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Third order low-pass filter using synthetic immittance elements with current conveyors

Abstract

The paper deals with a theoretical proposal of the resulting circuit of the frequency filter using synthetic immittance elements of higher order with current conveyors. The text pays particular attention to design process of synthetic immittance elements, explains the principle of increasing of order, which is then reflected to the frequency filter order. The text then deals less with the theory of current conveyors, which has already been discussed, in detail, in previous papers. Universal current conveyor (UCC) is discussed more. This active element is used for the theoretical implementation of the synthetic element solution used in the frequency filter. The theoretical knowledge is then demonstrated in the design of 3rd order low-pass frequency filter. The final functionality of the proposed frequency filter circuit solution is validated by PSpice simulation.

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Third order low-pass filter using synthetic immittance elements with current conveyors

Author: Brandštetter, Pavel
Publisher: Vysoká škola báňská - Technická univerzita Ostrava
Year: 2012
Source: https://dspace.vsb.cz/bitstreams/d5f253dc-c2fb-499e-a84e-921838513080/download
THEORETICAL AND APPLIED ELECTRICAL ENGINEERING VOLUME: 10 | NUMBER: 2 | 2012 | JUNE
THIRD ORDER LOW-PASS FILTER USING SYNTHETIC
IMMITTANCE ELEMENTS WITH CURRENT CONVEYORS
Pa el BRANDSTETTER1, Lukas KLEIN1
1Depa men o Elec onics, Facul y o Elec ical Enginee ing and Compu e Science, VSB-Technical Uni e si y o
Os a a, 17. lis opadu 15, 708 33 Os a a, Czech Republic
pa el.b ands [email p o ec ed], lukas.klein@ sb.cz
Abs ac . The pape deals wi h a heo e ical p oposal o
he esul ing ci cui o he equency il e using syn he ic
immi ance elemen s o highe o de wi h cu en
con eyo s. The ex pays pa icula a en ion o design
p ocess o syn he ic immi ance elemen s, explains he
p inciple o inc easing o o de , which is hen e lec ed o
he equency il e o de . The ex hen deals less wi h he
heo y o cu en con eyo s, which has al eady been
discussed, in de ail, in p e ious pape s. Uni e sal cu en
con eyo (UCC) is discussed mo e. This ac i e elemen is
used o he heo e ical implemen a ion o he syn he ic
elemen solu ion used in he equency il e . The
heo e ical knowledge is hen demons a ed in he design
o 3 d o de low-pass equency il e . The inal
unc ionali y o he p oposed equency il e ci cui
solu ion is alida ed by PSpice simula ion.
Keywo ds
Cu en con eyo , equency il e , low-pass il e ,
syn he ic immi ance elemen .
1. In oduc ion
Me hod o he syn he ic elemen s is p ima ily based on
he needs o classical induc o s subs i u ion by syn he ic
equi alen s in elec onic ci cui s. I is no a new me hod,
bu i s use in combina ion wi h new mode n ac i e
componen s (cu en con eyo s), o he design and
ealiza ion o equency il e s, is a ela i ely new idea
[1], [2], [3], [4], [5], [6], [7], [8].
The basic ad an ages o using cu en con eyo s
[1] include a wide equency ange, ease o in eg abili y
o he esul ing ci cui solu ions, low supply ol age o
ac i e elemen s and he possibili y o use o ba e y
supply in esul ing ci cui , when i is used in he mobile
de ices.
Cu en con eyo s
[1] can be basically ega ded as
uni e sal elemen s, because ou basic unc ional block
s uc u es can be ealized by combina ions o hese ac i e
elemen s.
Howe e , he basic disad an age is low
comme cial a ailabili y o cu en con eyo s and
comme cial una ailabili y o uni e sal cu en con eyo
(UCC), which was selec ed o he ealiza ion o il e
p oposed in his pape . Selec ion o UCC has i s
impo an easons. This elemen seems o be e y
p omising, especially in he design o ci cui solu ions
wi h cu en con eyo s, because i could be used o he
implemen a ion o all cu en con eyo s a ia ions.
Uni e sal cu en con eyo cu en ly exis s only as a
labo a o y sample and he wide ex ension ye o come.
The pape ies o show i s impo ance and he
ad an ages.
2. Syn he ic Immi ance Elemen s o
Highe O de s
Syn he ic dipoles wi h immi ance o highe o de [2] a e
di ided in o ou g oups – DP, DS, EP, ES. They a e
consis ing o se ial o pa allel elemen a y dipoles
connec ions. Syn he ic elemen s DP, DS a e c ea ed by
elemen a y D ype dipoles o o de 0 o ND,max. Syn he ic
elemen s EP, ES a e c ea ed by elemen a y E ype dipoles
o o de 0 o NE,max.
The linea ci cui s heo y discusses ha s able
equency il e s can be ealized, i he elemen a y dipoles
o all o de s om he lowes (nd,min, ne,min) o highes
(nd,max, ne,max) will be connec ed in he syn he ic
elemen s. Mos o he alues o nd,min, ne,min equal o 0 o
1, alues o nd,max, ne,max se he o de o he syn he ic
elemen . In he mos cases, hese alues also se he o de
o equency il e ans e unc ion, espec i ely.
As s a ed abo e, he e a e ou connec ions o
syn he ic elemen s wi h immi ance o highe o de [2]:
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 dipole DP ND,min ND,max consis s o a pa allel
connec ion o syn he ic elemen a y dipoles o ype
Dn o n = ND,min, ND,min + 1, ..., ND,max - 1, ND,max,
 dipole DS ND,min ND,max consis s o a se ial
connec ion o syn he ic elemen a y dipoles o ype
Dn o n = ND,min, ND,min + 1, ..., ND,max - 1, ND,max,
 dipole EP NE,min NE,max consis s o a pa allel
connec ion o syn he ic elemen a y dipoles o ype
En o n = NE,min, NE,min + 1, ..., NE,max - 1, NE,max,
 dipole ES NE,min NE,max consis s o a se ial
connec ion o syn he ic elemen a y dipoles o ype
En o n = NE,min, NE,min + 1, ..., NE,max - 1, NE,max.
2.1. The Condi ions o Syn he ic
Immi ance Elemen s Realiza ion
I sui able syn he ic immi ance elemen s o highe o de
should be designed, hen an app op ia e o m o inpu
impedance, espec i ely inpu admi ance is sea ched [3].
The equi ed inpu impedance espec i ely inpu
admi ance o m o syn he ic immi ance elemen s o DS
and ES ype should be:
VWV
U
IN YYY
Y
Z1
 ,
WU
WV
IN YY
YY
Y
. (1a, b)
Inc ease o syn he ic elemen o de is done by
epea edly eplace o admi ance YV wi h ci cui wi h
inpu admi ance (1b). Inc ease o o de o syn he ic
immi ance elemen can also be achie ed by eplacing he
admi ance YU wi h ci cui wi h he inpu admi ance (2b).
Fo syn he ic immi ance elemen s o DP and EP
ype, i is equi ed inpu impedance espec i ely
admi ance in o m:

WVU
W
IN YYY
Y
Z
, U
W
VU
IN Y
Y
YY
Y . (2a, b)
Admi ance YV is epea edly eplaced wi h ci cui
wi h he inpu admi ance (2b), i we wan o inc ease
o de o syn he ic immi ance elemen .
3. Uni e sal Cu en Con eyo
Uni e sal cu en con eyo (see Fig. 1) was c ea ed on
he base o he uni e sal elemen idea, which could easily
implemen e e y cu en con eyo gene a ion o a ia ion
in p ac ice. This elemen would allow a di e en
applica ion use o cu en con eyo s and hei wide
expansion. Uni e sal cu en con eyo has me hese
equi emen s [4].
I can ealize all he known ypes o cu en
con eyo s. I is he basic p inciple o i s e sa ili y.
Implemen a ion o he a ious ypes o cu en con eyo s
is p o ided by use o only ce ain inpu and ou pu
e minals o uni e sal cu en con eyo , he emaining
e minals a e p ope ly connec ed o g ounded.
Ano he ad an age o he elemen is ha i
con ains se e al inpu and ou pu e minals, which
p o ides an oppo uni y o sum signals a he inpu o
con eyo o o di ide he ou pu signals o mul iple
loca ions [4]. The ac i e elemen is no cu en ly mass
p oduced, and he e o e no widely a ailable.
Fig. 1: Schema ic symbol o uni e sal cu en con eyo (UCC).
Te minals Y1+, Y2-, Y3+ a e he ol age inpu s, X
is he cu en inpu (see Fig. 1). Te minals Z 1+ and Z2+
a e cu en ou pu s wi h a posi i e ans e o cu en , Z1-
and Z2- a e cu en ou pu s wi h a nega i e ans e o
cu en om e minal X.
The uni e sal cu en con eyo is gene ally
desc ibed by equa ions [4]:
321 YYYX uuuu



, ,
0
321

YYY
iii
XZZ iii


 21 , . (3a, b, c, d)
XZZ iii   21
4. Realiza ion o Syn he ic
Immi ance Elemen s wi h
Cu en Con eyo s
I he app op ia e s uc u e o syn he ic immi ance
dipoles o ype DP, DS, EP and ES ype is sea ched, hen
he pa icula o m o inpu admi ance o impedance is
p ima ily equi ed. I is e y di icul o ind he exac
exp essions ha equal o he o mulas (1a, b) espec i ely
(2a, b). We can mo e o en ind he exp essions
app oaching hese o ms han exac o ms. They can be
also used.
Howe e , i is necessa y o heo e ically e i y
hei sui abili y o use in equency il e s. The main
a ge is o ge o ms o equa ions ha will be mos
simila o he equa ions (1a, b) espec i ely (2a, b).
The gene al ci cui ne wo k o sea ching o
sui able ci cui s uc u es was used o implemen
syn he ic immi ance elemen . The gene al ci cui
ne wo k consis s o nine passi e elemen s (admi ances)
and one gene al ou -po cu en con eyo [2]. Final
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s uc u e is shown in Fig. 2.
Fig. 2: De aul admi ance ne wo k o sea ch he syn he ic elemen
solu ion.
The syn he ic elemen sea ching p ocedu e is qui e
simple. The selec ed admi ances a e emo ed om he
gene al ci cui ne wo k. The esul ing ci cui s uc u e
should consis o h ee admi ances and gene al ou -po
cu en con eyo . Th ee admi ances a e enough o ealize
he syn he ic immi ance elemen . Any o he gene al
cu en con eyo e minals Y, X, Z1 o Z2 can be used as
he inpu o he esul ing ci cui s uc u e [5]. The inpu
admi ance o m is hen edi ed again by he sui able
choice o he gene al cu en con eyo coe icien s a, b,
c11, c22. I is inal change o he inpu admi ance. The
inal inpu admi ance o he esul ing ci cui is hen
deduc ed, i i equals (1a, b), (2a, b) o o ms close o
hese equa ions. Se e al dozens o combina ions we e
examined his way.
Figu e 3 shows one o he ound s uc u es ha
can be used o he ealiza ion o syn he ic elemen . The
ci cui is sui able o implemen ing il e s o highe o de .
Fig. 3: Ci cui s uc u e sui able o ealiza ion o syn he ic elemen .
The inpu admi ance gene al o m o he ci cui
shown in Fig. 3 has he o m:
22711771122
9722929222722272
1172117272727272
IN cYcYYcYY
abYYacYYabYYacYYcYY
acYYcYYabYYbYYaYYYY
Y


. (4)
The e he alues o he gene al cu en con eyo
coe icien s om he possible combina ions we e chosen.
Bes sui ed combina ion is a=-1, b=0, c11 =-1, c22=1. This
combina ion o alues simpli ies he inpu admi ance
gene al o m and b ings i o i s ideal o m. Gene al
ci cui s uc u e is sui able o implemen he syn he ic
immi ance elemen s DP o EP (1a, b). Selec ed
coe icien s co espond o he in e ing cu en con eyo
o second gene a ion ICCII+/-. A e his adjus men , he
inpu admi ance o he ci cui is ans o med in o he
o m:
2
7
92
IN 2Y
Y
YY
Y ,
)2( 792
7
IN YYY
Y
Z
. (5a, b)
Ta ge ed selec ion o passi e elemen s and hei
subs i u ion o gene al admi ance in he ci cui s uc u e
c ea e he syn he ic immi ance elemen DP o second
o de . The ci cui s uc u e is shown in Fig. 4.
Fig. 4: Ci cui s uc u e o second o de syn he ic elemen DP.
The esul ing inpu admi ance o syn he ic
immi ance elemen shown in Fig. 4 has he o m:
. (6)
2927
2
IN 2CpCCRpY 
4.1. Syn he ic Immi ance Elemen O de
Inc easing
Inc easing o he syn he ic elemen o de will be
demons a ed on he syn he ic elemen shown in Fig. 4.
Inc easing o he syn he ic elemen o de is cascade, i.e.
he e is a epea ed eplacemen o a passi e elemen o a
whole ci cui s uc u e o iden ical syn he ic elemen in
he s uc u e o syn he ic elemen . Inc easing o o de o
syn he ic elemen in Fig. 4 o hi d o de shows Fig. 5.
As can be seen om Fig. 5, he capaci o ma ked
in Fig. 4 as C9 was eplaced by ci cui s uc u e o
syn he ic elemen DP shown in Fig. 4.
Fig. 5: Thi d o de syn he ic immi ance elemen DP.
© 2012 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 91
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The numbe o capaci o s in he s uc u e o a
syn he ic elemen was inc eased. The esul is also
inc easing o he syn he ic elemen o de . The inpu
admi ance o he newly c ea ed syn he ic elemen o
hi d o de has o m as ollows:
. (7)
1211
2
32121
32CpCCRpCCCRRpYIN 
The new inc easing o o de o syn he ic elemen
would be made by eplacing he capaci o C3 o he
whole syn he ic elemen s uc u e shown in Fig. 4. Fo ms
o o he inpu admi ance caused by inc easing o he
syn he ic immi ance elemen o de a e shown in Tab. 1.
Tab.1: Inpu admi ance o ms.
O de o
Syn he ic
Elemen Inpu Admi ance Fo m
4. YIN = p4R1R2R3C1C2C3C4 + p32R1R2C1C2C3 +
p2R1C1C2+ p2C1
5.
YIN = p5R1R2R3R4C1C2C3C4C5 +
p42R1R2R3C1C2C3C4 +
p32R1R2C1C2C3 + p2R1C1C2 + p2C
1
6.
YIN = p6R1R2R3R4 R5C1C2C3C4C5C6 +
p52R1R2R3R4C1C2C3C4C5 +
p42R1R2R3C1C2C3C4 +
p32R1R2C1C2C3 + p2R1C1C2 + p2C1
7.
p52R1R2R3R4C1C2C3C4C5 +
p42R1R2R3C1C2C3C4 +
p32R1R2C1C2C3 + p2R1C1C2 + p2C1
YIN = p7R1R2R3R4 R5R6C1C2C3C4C5C6C7+
p62R1R2R3R4 R5C1C2C3C4C5C6 +
5. F equency Fil e s Using Syn he ic
Immi ance Elemen s
The e was used syn he ic immi ance elemen DP shown
in Fig. 5 o he ealiza ion o low-pass il e o hi d
o de . Ci cui solu ion o hi d o de low-pass is shown in
Fig. 6.
FThi d o de low-pass using syn he ic elemen wi h cu en
con eyo s.
Two uni e sal cu en con eyo s we e used in he
inal ci cui solu ion o ac i e equency il e . Wi h i s
help, ICCII+/- was implemen ed. The e was also used
passi e low-pass a he inpu o ac i e il e o smoo h he
inal equency esponses a highe equencies. Resis o
R
ig. 6:
he wi h capaci o C1. T ans e unc ion o
ac i e hi d o de low-pass shown in Fig. 6 has o m as
ollows:
1 was di ided in o wo pa s, and i c ea es passi e low-
pass oge
1442 213221
2
432321
3
CRpCCRRpCCCRRRp
KU
Speci ic alues o passi e componen s we e
calcula ed wi h gen
1
)( p. (8)
e al design ela ions o ac i e hi d
de low-pass [6]:
o
432321
3
0
33 2
cCCCRRR

, (9)
3221
2
0
32 4
cCCRR

, (10)
21
0

Bu e wo h app oxima ion was chosen. The
coe icien s o his app oxima ion o il e s o hi d o de
ha e alues c
31 4
cCR. (11)
esis o s (12), (13), (14) a e
exp essed om equa ions (9), (10), (11):
31=c32=2, c33=1 [6]. As al eady men ioned
in he p e ious ex , he alues o capaci o s a e chosen
and alues o esis o s a e calcula ed. The alues o
passi e elemen s o equency il e a e also based on he
chosen alue o cu -o equency 1 MHz and he
coe icien s o chosen app oxima ion. The o ms o
calcula ion o alues o
20
31
14
c
C
R

, (12)
3310
32
2
c2
Cc
R

, (13)
4320
3Cc

Values o esis o s a e calcula ed a e subs i u ing
o speci ic alues. Op imiza ion in PSpice was also used
o de e mine he ideal alues o passi e elemen s. The
esul ing alues o he passi e elemen s we e de e mined
R
33
c2
R. (14)
1=2,7 kΩ, R2=5,6 kΩ, R3=1,2 kΩ, C1=C2=C3=22 pF,
C4=100 pF. The esul ing ampli ude equency esponse
and phase esponse o a eal model o hi d o de low-
pass is shown in Fig. 7. The e a e wo aces he e. Fi s
ace is o ci cui solu ion o ac i e low-pass and second
ace desc ibes he beha io o ci cui solu ion o ac i e
low-pass using also passi e low-pass. As can be seen, use
o passi e low-pass in he ci cui s uc u e o hi d o de
ac i e low-pass changes he posi ion o cu -o equency.
Howe e , his solu ion also gi es good esul s a highe
equencies, whe e he gain inc ease is educed. Cu -o
equency o he il e is de ined as a dec ease o
magni ude abou 3 dB [6]. Cu -o equency in his case
was chosen 1 MHz. The simula ed cha ac e is ic shown
in Fig. 7 does no exac ly ma ch hose equi emen s. The
selec ed cu -o equency o 1 MHz is de ined as a
dec ease o ampli ude equency esponse abou 4,43 dB.
Such a la ge de ia ion can be ole a ed. Some o
© 2012 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 92
THEORETICAL AND APPLIED ELECTRICAL ENGINEERING NUMBER: 2 | 2012 | JUNE VOLUME: 10 |
© 2012 IN ELECTRICAL AND ELECTRONIC ENGINEERING 93
ideal
ope
hange o cu -o equency o ac i e low-pass depends
cula aces depending on he a iable ole ance o
C2.
he ac o s ha could cause he de ia ion a e he
p ies o he used uni e sal cu en con eyo model
and he passi e low-pass a he inpu o ac i e il e .
Also, sensi i i y analysis was ca ying ou . The
mos ly on capaci o C2. The ampli ude equency
esponse and phase esponse shown in Fig. 8 desc ibe
pa i
c
Fig. 7: Ampli ude equency esponse and phase esponse o hi d o de low-pass using syn he ic elemen wi h cu en con eyo s.
Fig. 8: Mon e Ca lo analysis o ampli ude equency esponse and phase esponse o hi d o de low-pass wi h passi e il e .
he inal ci cui solu ion. This
y is a disad an age and
ADVANCES
6. Conclusion
The pape ies b ie ly desc ibe he ealiza ion o
equency il e s wi h syn he ic immi ance elemen s o
highe o de wi h cu en con eyo s. Applica ion use
o syn he ic immi ance elemen s b ings a lo o
ad an ages. One o he mos impo an ad an ages is
he easy in eg abili y o
is a e y impo an ac o especially in elec o-
indus ial p oduc ion.
I is ad an ageous o use uni e sal cu en
con eyo in design. UCC is able o subs i u e all
p e ious gene a ions o cu en con eyo s bu i s
comme cial una ailabili

THEORETICAL AND APPLIED ELECTRICAL ENGINEERING VOLUME: 10 | NUMBER: 2 | 2012 | JUNE
un sal cu en con eyo can be used only as a
heo e ical elemen now.
The desc ibed heo y and he inal ci cui
solu ion o hi d o de low-pass indica e ha he
desc ibed me hod p oduces ela i ely good esul s. The
a icle desc ibes only one o o al h ee ound syn he ic
elemen s. Despi e u he a emp s no o he elemen s
we e ound. I can he e o e be assumed o ind ano he
solu ion o syn he ic immi ance elemen s wi h cu en
con eyo s is e y di icul . Howe e , o he solu ions o
syn he ic immi ance elem
i e
en s can be ound wi h
combina ions o di e en ypes o cu en con eyo s o
wi h o he ac i e elemen s.
SP2012/85, which was suppo ed by S uden G an
Compe i ion o VSB-Technical Uni e si y o Os a a.
u en
c ions using
Uni e sal Cu en Con eyo . In: Con e ence
3868-6.
ISSN 0925-1030. DOI: 10.1007/s10470-
onics. 2009, ol. 96, iss. 8,
iwice: IEEE,
ional
ampli ie s. P aha: BEN, 2002. ISBN 80-7300-047-4.
n s,
Acknowledgemen s
In he pape , he e a e he esul s o he p ojec
Re e ences
[1] SMITH, K. C. and A. S. SEDRA. The cu en con eyo : a
new ci cui building block. IEEE P oceedings o he CAS.
1968, ol. 56, iss.1, ISSN 0018-9219.
[2] SPONAR, R. and K. VRBA. Syn he ic dipole elemen s wi h
highe -o de immi ances in equency il e s wi h c
con eyo s. Elek o e ue [online]. 2004, ol 2004, no. 13.
ISSN 1213-1539. A ailable a :
h p://www.elek o e ue.cz/clanky/04013/index.h ml.
[3] HORNG, J.-W., Ch.-L. HOU, Ch.-M. CHANG, H. YANG
and W.-T SHYU. Highe -o de immi ance un
cu en con eyo s. Jou nal Analog In eg a ed Ci cui s and
Signal P ocessing. 2009, ol. 61, no. 2, pp. 205-209. ISSN
0925-1030. DOI: 10.1007/s10470-009-9298-6.
[4] ZHANG, Q., Ch. WANG and Y. LENG. A No el Building
Block:
P oceedings o IEEE 8 h In e na ional Con e ence on ASIC.
Changsha: IEEE, 2009, pp 1109-1112. ISBN 978-1-4244-
[5] PSYCHALINOS, C. and G. SOULIOTIS. Low-Vol age
Cu en Con olled Cu en Con eyo . Jou nal Analog
In eg a ed Ci cui s and Signal P ocessing. 2010, ol. 63, no.
1, pp. 129-135.
009-9416-5.
[6] KOTON, J., K. VRBA and HERENCSAR. Tuneable Fil e
Using Vol age Con eyo s and Cu en Ac i e Elemen s.
In e na ional Jou nal o Elec
pp. 787-794. ISSN 0020-7217.
[7] BRANDSTETTER, P. and L. KLEIN. Applica ions o Non-
In e ing Posi i e Second Gene a ion Cu en Con eyo as a
Comme cially A ailable Ve sa ile Ac i e Elemen . In:
Con e ence P oceedings o In e na ional Con e ence on
Signals and Elec onic Sys ems - ICSES´10. Gl
2010, pp. 157-160. ISBN 978-1-4244-5307-8.
[8] PUNCOCHAR, J. His o y and p esen o ope a
Abou Au ho s
Pa el BRANDSTETTER was bo n in Os a a, Czech
Republic, 1955. He ecei ed he M.Sc. and Ph.D.
deg ees in Elec ical Enginee ing om B no Uni e si y
o Technology, Czech Republic, in 1979 and 1987,
espec i ely. He is cu en ly ull p o esso in Elec ical
Machines, Appa a us and D i es and ice dean o
Facul y o Elec ical Enginee ing and Compu e
Science a VSB-Technical Uni e si y o Os a a. His
cu en esea ch in e es s a e applied elec onics,
mic ocompu e con ol sys ems and mode n con ol
me hods o elec ical d i es.
Lukas KLEIN was bo n in Uhe ske H adis e in 1984.
He ob ained Bachelo ’s deg ee a B no Uni e si y o
Technology in ield o Telein o ma ics in 2007 and
hen he ob ained his Mas e ’s deg ee in ield o Mobile
echnologies in 2009 a VSB-Technical Uni e si y o
Os a a. He is cu en ly pu suing Ph.D. s udy a
Depa men o Elec onics on Facul y o Elec ical
Enginee ing and Compu e Science. His esea ch a ea
includes applica ion o mode n ac i e eleme
especially cu en con eyo s, in elec onic ci cui s.
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