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

Brandštetter, Pavel

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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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]: © 2012 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 89 THEORETICAL AND APPLIED ELECTRICAL ENGINEERING VOLUME: 10 | NUMBER: 2 | 2012 | JUNE  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 © 2012 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 90 THEORETICAL AND APPLIED ELECTRICAL ENGINEERING VOLUME: 10 | NUMBER: 2 | 2012 | JUNE 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 THEORETICAL AND APPLIED ELECTRICAL ENGINEERING VOLUME: 10 | NUMBER: 2 | 2012 | JUNE 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. © 2012 ADVANCES IN ELECTRICAL AND ELECTRONIC ENGINEERING 94