Györök, György

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Automatic Analog Circuit Synthesisby BF methodsGyo¨rgy Gyo¨ro¨kAlba Regia technical FaculityO´buda UniversityBudai Str. 45, H-8000 Sze´kesfehe´rva´rgyorok.gyorgy@amk.uni-obuda.huAbstract—As we wrote in our earlier article [10] the automaticsynthesis of digital circuit is mostly solved, at a well definedboundary conditions. Algorithm of a digital topology generatingcan be performed. From traditional discrete electronic partsan analog circuit implementation is almost impossible,becauseanalog integrated circuits configurable through a digital interfacealready exist.Automatic synthesis of analog circuits can be important,because are through a digital interface configurable analogintegrated circuits.All these, and increasing processing performance of computersare new approaches to be made, even the brutal force (BF)methods [23] [25].Such synthesis may be important not only in the synthesis ofdiscrete components, but circuit modules can be used, whetherthe case of configurable analog circuitry system synthesis.In engineering practice the commonly used brute force methodis very resource-intensive process.The present article shows an optimization method by which thepurely theoretical possibilities are considerably reduced therebyit increases the rate of synthesis.In the current article, partly as a result, finished a computerprogram that can automatically generate circuit topologies. Wewill now deal with some aspects of this.I. INTRODUCTIONAn analog electronic circuit function ( Gc) and behavior (f)is determined by the parameters of the used components (P)and the connect topology (n), according to (1);Gc = f(n;P): (1)The circuit function is of course not an exact definition, butit can mean for example from input to output time domaindetermined amplitude function, frequency-domain amplitudebehavior...etc. The used circuit description depends on thesuspected, or the realized function of circuit [24] [26] [28].Parameter (n) describes the network of the discrete com-ponent, in there pins are well determined connected to eachother.In equation (1) the P parameter is a scalar vector, thatcontains the relevant parameters of used electronic parts informal (2);P 2 p0; p1; p2:::pn; (2)Fig. 1. Integrator circuit.where pn the significant parameter of electronic part, forexample resistance of a resistor, capacitance of the a capacitor,h21 of a bipolar tranzistor. . . etc. [6] [22].On Fig. 1 is seen, as above example an integrator circuit.This circuit contains an operational amplifier (A1), a squarewave input generator; (V1) Upp = 2V , Uo f f set =  1V , twopower source; (V2, V3) with 15V, a feedback capacitor (C1)its value is 22mF, and a resistor (R1) and value of last one is330W. These parts lists and entering a value defining of the Pvector [2] [3] [9].Fig. 2 shows a connection network in short form ”netlist”about of circuit of Fig. 1. This netlist describes the nods ofcircuits (N$1, N$3, N$5). The nods N$3 connect 2 numberpads of capacitor (C1), output of amplifier (A1) with 4 padsof integrated circuit, and output of circuit to X2 connector [5][7].Nowadays the development of such a circuit heuristicmeans. We know the circuit operation, the availability of partsand components to form a network with the appropriate values[16] [1]. To draw the circuit CAD tools are used, as well ascircuit simulation. Network of Fig. 2 is generated from wiringdiagrams[8] [4] [27] [29].Computing environment is possible to check by circuitsimulation software the operation of the realized circuit. Fig.3 shows in time domain the circuit operation from input tooutput [13] [14] [15].Net Part Pad PinGND IC1 1 +INX1 1 SX2 2 SN$1 C1 1 1IC1 3 -INR1 2 2N$5 R1 1 1X1 2 SN$3 C1 2 2IC1 4 OUTX2 1 SVCC- IC1 2 V-VCC+ IC1 5 V+Fig. 2. A integrator circuit’s connection network.Fig. 3. Time domain simulation of integrator circuit. Bottom input signal,above the output.II. ANALOG CIRCUIT REALIZATION BY A SWITCHINGMATRIXTheoretically, if we have n numerous electronic componentseach of them has got fi pins which are necessary to properlyconnect with a wished analog circuit. If every possible waywe want to create a circuit network, we need a matrix thatconsists of o number of columns according the (3);o=n 1åi=0fi 1åj=0ci j; (3)where for Am;(i; j) is true (4);Am;(i; j) 2 [0;1]: (4)On Fig. 4 theoretical arrangement of a switching matrix isshown. This matrix consists of electronic parts’s dev0–devnleg wires as columns c00–cn(f 1), and row wires for possibleinterconnections r0–rm 1. In (4) 0 means no connection be-tween column and row wires, and 1 case is have got, this isactually a switch function, which is described of turned ONand OFF state. On Fig. 4 we signed this function by a switchkg [20] [19].It can be seen that the pins of electronic components andthe interconnection wires formed from a matrix of mxn type,where m=n, so there is square matrix, which contains all thepossible options of connections, according in equation (5):This square matrix from equation (3) contains numerouscross points according to (6) is;Cp = o2: (6)Thus, the number of theoretically possible different topol-ogy (Tn) from equations (5) and (6) is;Tn = 2Cp : (7)Fig. 4 layout and description of equations (5) and (6) are soperfectionist that includes abilities of all the parts legs wiresthe possibility of connecting a node, as well as the possibilityof all parts foot stand-alone, a unique node [18] [17].dev 0 dev 1 dev 2 dev 3 dev nkgr0r1r2r3r4r5rm-1c00 c01 c10 c11 c12 c20 c21 c30 c36 cn0 cn(φ−1)crFig. 4. Theoretical arrangement of a switching matrix for the evolving everyabilities connections.III. OPTIMIZATION OF A SWITCHING MATRIXIn the previous paragraph the possibility formation of thetheoretical switch matrix is shown. According to the describedsolution we generate from the circuit of Fig. 1 or net list ofFig. 2 in matrix’s in Fig. 5.On Fig. 5 it can followed that every nods of netlist meansa row of matrix; r0 = GND, r1 = N$1, r2 = N$2, r0 = N$3,r0 = N$4, r0 = N$5. You can see that the rest of any unusednods abilities from r6–r16.The electrotechnical or physical reason of the not used abili-ties is understandable, because it is meaningless to connect, forexample, two power supplies (N2, N4), or output of operationalamplifier (N3) with input signal source (N5). Of course one canfind too much refusal of this kind.Am;(i; j) =2666664b0;(0;0) b0;(0;1) b0;(1;0) b0;(1;1) b0;(1;2) b0;(2;0) b0;(2;1)    b0;(n;f 1)b1;(0;0) b1;(0;1) b1;(1;0) b1;(1;1) b1;(1;2) b1;(2;0) b1;(2;1)    b1;(n;f 1)b2;(0;0) b2;(0;1) b2;(1;0) b2;(1;1) b2;(1;2) b2;(2;0) b2;(2;1)    b2;(n;f 1)................... . ....bm 1;(0;0) bm 1;(0;1) bm 1;(1;0) bm 1;(1;1) bm 1;(1;2) bm 1;(2;0) bm 1;(2;1)    bm 1;(n 1;f 1)3777775 : (5)R1r0r1r2r3r4r5c00 c01C1 V1 V2 V3 Out A1r6r7r8r9r10r11r12r13r14r15r16c10 c11 c20 c21 c30 c31 c40 c41 c50 c51 c60 c64c62Fig. 5. Integrator circuit realization in actually connections on a switchingmatrix.So our proposal is such structural switch matrix which cannot afford such unusual theoretical, often catastrophic resultinflict solution.On the other hand, it is necessary to minimize number ofcross points, because the number of ability network accordingto the equation (7) easy to be huge combination.In the theoretical matrix (Fig. 5 and 5) the number ofconnection, according equations (6) and (7) was: rm 1 cn(f 1),actually in examples are Cp = 172;Cp = 289 so the abilitiestopology are Tn = 2289;Tn = 9;94 1086.These values at the proposed structural switch matrix arein order to form; Cp = 17  10;Cp = 170, and Tn = 2170;Tn =1;49 1051. The different according Tn parameter in 1035.R1r0r1r2r3r4r5c00 c01C1V1V2V3Out A1r6r7r8r16c10 c11 c20 c21 c60 c63r9r10r11r12r13r14r15Fig. 6. Integrator circuit realization on structural switching matrix.Other mitigation options appropriate management of com-mon GND node, and self-evident is providing of active de-vice’s power supply [11] [12].A special heuristic approach is the elimination of not usedrows of matrix, on Fig 6 from r8  r16. So the number of Tcis ”only” 1;2 1024.IV. AUTOMATIC SYNTHESIS BY BRUTAL FORCE METHODSBased on the principles described in the previous chaptercreated a computer program using the structural switch matrix-oriented aspects. The main screen of running netlist generator-program shown on Fig 7, and on Fig 8 are seen a part ofgenerated netlist directories [21].Fig. 7. Main screen of topology generator program.The generated files are all made the right format, so calledCKT, for Spice (MICROCAP-10) circuit simulation program.This standard format shows Fig 9.Together with the generated files clearly describe the circuittopology, the circuit graphic display can also be important. Is afree program can help solve the visualization of the connectionof circuit, with using some circuit macros. On Fig 10 sows anyrandom topology of generated netlist files.Of course, each of Fig 9 has a netlist format a real elementsfeasible circuit, but they are usually unnecessary to show.However, the practicing engineer with more information isFig. 8. A part of generated netlist file’s directory.Fig. 10. Any automatically generated ”integrator” circuits on a Netlist-viewer program’s screen. On upper side of figures there are from 1–6 poles of abilitynodes of integrator of Fig. 1.Fig. 11. Three wrong ”integrator” circuit in Micro-Cap simulation environment.displayed in the traditional circuit diagrams, some examplesof which are shown in Fig 11.V. CONCLUSIONSThe previously proposed structured switch-matrix we cangenerate a combinatorial topology wit an appropriate computerprogram. 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Automatic Analog Circuit Synthesis by BF methods

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