology, being in the same time
succinct overhung the actual study of the research in this domain. Are emphasized the advantages of
the magnetic planar technology with respect to the conventional classic technologies in the
implemenration of some integrate magnetic devices that compose the power electronic converters.
This technology of planar integration can be implemented also in the case of EMI filters, standing
out the fundamental major differences between the functional demands of this HF integrate passive
devices and those of the EMI filters. In the last part of the chapter is underlined the fact that the
behavior key element of the EMI filters – that is a low-pass filter – can be directly implemented
using a LC structure that is magnetic planar integrated. So, the detail study of the behavior of this
fundamental cell in report with the frequency represent a first important step in the light of
understanding the EMI filters behavior in HF planar magnetic technology, and for the improvement
of theirs performances, the next chapter of the thesis being dedicate to this study. This chapter ends
with the presentation of the fundamental principle used to realize an integrate EMI filter with
magnetic planar technology by interconnecting the LC integrate cells, accentuating the
implementation mode of the CM and DM filter components.
3
Chapter 3, entitled Electromagnetic modeling of a LC planar integrate cell, proposes a
modern modeling method in frequency domain of a LC integrate cell. Is stand out the fact that for a
correct functional modeling is adequate the multi-conductor transmission line method generalized
with losses. For a simple structure with two symmetrical conductors, the solution can be convenient
obtained by decompose in even and odd modes. The equivalent circuits with different charge
conditions can be represented by two independent transmission lines series or parallel connected.
For other connections and configurations, the characteristics can be easy determinate using the A
and Z matrixes. The create models stand out the fundamental properties of a LC integrate cell
regarding the behavior of these cells in frequency domain. Therewith, the create numerical models
help to understand the dependence of the frequency characteristics with constitutive
electromagnetic parameters, helping in this way the functional optimization of these structures in
report with the application in which these are used. Last but not least, the create models open the
research topic by modeling with equivalent circuits in the case of planar integrate structures with
very complex geometries. The author contribution in this chapter is the systematization of the
specialty literature in the planar integrated structures modeling domain and the realization of the
response frequency characteristics by analytical and numerical modeling with Mathematica and
PSpice of all the study structures.
Chapter 4, entitled Integrate EMI filters performances improvement by increasing the
losses in the conductors, outlines the author contributions to the integrate EMI filters performances
improvement by increasing the losses in conductors at HF. In this light, for increase the winding
losses at high frequency, is proposed the conductors nickel-plate method. The test of this method
was initially done using a simple model, composed of only two cooper conductors, and then the
technique was extend to more complex structures. This study was realized for common mode
excitation (CM), and for differential mode excitation (DM), each proposed configuration being
tested for a frequency range with values between 100 kHz and 10 MHz, conduction emission
analysis domain.
For the two copper conductors model were analyzed seven types of configurations: pure
cooper conductors, cooper conductors global nickel-plate, cooper conductors partial nickel-plate,
conductors plate with nickel only on above surfaces, and below respectively, conductors plate on
the external surfaces, and cooper conductors plate only on the internal surfaces. Doing this study
result that the bigger losses are obtained for the case of the cooper conductors plate with nickel only
on internal surfaces, for both common and differential mode excitation. For example, at the
frequency of 10 MHz, the losses on the length unit are 2 Ω/m in the case of pure copper conductors
and for the case of the conductors plate with nickel on the external surfaces are 57 Ω/m, and in the
case of the conductors plate with nickel only on the internal surfaces the losses increase, being
4
109 Ω/m, that means approximate 50 times bigger that those from the case of pure copper
conductors.
Fig. 4.1. HF losses for two conductor configurations
Starting from this simple model, the conductors plate-nickel technique was extend for a
complex structure, the reference structure that is proposed by the author for the considerate
analyses, named in the chapter Original_structure.
Fig. 4.2. The Original_structure
If in the previous case ware studied all the possible combinations of nickel-plate conductors,
for this structure were analyzed only the models that could be realized practically. So, for the
Original_structure are proposed two alternatives: the solution of plate with nickels only the external
surface of each conductor and the solution of plate with nickel both external and lateral surfaces of
each conductor. For each proposed method were analyzed four cases depending on the supply mode
of the LC integrate structure and of auxiliary winding. Doing this analysis we can conclude that the
most efficient method to increase the HF losses in the case of the Original_structure is the solution
to plate the external and lateral surfaces of each conductor with nickel. This conclusion can be
extend and use also for structures with more complex geometries. Also, we observed that the supply
mode of conductors does not influence significant neither the losses on each conductor nor the total
losses on each structure. In conclusion, observing the losses values, for example at the frequency of
10 MHz, the losses per unit length in the case of pure copper conductors are 0.68 Ω/m, while for the
case in which the external and lateral surfaces are plate with nickel the losses increase, being
approximate 14 Ω/m, that suggest a big potential for the propose technology.
Also, in this chapter are presented some of most suggestive representations of current
densities distributions obtain by numerical modeling both in pure copper conductors and in those
plated with nickel, in CM and DM supply sequences.
5
Fig. 4.3. Current density distributions for the Original_structure study configurations proposed
Is interesting to observe that at high frequency, in the case of pure copper conductors, the
current flow on the lateral sides of the conductors, while in the conductors plate with nickel the
bigger current densities are observed only in the areas plated with nickel, for both supply sequences,
that lead at the idea that in HF in this case the losses are not influenced by the supply sequences.
Chapter 5, entitled Integrate EMI filters performances improvement by reducing the
structural parasitic capacitance, shows the author contributions at the EMI filters performances
improvement, that are realized with planar magnetic technology, by reducing the structural parasitic
capacitance. Are presented the principles of structural capacitance reduction of the respective
system, taking account of the problem complexity, are proposed two method of approach the study:
using the energetic method and applying the partial capacitance. Starting with the basic models, we
want to efficient the proposed techniques by 2D and 3D numerical modeling. The conclusion is
unique for all the tested types of the models, that the using of the staggered winding represents the
best compromise between the mechanical stability of the system and the minimal value of the
structural capacitance, the medium factor of reduction being 8. In this light, in the second part of the
chapter, the author outlines the optimal study of the winding staggered such as to obtain the minim
structural capacitance. For this was developed an original optimal design software package.
6
Fig. 5.1. The 3D model for the analysis of the structural capacitance
Fig. 5.2. The way the 3D staggered winding is realized, 2 solutions
x
0
xmin xmax
(a) problem formulation (b) objective function variation in the search space
Objective function
1.24E+00
1.34E+00
1.44E+00
1.54E+00
1.64E+00
1.74E+00
0 1 2 3 4 5 6 7 8
no of i t e r a t i on
Fmin = 1.24054 Foptim = 1.24055 reduction to 73% εr
= 8 E-4 [%]
(c) the optimal solution and several start points in the optimal design. Routes to the optimal solution
Fig. 5.3. Testing the convergence of the optimal design algorithm developed
7
After it was tested on applications that consist of one and two design variables, it passes at
study of more complex geometries, with until 8 design variables. The obtained results relieving the
optimal arrangement of the conductors, the mode in which the distance between the winding spirals
influence the optimal solution and his oneness, being a very useful tool in the established of the
optimal geometrical configuration of the EMI filter layers structure for the minimization of his
parasitic capacitance. In the last part of this chapter is show an original graphic interface that allows
the easy utility of the developed optimal design algorithm and that helps to directly follow up the
steps with which get to the optimal solution in the optimization process and allow the quick
visualization of the simulation results.
Chapter 6, entitled Integrate EMI filters performances improvement by simultaneously
application of the proposed techniques and experimental validation, shows the authors’
contributions in the direction of simultaneously application of EMI filters performances
improvement proposed techniques on the proposed and developed EMI filters in the anterior
chapters and the validation by experimental measurements of the proposed solutions. As in the
anterior chapters, the study is gradually realized, starting from the proposed techniques
simultaneous effects analysis for a LC structure type ‚nucleus’ of an EMI filter, that is composed of
3 windings. The follow of this realized study both in 2D and 3D cases, is the fact that this structure
realize superior performances in report with the original by simultaneous application of the two
techniques and the fact that the winding stagger does not affect the HF losses by nickel-plate of the
copper conductors, we pass at the study of the structures type EMI filter. We start also in this case
from a simple 2D structure; the good obtain results motivating the pass to the study of the 3D real
structure of the EMI filter.
(a) the original structure (b) the optimized staggered winding
Fig. 6.1. The 2D EMI Filter
Given being the limited 3D numerical modeling possibilities of the cumulative global effects
of the proposed techniques on the transfer characteristics of the filter, his performances are
separately studied. So, for the electrical component, the conclusion being that the structural parasitic
capacitance is decrease until 47% of initial value. For the magnetic component, the response in
8
frequency is compared between the original structure without stagger winding and without nickel-
plate, with the final structure that consist of optimal stagger winding and nickel-plate of the
conductors. We determinate that the impedance on the in terminals increase with 32%, the results
being obtained by numerical 3D modeling.
(a) the compact view and the equivalent circuit (b) exploded view of the two structures analyzed
Fig. 6.2. The 3D EMI filter implemented
(a) the filter metallic structures, interconnected (b) structure 1
(c) structure 2 (d) structure 3
Fig. 6.3. The 3D EMI filter – details for interconnections
9
Fig. 6.4. The computed transfer function
In conclusion, we can say that the EMI filter parameter improvement techniques proposed and
systematically analyzed in this thesis and which has the purposed the reduction of structural
capacitance and the HF losses increased prove the efficiency by numerical modeling.
For the final validation of the research activity done in this doctorate thesis, in the last part of
the chapter are presented the experimental measurements results. Because of the technological
possibilities limitation, the experimental measurements are realized in the case of some filters type
FTJ (LPF) made in planar magnetic technology. Are compared the frequency responses and the
filter attenuations made in original mode, without stagger between the windings, with filter that
contain the optimal stagger between these. The superior attenuation on the frequency range of the
conduction emissions in the electrical-power network of the BD filter 150 kHz – 30 MHz in report
with SO filter represent the experimental validation of the solution correctitude by the suppression
of the propose structural capacitance and applied in the case of EMI filters. Not the last, has to be
remarked the good attenuation of the planar integrated LC structure – both in SO mode as in the BD
mode – realized in FTJ connection type, in this way we can conclude that the planar integrate
structures are an attractive solution for the passive EMI filter realization.
(a) exploded view (b) experimental measurements set-up
Fig. 6.5. The low pass filter in planar magnetic technology
10
Ref 87 dBµV Att 0 dB*
B
*
*
3DB
RBW 10 kHzVBW 30 kHzSWT 1.5 s
AC
TG -20 dBm
Start 15 kHz Stop 30 MHz2.9985 MHz/
NOR
1 SACLRWR
IFOVL
-40
-35
-30
-25
-20
-15
-10
-5
0
5
10
1
Marker 1 [T1 ] -1.26 dB 74.970000000 kHz
NOR 0 dB
Date: 18.AUG.2010 09:35:36
Ref 87 dBµV Att 0 dB*
B
*
*
3DB
RBW 10 kHzVBW 30 kHzSWT 1.5 s
AC
TG -20 dBm
Start 15 kHz Stop 30 MHz2.9985 MHz/
NOR
IFOVL
1 SACLRWR
-40
-35
-30
-25
-20
-15
-10
-5
0
5
10
1
Marker 1 [T1 ] -5.54 dB 74.970000000 kHz
NOR 0 dB
Date: 18.AUG.2010 09:27:31 (a) the original structure (SO) (b) the staggered winding structure (BD)
Fig. 6.6. Experimental results of the transfer function for the low pass filter realized in planar magnetic technology
The authors’ contribution in this chapter consists in the design, implementation, 2D and 3D
numerical modeling, and results assumption and interpretation in the case of all the presented
electromagnetic devices. Also, the author design and practically made the LC integrate structures
presented in this chapter and take part to the experimental measurements of their attenuation in FTJ
type configuration and at the dates assumption and results interpretation. The final conclusion of the
chapter is that by the presented and obtained results, we can say that the doctorate thesis purpose
was reach, the propose techniques for the EMI filters performances improvement are full efficient.