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6961. HOUVW2 u Ta a gaT2u2J0 Sq- Tn aedUT ceouaT os BuTaeeuT Ous Jo aeq swJo esaep eqJOJDavid J .Greig B .Sc . B .E . ( Hon s .)NOLITIMONumaNO

ACKNOWLEDGEMENTSThe work contained in this thesis was carried out inthe Electrical Engineering department of the University ofTasmania. The author wishes to thank all the members of the, above department for their assistance. In particular theauthor thanks Professor C.H. Miller, and Hr. P. Watt,alis,supervisor, for their help and encouragement.I hereby declare that, except as stated herein, thisthesis contains no material which has been accepted for theaward of any other degree of diploma in any University, andthat, to the best of my knowledge this thesis contains nocopy of material previously published or written by anotherperson except where due reference is made in the text of thisthesis.

INDEX1INTRODUCTION1. INVESTIGATION OF THE CONTINUOUS-CARRIER AND PULSEMODULATIONS3Introduction11 Continuous Carrier Systems.12 Pulse Modulations.1.3 Comparison of Modulations.1.4 Introducing Delta Modulation.2. INVESTIGATION OF DELTA MODULATION14Introduction2,1 The Principles of Delta and Delta-Sigma Modulation.2.2 Early work by de Jager on Delta Modulation.2.3 A Review of Zetterbergis paper "A Comparison.Between Delta and Pulse Code Modulation".2.4 Delta-Sigma Modulation.2.5 Thermal Noise Considerations.2.6 The Problem of Obtaining Output Spectrum of aDelta Modulator in Terms of the Input Spectrum.2,7 Conclusions.3.AN EiTERIMENTAL DELTA-SIGMA MODULATOR41Introduction3,1 The Delta-sigma Modulation System,3.2 Demodulator Circuitry.3.4 Channel Simulation.3,5 Performance of System.3.6 Measurement of Signal to Noise Ratio.3 7 Quantizing Noise on D.C. Signal.5.8 Comparison of Theoretical and Measured Signal-toNoise Properties3.9 Conclusions.--4, OTHER CONSIDERATIONS OF DELTA MODULATION-664.1 Introduction4.2 Simple Method of Improving the Performance ofExisting System.4.3 Companded Delta Modulation.4.4 Analogue-to-Digital Converter.4.5 Considerations in Choosing Delta Modulation.4.6 Consideration for Delta Modulation for TelephoneSystems.4.7 Conclusions.APPENDICES79BIBLIOGRAPHY87

SYMBOLS USED IN BLOCK DIAGRAMSTwo Input NOR GateNegation w Pass FilterBlock as labelled

INTRODUCTIONThe purpose of this thesis is to introduce DeltaModulation as an alternative to the more conventional carrierand pulse modulations,Chapter I briefly discusses the carrier and pulsemodulations from the standpoint of signal - to - noise ratio,bandwidth occupancy and threshold effects. In this way, themerits of each is brought to the fore and the superiority ofFM and PCM can he seen.Chapter II introduces Delta Modulation ) a pulse codemodulation ) giving an extensive review of much of the moreprominent literature on the subject. Aspects such as channelcapacity) power, spectral densities, overloading, signal - tonoise ratio and bandwidth ) are discussed.In Chapter III an experimental Delta-Sigma ModulationSystem is described in detail, from design to performance.Observations are made which correspond to some made in theory.The system transmits static signals and AC signals up to 20 HZ.The accuracy is good and the circuits simple.In Chapter IV suggestions are made to improve thesystemis performance by simple means. Also mentioned are moreelaborate means (Continuous Delta Modulation) which enhance theperformance considerably but detract from the simplicity.Much of the literature quoted in the bibliography showsand discusses how delta modulation is simple in circuitry yethas all the advantages of PCM. It is upon this theme that theprototype Delta-Sigma Modulator is designed and built. All thecircuits are kept as simple as possible. With integrated circuits,delta modulation is fast becoming an economical proposition.

Delta modulation, though simple to implement ) requiresgreater bandwidth than the conventional carrier modulationsand PCM (for the same performance). At times this would makeDelta Modulation uneconomical. However, there is a place forDelta Modulation alongside FM and PCM for some particularapplications.

— 3 —CHAPTER ONEINVESTIGATION OF THE CONTINUOUS CARRIER AND PULSE MODULATIONSINTRODUCTIONThe earliest electronic communication systems were thetelegraph and telephone. The telegraph preceded the telephoneand made use of a 'pulse code' known as morse code. At thetime of the telegraph, man was unable to send his own voiceover a transmission line. He could only switch simple on—offsignals onto the line.The next development was the telephone.A microphone(voice to electrical signal transducer) was invented to put thehuman voice on the transmission line. The telegraph and telephonereduced the size of the world by making communications faster andeasier. A demand was created for more telephones and greatertransmission distances.With greater distances, the cost of a single channel pertransmission line becomes large. Hoveover, increased interferenceover greater transmission distances reduces the quality of thetransmitted signal.The signal to be transmitted generally has a small finitebandwidth compared to the channel itself. It is, therefore )wasteful to transmit one signal at a time on the transmissionpath. In order to make full use of the transmission path ) anumber of messages are transmitted simultaneously by one oftwo accepted methods. They are, frequency division, bymodulating subcarriers, and time division, which allows timesharing of the path. In either case modulation of the signalsis required.

4Signals are modulated for a number of reasons. Someare listed below:(1)To multiplex channels.(ii)To shift frequencies to their assigned location.(iii) To increase bandwidth occupancy and transmitted power.(iv)To increase frequency for ease of radiation.(v)To balance bandwidth occupancy and sensitivity to noise.(vi)To translate frequencies for ease in meeting transmissionrequirements.1.1CONTINUOUS CARRIER SYSTEMSThe most widely used modulations are the sinusoidalcarrier modulations. The waveforme(t) A(t) cos (t 42(t))has three parameters which may be varied: A(t) the amplitude,gives rise to amplitude modulation (AN). By varying the phase,( t), gives phase modulation (PM). If the derivative of 4141.(t)with respect to time is allowed to vary, a variation in frequencyoccurs and frequency modulation (FM) is obtained.Frequency modulation is superior to amplitude modulation,the chief reason being in the ability of FM to exchange bandwidthoccupancy in the transmission medium for improved noise performance.fc carrier frequency,fm modulating frequency,W bandwidth.The various continuous carrier and pulse systems areinvestigated in terms of their signal — to — noise ratios atthe outputs of the detect9rs. For a given f m , some systems

require a greater bandwidth than others. The systems areconsidered on the basis of same signal - to - noise ratio atthe input to the detector. The greater the bandwidth, thegreater the noise at the input. Therefore, to give the samesignal - to - noise ratio at the input, different signal powerswould have to be transmitted,If S /N denotes signal - to noise ratio at theo ooutput, and Sin/Nin denotes signal - to - noise ratio at theinput, then for AM double side band (124 - DSB) (1) ,So/No 2 Sin/Nin(1. 1)2f(1.2)and bandwidth, For 114 single sideband (AM - SSB)S o/No Sin/Nin(1.3)f(1 .4)and bandwidth In both cases, the signal-to- ,noise ratio is independentof the bandwidth W and, therefore, cannot be improved by usinga greater bandwidth.For frequency modulation if f d is the maximumfrequency deviation of the carrier, thenfd/fm mfis defined as the modulation index for an FM system. A distinctionis made within the FM system depending upon the value of in f. Formf 0.6 the system is known as wide band FM (WBFM), and m f 0.6is narrow band FM(NBFM).

Evaluation of output signal-to-noise ratio for lowvalues of signal-to-noise ratio is quite difficult, but asimplified analysis (1) for large signal-to-noise ratiosgives some idea of the performance of F.M.For WBFM,So/No finn/Nin(1.5)with bandwidthidizf 2mFor NBFM,(mf ,› 5 )f fmSo/No (1 .6 )(1 . 7 )Sin/Ninwith bandwidth 2f(1 .8)mEquation 1.6 is an approximation, but with equation1.5 a good indication of how bandwidth and signal-to-noiseratio can be exchanged ) is obtained.I comparison between WBFM and kM DSB can be made as-regards signal-to-noise ratio for two cases.(1) Identical total transmitted power(So/No )wum(S o/NdAMr.DSB/)( 1.9)(2) For identical carrier powers(S o/No )WBFM7-070-7-LT-IBIn case (2) for m2 23mf(1 .1 0),1r, the ratio is greater thanone, and an improvement of FM over AM is obtained. The casemf 1/ 3 11.0.6 is the crossover point from NBFM to WBFM.Narrow band FM has no noise advantage over 41\1 for a givencarrier power.

60 -.S.HighresultsWBFM40 Exactanalysis.0 20-SSB0—20 —20—1001030S,11Vw dbFigure 1.1WBFM.Output signal-to-noise ratio versus input signal-to-noise ratio for SSA andWith noiseNoisevoltageNo noiseError dueto noiseDetail of received pulse. (d)Figure1.2Received signals in a PPMsystem.

If fm 15 KC and maximum frequency deviation(fd) is 75 KC (this is usual for commercial broadcasting), then foridentical carrier powers,(S o/No )WBFM(S o/No )LM-DSB 32i152 75This is an improvement of 18.75 db.These results for Fn indicate that, by increasing m f ,unlimited advantage over I114-DSB is achieved for large signal-Ls mf increases, the bandwidth increasesto-noise ratios.and, therefore, there is a corresponding increase in thenoise. It has been shown (1) that the output noise power .foris given by2'17fNo wherePc3Pc carrier power spectral density of the noise (considereduniform over the bandwidth).It can be seen from this expression (equation 1.11)that, for a fixed carrier power P c , the noise power increaseswith the cube of fmfm increases, holding the carrierpower constant, there is a point reached where the noisesuddenly takes over, causing a large reduction in theoutput signal-to-noise ratio. The region where this reductionoccurs is called the threshold.Figure 141 illustrates the performance of FM.and al-SSB. The low value S/N analysis is also shown andclearly illustrates the threshold effect. The carrier-to-noisepower ratio should not be below approximately 9db, this minimumbeing increased to 15 or 16 db if receiver noise is included.Below this 9 to 16 db figure the output signal-to-noise ratiodeteriorates rapidly.

1.2PULSE MODULATIONS1.2.1 PAM, PWM, PPMPAM, PWM and PPM have a carrier of an evenly spacedtrain of pulses, some parameter of which varies according tothe modulation signal. The height width or position of thepulses can be varied. The first is known as pulse amplitudemodulation (PAM), the second as pulse width modulation (PWM),and the third as pulse position modulation PPM. A fourth ispulse code modulation PON. The signal is 'quantized' eachsampling time, and the quantized value represented by a codeof pulses. In all cases, the time function is uniquely determinedby sampling every-1- seconds (sampling theorem(2)).2fliiIf a PAM system is considered where the pulses aretransmitted by AM, then the system (Pi/ii) requires a bandwidthof 2 mfm ) assuming t14-DSB, or mfm for AM,-SSB. the numberof message channels). This is the same band width as ordinaryAM.PWM and PPM are closely related, and their signal-to-noiseproperties are treated simultaneously. Figure (1.2) showsdetails of a received pulse. For a reasonably sharp bandpass characteristic, it can be shown thatw 1/ti.(1 . 12 )t rise timeto maximum displacement of pulse for a sinusoidal inputsignal. In terms of the input signal-to-noise ratio, the outputsignal-to-noise ratio is given by:s002t2 WW33 S.infmN.in(1.13)

Thus, the output signal-to-noise ratio varies as thecubic of W. This is the same functional relationship as forFM (equation 1.5). Ggain these results are only for largesignal to noise ratios at the input.1.1comparison betweenPGM/GM and PPM/GM yields:(S o/No ) PPM/GM(So/No)PGM/GM2- 2 t (W) 2o( 1 .14)W 1/trwhereConsider a time division multiplies system of 50channels. Each source of information has a band-width of 5KC,rise time t is 0.1 tiS, and pulse width 0.10, then themaximum value of to is about 0.95141S. For a PAM/GM system, aband width of 2 x 50 x 5000 500 KC is required. For thePPM/LM system, a bandwidth of approximately1OOHS- 10 MCis required.The improvement of PPM/GM over PLM/GM is 2(0.95) 2 (10) 2 180 or 22.6 db.Gs FM was to GM, so is PPM to PGH, in that this usefulexchange of bandwidth with signal-to-noise ratio can be madefor FM and PPM but not with GM and PIZ. PPM has no greatadvantage over FM and has not been used to the same extentas FM.In both FM and PPM, the improved signal-to-noise ratiois obtained at considerable expense in bandwidth.1.2.2 Pulse Code Modulation (PCM)Pulse code modulation is a very different pulsemodulation. In the previous pulse modulations discussed here,modulation was achieved byvarying one parameter of a standardpulse. In PCM, the continuous time function is sampled in the

10--usual manner, then !quantized'. The signal is transmitted bya code of pulses representing the particular quantized value.The digital code is more favourable because of its simplicityin detection and instrumentation. Usually, the binary digitalcode is employed, that is, 0 or 1 are the only values thesignal can have. This can be achieved by carrier on or offrespectively.Despite the complexity of the mechanism of PCM, thereare many advantages in its use. PCM allows for considerableincrease in signal-to-noise ratio at the receiver. The onlydecision that needs to be made by the receiver is whether thepulse is present or not. The receiver need not know itsamplitude or width. This is one property which other pulsesystems do not possess. Of equal importance, is the fact thatthe encoded signal can be repeated without introducingsignificant distortion.Ls with other pulse modulations, the signal is sampledat the rate of 2 f m Per second. If there are m signals andn digits per code group, the time interval between pulses is1/2mm fn(2)and the minimum bandwidth requirement is 4#*W nrn fm(1.15)The only source of noise is assumed to be the originalIquantizing noise inherent in the modulation. The noiseover the channel is assumed never to cause a pulse to bemisinterpreted. Therefore, any received sample may be inerror by as much as half a quantizing level (V K/2). Thenoiao power, for the maximum error V K/2 in each sample isgiven byN o V2/12 (1)

— 11 —and the signal power,So V2/12 (2 n - 1)The output signal to noise ratio is givenS o/No 2n - 1(1.16)(This is for large signal-to-noise ratios, 710 db).For these large signal to noise ratios,s 0Ar 02.22'(1.17)Equation 1.15 shows bandwidth to be directly proportional ton. Output S/N, however, increases exponentially with n, andhence output S/N increases exponentially with band-width. Thisrate of improvement, with increase in bandwidth, is greater thanthe other pulse systems and FM. (For FM the signal-to-noiseratio increases with W 3 ).Shannon (3)derived a relationship between input andoutput signal-to-noise ratios from information theoryconsiderations based on channel capacity and Hartley's law.The rate at which the channel supplies information for a FCMsystem is given byR 2n W(1 p log p q log q) bits/second (1.18)This rate must be equal to that supplied bk the channel (for noinformation lost), thus giving the output signal to noiseratio as;S/N0o 22n (1 p log p q log q) . 1 where -ai Si n/Nin2 17 0 f exp(-y 2/2)dy where a j41Figure 1.3 shows output versus input signal-to-noise ratiofor n 1, 5, 10. Below 10 db for S 1 /N the output signalto-noise ratio decreases rapidly. Above 10 db, S /N levelso ooff to a constant value.

/140 0Ob)n 106040n 5n 12b-2'041 0?)c)8b3.in (db)N in-20Figure 1.3Figure 1.4OUTPUT VERSUS INPUT S/N FOR PCMCOMPARISON OF VARIOUS SYSTEMS

- 12 This threshold of 10 db for PCM is an improvement onthe 15 to 16 db threshold already described for FM.1.3COMPLRISON OF MODULLTIONSL comparison of the modulation systems discussedhere can be made on a common basis of input signal-to-noiseratio, the noise being contained in the message band widthW.Figure 1.4 shows how various systems compare. Belowthreshold, (i.e. small signal-to-noise ratio) the LIAr-SSB issuperior, in both conservation of band-width and in greatersignal to noise ratio.If the received signal-to-noise ratio is to be large,then a binary PCM system should be used for maximum outputsignal to noise ratio. L better trade off of S/N with bandwidth is achieved.'It becomes increasingly difficult to ensure interferencefree transmission with increasing distances. In moderncontinuous carrier systems, the signal transmitted by cableover a distance of 100 kilometres is attenuated 240 db, thatis a power ratio of 1o 24 times. The attenuation does not,in itself, constitute any difficulty, for it can be compensatedfor by a series of repeaters. Besides the attenuation however,there is interference which is cumulative and is exiplified ateach repeater, thus decreasing the signal to noise ratiofrom repeater to repeater. On the other hand, PCM does notaccumulate interference. The pulses are regenerated at eachrepeater.Llthough PCM should have been used in preference to WBFM,it was not because of the complexity of instrumentation. TheBell Systems Laboratories (and others) have carried out muchresearch into PCM in order to bring it to a stage of development

- 13 such that it be economical to install. PCM is currently inuse in the United States of Lmerica (fairly extensively)and in small installations in Britain and Holland.1.4INTRODUCING DELL:. MODULLTIONSo far there has been no mention of delta modulation(DM). The discussion has gone into the relative merits of themore common methods of continuous carrier modulations, and hasbriefly compared them. Next the pulse modulations wereintroduced and compared with the continuous carrier modulations.PCM has emerged the more favourable as regards performance, butis handicapped by the complexity of instrumentation.Rather than give details of DM here, a few pointswill be stated. These points form a basis on which furtherinvestigation is carried out, and appears in the followingchapters.Delta Modulation is a one-unit binary code. It hasthe same properties as in PCM, in that pulses need only berecognised as present or absent, without concern for shape.Hence, as in PCM, the only noise which is present in DM isquantizing noise. It could be expected to achieve a similarperformance (signal-to-noise ratio) to that of PCM.The main advantage of delta modulation over PCM isthe simplicity of instrumentationDelta modulation uses a principle of quantized feedback, whichresults in extremely simple coding and decoding operations.It is in fact so much simpler that it would be used inpreference to PCM, were it not for a disadvantage in band widthrequirements. It is shown later that delta modulation requiresabout 1 times the band width of PCM for similar performances.

DifferenceCircuitf( t)(a)p(t)BASIC BLOCK DIAGRAM FOR DELTA MODULATIONDemodulatedOutputFigure 2.1BASIC BLOCK DIAGRAM FOR DEMODULATIONP. G.DifferenceCircuitp(t)d( tp(t)(a)BASIC BLOCK DIAGRAM,DELTA—SIGMA MODULATIONp(t)(b)DemodulatedOutputBASIC BLOCK DIAGRAM,DELTA—SIGMA DEMODULATIONFigure 2.2

- 14 -CHAPTER TWOINVESTIGATION OF DELTA MODULATIONINTRODUCTIONThe principles of delta and delta sigma modulationare introduced. Some of the more significant early works ondelta modulation are studied and results pertaining to suchfactors as signal-to-noise ratio, bandwidth, spectral densitiesand power are discussed.The discussions are extensive, and conclusions areachieved which indicate delta modulation to be a suitablemethod of modulation and a competitor with P.C.M.2.1THE PRINCIPLES OF DELT/. AND DELTA-SIGMA MODULATION2.1.1 Delta Modulation (4)The delta modulator is a feedback system (figure 2.1)consisting of a pulse generator (PG), a pulse modulator (PH),a linear network (F) and a difference network.The output pulses p(t) are fed back through the networkF to produce a function g(t) which very closely approximates theinput signal f(t). The difference meter produces the differencef(t) - g(t) d(t) and passes it into tho pulse modulator. Thepulse modulator passes positive pulses from the pulse generatorif f(t) g(t)„ and negative pulses if f(t) (g(t). These pulsesare the modulator output pulses p(t). Each pulse tries toreverse the polarity of the difference signal d(t). By doingthis, the difference between g(t) and the input signal f(t) iskept small. (Essentially,the network F is a low pass filteror an integrator with a large time constant).At the receiving end (figure 2.1(b)), if the pulses p(t)are applied to a similar network to F, an output signal eo(t),

- 15 which is a close approximation to the input f(t), is obtained.The difference between the original input signal f(t) and thereproduced signal e 0 (t) gives rise to the "quantizing noise".This can be reduced by increasing the pulse frequency.2.1.2 Delta-sigma Modulation (5)Delta-sigma modulation is similar to delta modulation,the difference being that the input signal f(t) is first integrated.The integrated difference signalEi(t)is fed to the pulsemodulator. (see figures 2.2(a) and (b)). The same feedbackof the output pulses p(t) applies. In the modulator, theintegrated difference signal E;(t) is compared with a predeterminedreference voltage Va . L. positive pulse is allowed to passfrom the pulse generator if E(t) ) VR , and a negative pulse ifE(t) VR In this way, the integrated difference signal isalways in the vicinity of the reference voltage V R , providedthe input signal does not have too great a slope, or is toolarge.The larger the input signalpthe more frequently do theoutput pulses appear.Demodulation is produced (as with delta modulation) bypassing the received pulses through a low pass filter therebyobtaining a reconstruction of the input signal f(t) I with ofcourse oquantizing noise". The manner in which the quantizingerrors occur determines the signal-to-noise performance thatthe system will attain. Quantization noise for P.C.M . anddelta modulation is discussed in a further section,Ls channel interference will distort the pulses p(t) )they must be rogenera ted in the receiving network before filtering.This has been done in the experimental delta-sigma modulatordescribed in chapter III.

Input1A-2.121.1toyut --InputOultputFigure 2.3 BLOCK DIAGRAM SHOWING SIMILARITY BETWEENDELTA AND DELTA—SIGMA MODULATION0 1 41, Figure 2.4 SINGLE INTEGRATION (deJager)f(t)p(t)e 0 (t)I.IFigure 2.5 STEP WAVEFORM AND INPUT WAVEFORM FORSINGLE INTEGRATION

- 16 2.1.3 Relation Between Delta and Delta-Sigma Modulation.Essentially, a delta-sigma modulator is the same as adelta modulator, except that the input signal f(t) is firstintegrated in the delta sigma case. (see figure 2.3). Inthis way, the delta-sigma modulator carries information accordingto the amplitude of the input signal, as opposed to deltamodulation, where the modulated signal carries informationaccording :to the slope of the input signal.2.2 EARLY WORK BY DEJAGER (4) ON DELTA MODULATIONde Jager l in his paper on delta modulation, as describedin section 2.1.1, considered two cases:(i) When the demodulator is single integration.(ii)When the demodulator is double integration.2.2.1 Single Integration (figure 2.4)The network has a large time constant, and theresponse to an impulse is practically a unit step. Figure 2.5illustrates the input signal f(t), the step curve and thepulse train. The difference between c 0 (t) and f(t) is thequantizing noise."This is audible as a type of noise which is moreor less correlated to the speech. At a pulsefrequency of 40 KC/S the intelligibility ofthe speech is good, but the quantizing noisehas an effect on the speech which may be calledIsandinessf ".Also, when the slope of the input signal reaches acertain limit, an overloading occurs. For a sine wave offrequency f at the input, the maximum amplitude which can

RR21NA/Vs- Figure 2.6 DOUBLE INTEGRATION (deJager)f(t)IFigure 2.7IiIiISLOPE STEPPING DOUBLE INTEGRATION

— 17be transmitted isa 27-r fvKwhere f is the pulse frequency and V K the height of one stepin the approximating function g(t).de Jager also derived an expression for the signal—tonoise ratio in the case of single integration. The result was:3/2fS/N C1 tfIZwhere f o is the cut—off frequency of the low pass filter.2.2.2 Double Integration (figure 2.6)By using a double integration linear network, theapproximating function now increases or decreases by a unitslope instead of a unit step per input pulse. By making bothtime constants large, a unit pulse at the input provides aunit pulse at the first condenser and an output signal ofconstant slope (figure 2.7).It can- be seen by observing figures 2.5 and 2.7, thatdouble integration gives the better approximation to the inputdejager goes a little further and introduces predictionmethods into the- system to give an even better approximation tothe input signal (see reference 26). .The expression for the signal—to—noise ratio for doubleintegration isS/N Gf 5/3/2f foThe improvement in signal—to—noise ratio varies with the 3/2or 5/2 power of fthe clock frequency, for single and doubleintegration respectively. Using the digits of a binary code )it varies exponentially. Values of G i andC1 0.2002 are approximately,0.026.

- 18 -2.2.3 Experimental Workde Jager's experimental measurements of signal-to-noiseratio are shown in figure 19, reference 4.The theureticalcalculations agree fairly well with the measured values, andthe improvement obtained by using double integration is clearlyillustrated.2.2.4 General RemarksdeJager found that a good reproduction of speech ispossible at a pulse frequency of 100 KC/S. Compared with P.C.M.the quality was the same as an eight unit code. In taking 800 C/Sas reference frequency, a signal-to-noise ratio Of 50 db isobserved, while according to a formula by Bennett (6) the signalto-noise ratio in db for a full lead test tone, in using a codeof n digits isD 6 n 3which gives n 8 for d 50 db. In this case, the bandwidthneeded for transmission with delta modulation is about 50%greater than by using P.C.M.Ln experimental system was set up for the high qualityreproduction of music. The bandwidth was extended to 12 KC/S,and the signal-to-noise ratio raised to 67 dip, by increasingthe pulse frequency to 500 KC/S. It was found that the reproductionwas very good, but sometimes difficulties arose when the frequencyspectrum of the music contained much energy at high frequencies.In this case, the level had to be adjusted to draw a compromisebetween the quantizing noise and overmodulation. This impliedthat the method Of single integration at the receiver is notwell suited to music of this kind.

- 19 -dcJager's concluding comment was:it is even possible that in the future the wholesystem can be constructed in a rather inexpensiveway by making use of transistors".This has been done with the use of not only transistors, butintegrated circuits. Chapter III and IV discuss delta anddelta-sigma modulations as an efficient and economical meansof transmission of signals.2.3L REVIEW Of ZETTERBERGIS PLPER "L COMPLRISON BETWEENDELTA LND PULSE CODE MODULLTION (7)"The systems delta and pulse code modulation arecompared from the point of view of information theoryand from the study of the quality of transmission withspeech -like signals.It is shown that the systems have almost the samepotentiality to transmit information when the numberof amplitude levels are the same and reasonably large,more than ten levels. The amplitude distribution ofthe ideal signal for delta modulation implies asignal power about 60 percent less than for thecorresponding signal of pulse code modulation. Thespectral distribution of these signals shows for deltamodulation only, a marked dependence of frequency whichmakes the density decrease with increased frequency.In transmission and reception of speech signalsessentially two errors occur, over-loading andgranulation. When parameters are chosen to givean optimum of quality expressed as signal-to-noiseratio, delta modulation needs a much larger bandwidththan P.C.H. if the desired quality is moderate or high.

— 20 —Delta modulation becomes relatively more favourablewhen the bandwidth of the speech signal is large". (1)It is assumed that the pulses on the transmission channelare of such power that faulty reception of them duo to extensivedisturbances cannot occur. This assumption is justified by thefact that pulse systems operate almost undisturbed when thenoise level on the channel is below a given threshold level,but are completely unusable at a noise level above that value.Zetterbergts methods of analysis are as follows:(i) The discrete case: With certain restrictions onthe source, a rate of information can be definedwhich constitutes a statistical measure of theensemble of messages transmitted. The greatestvalue of the information rate is named "channelcapacity", and the corresponding ensemble iscalled optimal. He determines the statisticalcharacteristics for the optimum message ensemblefrom which the amplitude, power and spectralcharacteristics have been calculated for P.C.M.and delta modulation.(ii)Continuous Signal: A common measure of the qualityof transmission is used. This is called signalto—noise ratio. In the examination of transmissionquality, it has been assumed that the ensemble ofmessages has been generated by a stochasticnormal process, with the energy lying within adetermined frequency range f l to f2 1 and witha comparatively arbitrary distribution in thisrange.

fP.C.M.bits.„ ",.----ir 71. t0I0. e D. M.0.515

2,1 The Principles of Delta and Delta-Sigma Modulation. 2.2 Early work by de Jager on Delta Modulation. 2.3 A Review of Zetterbergis paper "A Comparison. Between Delta and Pulse Code Modulation". 2.4 Delta-Sigma Modulation. 2.5 Thermal Noise Considerations. 2.6 The Problem of Obtaining Output Spectrum of a Delta Modulator in Terms of the Input .

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