INTRODUCnON TO PAR IN LINEAR NETWORKS HUGO VIFIA~ 1400 FOUNTAIN GROVE PARKWAY SANTA ROSA, CALIFORNIA 95404 iI HEWLETT PACKARD www.HPARCHIVE.com OBJECTIVES "EXPLAIN" HOW ANETWORK MODIFIES A BlGNAI. WHAT PARAMETEM GENERATE DISTORTION HOW TO MINIMIZE THEIR EFFECT FIGURE OF MERIT OF A SYSTEM FIDELITY WITH WHICH A SIGNAL OR INFORMATION IS TRANSMITTED OR REPRODUCED. DEVIATIONS FROM PERFECT TRANSMISSION: HARMONIC DISTORTION CROSSTALK, INTERFERENCE ERROR RATE, f¥N- DEGRADATION 1 www.HPARCHIVE.com DISTORTION IS DUE TO ONE OR MORE OF THE BASIC NETWORK CHARACTERISTICS CD 0 0 LEVEL TIME DEPENDING DEPENDING FREQUENCY DEPENDING "'---....y '--------..y--------/ NON LINEAR 1 LINEAR TIME VARIANT TIME IttJVARIANT EFFECTS: NEW SIGNAL COMPONENTS ARE GENERATED 51GNAL COMPONENTS ARE MODIFIED? LINEAR NETWORKS I INPUT f(t) OUTPUT 0 > - - - - -..... e--_L1_N_EA_R_ _ _ IF fi(t) -. f Z (t) -. NETWORK r-------0 9 (t) LINEAR 91(t) } 9z (t) THEN al f l(t)+a Zf Z (t)'" a191(t)+aZ9z(t) SUPERPOSITION APPLIES jwt FOR A SINUSOIDAL INPUT FUNCTION f(t) = eTHE STEADY STATE OUTPUT FUNCTION get) IS GIVEN By THE TRANSFER FUNCTION H(jw) MULTIPLIED BY THE INPUT FUNCTION e-Jwt: - 11(" ) 9 (t) - M -jwt -_ At) -j0(w) -jwt _ A( ) -j[wt+0(W)] ~w· e .e OJ e JW . e ~'---v--J AMPLITUDE PHASE CHARACTERISTIC CHARACTERISTIC Gejw)= H(jw)· F(jw) get) = h(t) f(t) * 2 www.HPARCHIVE.com LINEAR NETWORKS "-----+------,-----1.- t TIME '-+----+-------,----1.- 9 H<jw) p'" TIME t f<¢i<>n) G~w) F{jw) A(wn) -----_: ,, I --------l-------JL-- Wn A(w n) ....,~ I w: FREQUENCY wn ",,(w n) I • W wn FREQUENCY DOES A LINEAR NETWORK IMPLY NO DISTORTION? YES FOR CW SIGNALS, HOWEVER ... MAGNITUDE VARIATIONS WITH FREQUENCY f(t)= sinwt +~sin 3wt +ksinsUlt F{jW) H{jW) .!. 3 1} 1 I 3" -5 1 5 FREQUENCY FREQUE~CY 3 www.HPARCHIVE.com FREQUENCY PHASE VARIATIONS WITH FREQUENCY f(t)=sinwt + ~Sin 3wt + kSin Swt A(w) w C E :z f---.------ '-' ~ F(j(l,) lZl(WL)~---;F~R::;:EQ~UC=EN:-:-:C::-y:-----1~ G(juJ) o f---.-::;---,FR,+,-,E~QT"'IU:=E:..:.Nc=.:y'-------1~ 0 I I -180 : I I I "3 5 I 5 I I I o FREQUENCY 3 FREQUENCY _ISO° DI6TORTIONLESS TRANSMISSION get) =Af(t-to ) f(t) H ideaI 0 A+-----,~-----, to 4 www.HPARCHIVE.com I t IDEAL TRANSFER CHARACTERISTIC A(w) h r----I I I I 0 I A(w) = CONST=A - - - - - - - - - - - - . - ,- - - - - - , I r I I r I I I wIc I ! -liw ¢(w) +liw .-w r-_ I I --_ : -- : -.. -.... ~--_ -liw We, +Aw ---+----='""+-<::::-----i-'---=---..:-----,---+----.----- W l ~-.. I -0 ----_ ¢o=± n7r -- -- __(t()) --- . . -J -.. --""""'.........: --- I --~ __ - -..: ~ ~4J.,.__0 I ---_ I I - - -----N I ---. __ I -_ I -I... I I --J CRITERIA FOR DISTORTJONLESS TRANSMISSION OVER LIMITED BANDWIDTH A(w) NETWORK TRANSFER FUNCTIONS 1. A MAGNITUDE BANDPA5S FILTER CONSTANT AMPLITUDE OVER BANDWIDTH OF INTEREST A(w) = A = CO~STANT '--------'----'------__ w </J(w) - BW -- FREQUENCY -. BW -- FREQUENCY 2. LINEAR PHASE OVER BANDWIDTH OF INTEREST '/J(w) = -wto = L1~EAR WITH w PHASE to = PROPAGATION DELAY OF AN IDEAL NETWORK 5 www.HPARCHIVE.com NON IDEAL TRANSFER CHARACTERISTIC A ideal A(w) j .~ ," " "I I ,,' I I t \ ' ,, .. -AW We tAw M(w) -AW , We., tAw I' , , :,, , I I II , =canst; ' ... , w ,, , +Aw ¢(w) -AW I<:-',---t-,--+,- I - ,- +Aw ":~ I I We. 1.1) ~P'.:" ,\Q ................ t:.¢(w) -110-\1 <Ds: Al( w ~-___ Cause: l::!.A, A(3-calculation ofeffec.ts on Signals IDEAL AND NON-IDEAL PART OF A NETWORK f(t)o H (jw) = = Hi ~r I I • JI---T- 6H 0. ± A· e- jwto• '-y--1 g(f) , Hi (j w) • Hn'j (jw) t - jwt ~ ! H(iw) I• I )LHid~/IHncn-idealll = ±Aoe = Hejw) fp(t) =Aof(t-to? (1+L\A(w))e [1 +LIA (w) - jl::!.¢(w) ~<)l(w) + J: l> ¢(w) + -- -] [1 +AA(w) - jA0Cw) + 0 \ •• ° higher order terms] Y Hni (jw)or~H(jw) Hi (jw) 6 www.HPARCHIVE.com J APPROXIMAnONS FOR 4AC/I1) & A~(C&I): CD EXAMPLE: ® 6.A = an COS n~w for -b..wL w< + 6.w FOURIER EXPANSION: n~ ~~(w) = ~ b..A(w) = , an'COS bn·sin 6.A n~w n~w ~ (t) = ~-1Fo(jW{1 + aln e jn't'lil+a; \~ t- 2'11 of ripple number ~l/.) periods overAw ?(llJ :.Shift Theorem:~n~I-.±n~1 w Jt fo(t+nl.') g (t)= fo(t)+a2n fo(t-n~)+an 2 Result: Echoes for discrete signals : 1- l an o f--~---+-I--~--+-----lT iii.t~~ iI\' to l ._, \ ~ ~¢ = -b n sin n?!w:. @ v l • ~ '-~ 2 Discrete Signals CALCULATE EFFECT OF 6.A, b..¢ ON SIGNA.L f(t) .... g(t) SIGNAL DISPERSION DUE TO ANON IDEAL AMPLITUDE AND PHASE CHARACTERISTIC f(t) Hideal i r-- 111 ~II~~}~ ~(i:¢i":" -" i ~ Ht-to) -Ito 1- H _ ° t::.rl. +.E.'P -=1'= +& get) t V I \lllllI=r~ 9b _t!lIIii b ~:su't 2: nr nT + ~igher order terms 7 www.HPARCHIVE.com 0 EFFECTS OF ECHOS ON DISCREET SIGNALS CROSSTALK ERROR, CROSSTALK TI-1RESHOLD - ~ - - ---.!. ~ 1 1 I I I TDM - CHANNELS I I I GUARD ~~~ _1_0~1~\_1.-1.I II I~' \ I I ~I ,\ I I I BANDS I --I 1 1..1/ " --l""'-------O>+---Lt-----f'"'""L~-~~---_t__'''''4_---->O'__._ 2 1 1\,3/" I 1 ,_/ + 4 @: 1 dB ripple generates echoes only ~ ZO dB down RISE TIME DEGRA.Di\TION -0---' I /1 1 1 1 I 1 I 1 1 I ....-!-:"---+---"'--I------,1--.... + ~tr~ : ~ --2.n?;'~ ; HOW CAN DISTORTION BE MINIMIZED? 1. MEASURE I:1A, /:).0, (r*) 2. EQUALIZE/MINIMIZE I:1H EXAMPLE: GAIN (AMPLITUDE) AND PHASE EQUALIZING A(w) ¢lW) ... w INCOt-iVEt-iIENT 10 ADJUST TO ASLOPED REFERENCE ... '" '---------- DELAY EQUALIZER /--- - --..., * MISMl\lQ.1 AND MULll PATH TRANSMISSION / MUCH EA51ER TO ADJUST TO A CONSTt\NT (GROUP DELA'() " '--------~l.U 8 www.HPARCHIVE.com REFERENCE. TWO ASPECTS OF GROUP DELAY ® CD SIGNAL PROPAGATION t9 =- SIGNAL DISTORTION d0(w) = t + d[a0(w)] dw ~ , dw , constant' deviation' .....AQI d0 dw ideal THE GROUP DELAY - ~~ non ideal TIlE DERIVATIVE OF THE DETERMINES THE PROPAGATION PHASE CHARACTERISTIC CAN DELAY OF SIGNAL ENERGY OR BE USED TO SPECIFY AND MEASURE THE DEVIATiON INFORMATION (ENVELOPE DELAY). FROM THE IDEAL (LINEAR) THE PHASE DELAY - ~ PHASE CHARACTERISTIC. IT IS A PHASE LINEARITY DETERMINES THE STEADY STATE PHASE RELATIONSHIP MEASUREMENT. ONLY THE B~TWEEN INPUT AND OUTPUT (CARRIER DEVIATiON FROM THE CONSTANT DELAY) FOR AN IDEAL NETWORK (GROUP DELAY) IS IMPORTANT t9 = tp. IN THIS CASE. PROPAGATION DELAY AND ELECTRICAL LENGTH FOR AN IDEAL PHASE CNARACTEIlISTIC f(t,n, g(t, [) t =ELECTRlCAl LEII6TH .--+~---J'----'o.--....- t ~>~-t to=i= -~ in vacuum r 0 C w dw '-y---l '--y-/ d0 t o = -=--=-'--y-/ PROPAGATION DELAY PHASE DELAY GROUP DELAY 9 www.HPARCHIVE.com PHAgE DELAY AND GROUP DELAY ENVELOPE get) = e(t-tg ) CA.RRIER COS [We (t-tp)] g(t) ¢(w) CARRIER: tp(Ul) =_ 0~(JJ) r-------,- w t CARRIER 1WIIII1fI-- t , -1 ENVELOPE: t (w) g = _ d dw (2\ (w) PROPAGATION DELAY FOR A NON IDEAL PHASE CHARACTERISTIC _(1M) ~ 1M eI,C"" CIiU f(t) ~---.-='+---_W tc. :; tg (0) LP =t (We) BP W-- 10 www.HPARCHIVE.com DISTORTION EFFECTS ON MODULATED SlGNALS~ CD TIME DOMAIt-J MODULATION: (PULSE MODULATION) INFORMATIOt-J It-J SIGt-JAL AMPLITUDE AND TIME: . } {DISCRETE SIGNALS: f(t) = 1· -M <t<M ... FOURIERAPPROACHFORAH { 0: t> IMI ECHO DISTORTION ~t -Lh. ® FREQUEt-JCY DOMAIN MODULATION: (CARRIER MODULATiON) INFORMATION IN CARRIER AMPLITUDE/ANGLE (ENVELOPE) w -"t ENVELOPE f(t) = CARRIER [1+o«t)].e- ~t AM} CONTINUOUS SIGt-IALS: jwct POWER SERIES APPROACH "'t . r. f(t) = e - JLLlJct~t) CARRIER ] Ir:::. PM/.M ENVELOPE DISTORTION / z:.... ID1DDrzl:1[]'jLt 11 ENVELOPE ~ SJGNAL DISTORTION DUE TO LINEAR BUT FREQUENCY DEPENDING TRANSFER CHARACTERISTIC t·_·,. - '., AM DI5TORTION T .... -, ? €. " .... _L..--..L----'----_ _ °9 LPF "'--~ ----------------- .... .... ---..t.. . USB ATTENUATED: ..... W ,.:'). ~!1. -- -- -1-------------1..1 /-' ,.,. I '\.~~~l . " \ EFFECT: , , :~ CHANGE OF INDEX MODULATION (m) ODD HARMONIC DISTORTION OF ENVELOPE FOR SMALL INDEX m. .;:,': " AM TO PM CONVERSION f 11 www.HPARCHIVE.com APPROXIMATIONS FOR AA(cu) & 11~(JAJ) ® POWER EXAMPLE: SERIES EXPANSION =a 1 w+a 2 w2. M(w) = a1 W+ a2. <.02.+ a~ <.0 3 + . ~A /::"(/)(w) = b o + b2. <.02. + b 3 <.0 3 + . g(t) = 3'-1 Fo(jw)· [1+a l W+ a2.w2.J :. DIFFERENTIATION THEOREM a 1 ·w -a'f(t) a2. £.02. - a1 f (t) get) = fO(t)+alfo(t)+a2.fJt) RESULT: TABLE FOR BASIC SIGNALS: AM-f(t) = Re [1+'" (t)] e -jwctJ 'fM-f (t) = Re [e -j [Wet t f(t>] ] T MODULATED SIGNALS -6w We I 8(t) = 3'-Fo (jw)' [lMA- tAW jMT:JJ CA1.CULA1E EFFECT OF l:>.A, 6.~ ON get) DISTORTION ON AM-SIGNALS .r [Q(t)]] f(t)=R [l+d(t)]e-jWct o-@-og(t)= Re e ~to«t)+P(t~2.+Q(tl.e -JLWcttarctg 1 to«t) + P(t) t:.A(w) = a1wtd1.w2ta3w3 l:>A(w) = b 2 w 2 +b 3 w3 / . "1(t) <1>1 / / / ,, r1 TABLE 1 0( PlJREAM 'f= CO~T. 81 82 P", Q", a1~ -a 20( a3 b2 f(t) 1 (t) b3 al b2 83« b3 « -b 2 0( 8 1b2.« EXAMPLE: o«t)= m cos W m t 0< = -m,wm sin Wmt gUadrature Phase 0< = -m wm2. cos wm t In Phase Quadrature Phase 0( = mw 3m sin wm t 12 www.HPARCHIVE.com AM·SIGNAL9~ DISTORTION ON CD EXAMPLE: USB ATTENUATED BY E J DISTORTION ON AM-SIGNALS: Dl~O P(t) r ENVELOPE p (t) -- 0 • t i "< b,L~--~"--------T--~ r(t)] r ~ Q(t) Q(t)=at 0 Q(t) (t) ~ i+offiV .......... ~~~=.y.-----""""-J"'--'_. 13 www.HPARCHIVE.com t ""'---/ t EXAMPLE FOR AM TO PM CONVERSION COLOR TV SIGNAL: BRIGHT ---tUNE ~/ , 'f- ~OC- DARK .. COLOR SATURATION PROBLEM: COLOR CHANGE AS A FUNCTION OF BRIGHTNESS DISTORTION ON ANGULAR MODULATION e[e-j E-uct+r(t>J] ~ get) = ReV[l+PCt~\Q(tre -jrct+rCt>tarct9 ~~J] f(t) =R D.A(w) = a 1 w ta zw Z+a 3 w.3 !::o.t/J(W)= b 2 w Z + b 3 w 3 'f (t) PURE 'fM o<=COIlST.= 1 ~---I a1 az I I \ I \.... -- 83 I bz I CARRIER '. ba \ f(t) a 1 b Z. P Q r a1r a2'f'Z .! ... 8 3(T -T) bzt .,. 3b3 Tr 3a1bz ~" I r ~,\ \ \ \ i -azi - 3a3 ·z bz'r tr " ~--r- rr '3 '" ~(i -'3'r> 81 bz(r-T ;l;Q'f: ','; I---i. " ' , P(t) I / ~ \. i I I ,~fCt) CARRIER\ \ ,\ ~f>.Y' "I .\ , ': 1 ) 9(t) EXAMPLE: ret): mcoswmt r r i =-mw m Sinwmt 'f2=m1.~mlCOS2wmt+l] = -m wh, COS wm t = m wtr, sin tum t 14 www.HPARCHIVE.com r3=m:lIlf[sin~wmt-35inwmt] DISTORTION 011_ MODULATION CD EXAMPLE: PM - SIGNAL b.C/J = b 2 w 2 f~liIIaI !::J.A=o A(/J ~W -AW We. iittl~ ---- A,W Fr i P(t) bz ~ r- elminate by limiting""'= HARMON Ie DISTORTION: @:W m =2'1f'10K"z" b2.= O.5deg .. ~2! 1 % +-------" , m»z :, , , ,, \ 15 www.HPARCHIVE.com DISTORT. . . . . MODULATION A H <jU)) MODULATOR ~~OD. f: <t) ~@--O . Pv ORIGINAL DISTORTED FM-ENVELOPE FM-ENVELoPE fe~(t) e , : ;ru ~ ru ll::, ru ~ t" We Feejw) DEMODULATOR :\ . \ -AU) ~en ge<t;-r;eW tg ~ . '----------1:----...'" . to l4r t GeejUl) --i--'-- ~w ~~ ge'it) Wuru EXAMPLE: HARMONIC DISTORnON =3oonsl @:/::,t 9 W m ~ 2 7r. 10 kHz d Z == 1% - . SECOND HARMONIC DIGroRTlQN WJ.lAT HAPPENS WWEN MORE THAN ONE SIGNAL IS PRESENT: f(t) = e -j [Wet + T1 (t) + i 2 (t)J-+ g (t) = TABLE a3 P r 1 I I a3[t~-fJ I - r t:. ('f2.):::: Q 1('('2) = DIFFERENTIAL PHASE /t:.T/(T2.)::::P1(Iz) = DIFFERENTiAl GAIN 16 www.HPARCHIVE.com V(1 +p)2+ Q2. e- .... arct91~p Qr -3a 3 rr SUMMARY AND CONCLUSIONS DISTORTION EFFECTS ON MODULATED SIGNALS: • CHANGE OF INDEX MODULATION -- CHANGE IN BRIGHTNESS (TV) OR LOUDNESS VS. FREQUEt.JCY • NON-LINEAR ENVELOPE DISTORTION -- HARMONIC DISTORTION • MODULATION CONVERSION (AM TO PM) -- COLOR CHAt.JGE VS. It.JTENSITY, CROSSTALK) ETC. • INTERMODULATION: DIFFERENTIAL GAIN At.JD PHASE -- MORE THAN ONE SIGNAL COMPONENT PRESENT RESPONSIBLE PARAMETERS: • L\A(W), L\lZ>(W) OR ~tg(W) MEASUREMENT PRINCIPLES FOR ~ 4A,4~ & ~t9 ® SEPARATION BY SUBSTITUTION @ SEPARATION BY DIFFERENTIATION "~(w) =I~O + ~~o~)}~~~ t:.A(w) = A(w)-~o dA dw SUBSTITUTED CONSTANT + d [bACw)] ~ AMPLITUDE LINEARITY SUBSTITUTED LINEAR TERM t:.(/J(W) =0 -d0 = d [L\0(W)] + t 0 dw dw + = ~(W)- £..Oto ~ PHASE LINEARITY SUBSTITUTED CONSTANT ~tg(W) = ~ -d[Ml>(w)] = t (W)-t =b.t dw 9 0 9 tg(W)- to 17 www.HPARCHIVE.com @ 414. A(/J MEASUREMENT BY SUBSTITUTION ~A(w) CD = A(w) - A o t.A(w) A(w) liA =DEVIATlON FI«lM CONgfAHT AMPLITUDE EXPANDED f----'---+--f----+-+---'I..--+w LL-------------'+w ~(/)(W) ¢(w) = ¢(W)-wto Ml(w) ® 1<::-----------1.0 .----- IE-,---.....-----I------\--+---+--W MEMUIIEMBIf EMMPLE • DEVIATION FROM LINEAR PHASE MAGNITUDE AND PHASE CHARACTERISTIC OF BAND PASS FILTER A = 5dB/div (top) (/) = 9O o/div (bottom) /).A = 1 dB/div (top) = 10o /div (bottom) J., = 4.2 m M/J J.=O CW = 1.1 GHz CW = 1.1 GHz ±l\F = 50 MHz. ±l\F = 50 MHz 18 www.HPARCHIVE.com (j) 'A, A0 MEASUREMENT BY DJFFERENTIATJON dA(w) dW A(w) CD L..-L------------'-+w _ d0(w) Q!(w) dw ® ""=:----------w • (,of f--------------'+w o DIFFERENTIATION PROCESS: Analog, Numerical,Modulation AA, 4(/J MEA9UREMENT BY DJFFERENTIATION dA(w) A(w) dw AMPliTUDE LINEARITY dA = 0+ d[AA(w)] dw dw -.---+l-----L....L.---.L...L u.> d0(w) -de;) PHMoE LINEARITY OR GROUP DELAY 1---+---1------W df) _ dOl _ t lw) _ t· + d [A o (w)] dw- g~ - 0 '---------'----w 19 www.HPARCHIVE.com GROUP DELAY AS DISTORTION PARAMETER CRITERIA FOR DISTORTION LESS TRANSMISSION: H ideal = <A(W) = A = constant <;Zl(w) =wto = linear with w 1 NECESSARY CONDITION: (SUFFICIENT IF ~w «1 ~ NARROW BAND) d~(w) dw b.H _ <:A(W) non ideal- = to = canst . Ao =AA(w) (Zl(w) - wt = 6.C/J (w) ~ 0 - At ( )_ -d[~0(W)] t 9 () W - t0 - u 9 W dw GROUP DELAY MEASUREMENT PRINCIPLES: t g (w)= - d0(w) BY DEFINITiON dw ¢(W) FREQUENCY 1.------------- W , tg(W) DEVIATION FROM CONSTA.NT GROUP DELAY GROUP DELAY I A0 • L-- - - ' -_ _ W FREQUENCY ® DIFFERENTIATION DEVIATION FROM CONSTANT GROUP DELAY INDICATES DISTORTiON ~ ENVELOPE DELAY TOTAL DELAY INDICATES TRANSIT TIME 20 www.HPARCHIVE.com DIFFERENTIATION TECHNIQUES FOR GROUP DELAY MEASUREMENTS ® NUMERICAL DIFFERENTIATiON tg(w)=_d(2l(W) dw ¢(w) = -lim ~0 =-lim 01-0 1 ... W AW.O W2-Wl AW.o W APERTURE 21 www.HPARCHIVE.com GROUP DELAY RESOLUTION AS A FUNCTION OF APERTURE AND PHASE RESOLUTION GROUP DELAY RESOLUTION 100 n5 10 ns 1 ns - PHASE DETECTOR RESOLUTION 0.1 ns 2.78 kHz 27.8 278 kHz kHz 2.78 MHz 27.8 MHz FREQUENCY APERTURE (Af) EFFECTS OF INCREASING APERTURE b.f= 200kHz IH=ZO kHz. ~ --a s: Q --~ ~ ~ <Il ~ 9 ~ ~ ~ ~ ::> 0 ~ \!) I>l ~ FREQUENCY- FREQUENCY f'I.IASE ¢ FREQUENCY- PHASE. III -.lAf f+I i ____ li.rI I REDUCE. NOISE I I I I (LARGER SIN) 1----t - -I A 9 - 360° li-f 22 www.HPARCHIVE.com LIMITATION DUE TO MEASUREMENT APERTURES l:::.tg(w) W 1-----'\----F--+--~--_7I_____+-- --I~w ... I.~--Wp~--~I l:::.w p Wo e = 1 - COS oc: = 1 - cos _6._00 2wp V II1I GROllP DELAY ERROR DUE / TO MEASUI1:EMENT APEImlRE 10 I 14.3== I EXAMPlE: WI' = 27l'· 1 MHz. min I:J,w =211'·100 kHz ma)l. e =5% IJ I 1 IJ 4.5 I I I VAWI' [%1 = 0.1 7 1 1.42 Aperture .100RIpple Period W '1 I I I IIII 10 I 20 23 www.HPARCHIVE.com ~w [%] p NOISE LIMITATIONS GROUP DELAY MEASUREMENTS NOISE ~;;<_ VECTOR ,\ / / I SIGNAL/NOISE (FOR A GIVEN \ J A¢ BI>.NDWIDTH) I / Atg * / 80dB ±O.OOGo ±0.06ns SIGNAL * CAUSES OF NOISE SOURCE RESIDUAL FM D.UT NOISE FIGURE PHASE DETECTOR NOISE 60dB ±O.OGo ±O.6ns 40dB ±O.Go ±G.ons 20dB ±G.Oo ±GO.Ons FOR l:i.f = 278 KHz. -I A¢ WI-lERE t g = 3GOo' .6. f NOTE: AS l1f - 0, THE SIGNAL/NOISE - 0 dB SIGNAL TO NOISE DEGRADAnON DUE TO DIFFERENTIATION f(t) 1'---\.-----1---\------,t------t N(t) Sew) set) r~~bf----'W 2 Ws BW 2 Sill f(t) =set) t T N(t) @: f(t) = lsi sin wst + n~ I Nnl sin sw -7 df dt ~ wn t = Wsisl cos wst + n± Wn INn! cos wnt 1'\11 T 24 www.HPARCHIVE.com LIMITATIONS DUE TO THE DIFFERENTIATION PROCESS SiN for~t9 SiN for~0 GROUP DELAY AND DEVIATION FROM UNEAR PHASE FOR THE SAME SIGNAL TO NOISE RAno [:€VIATION FROM W.lEAR PHASE: ~¢: 10 deS/div GROUP DELAY Atg: SOn6/div Aperture: 200 kHz. I~""'" CWo 70MHz 5MHL ±~F: 25 www.HPARCHIVE.com NOISE REDUCTlON USING SI6NAL AVERAGING r- -, 1 I I I I + [JZEJ (I/N)SN NEW OO~ (NOT DISPlAYED) I I(H/N)I {H/N)I\N-\ LASf SfORED AVERAGE (DISPLAYED) AN NEW STORED A'IERAGE (MEW OISPLA'O _ : _MElT LIMITATJONe IN GROUP DlLAY S APERTURE: MEASUREMENT APERTURE DUE TO t:.w NOISE: 6/N RATIO IN SOURCE, RECEIVER, DEVICE, ETC. HARDWARE LIMITATIONS: DETECTOR RESOLUTION, SOURCE RESOLUTION, ETC. PRINCIPLE RELATED LIMITATIONS: DIFFERENTIATION, NON LINEAR DISTORTION HOW DOES ~ t 9 COMPARE TO ~¢ t::.¢: WHEN EVER POSSIBLE SINCE IT HAS MUCH LESS AMBI6UETY. ~t9: 5/N CAN BE IMPROVED BY AVERAGING. 26 www.HPARCHIVE.com RELATIONSHIP BETWEEN DISPERSION AND GROUP DELAY DEYIATIONS A¢ .-.t =:::.wT lb -w~ ( ~2b n=1 ~lb AAAAfj4b 11(/J(w) =-b·sin(nTlO) I1tg (w) =nTb·cos(nTw) CONVERSION TABLE :t DEVIATION FROM to CONST~N1 GROUP DEL~Y t>. tg (W) .. t>.lll(W):: - -III 0 Jt.tg(w)dw -tW f-----+--------1 ~ -loll DEVI~TION fROM LINEAR PHASE t>.~(W) 0 ~ }Co }- 27 www.HPARCHIVE.com 2C o CONVERSION TABLE:It DEVIATION FROM DEVIATION FROM TO LINEAR PHASE - CONSTANT GROUP DELAY Mg (w) = ~~ [Ml(w)] -00 .. 6 -w A¢(W)=-b,W tW Atg(W)=b. {(J 1- b, 1- b2 M/J (w) =-b2w2 A¢(w) = -b3W~ !-b 3 A¢(W) = -b4 W4 a) LINEAR DELAY GIVEN SPEC: Atg ..:::: ins OVER 1MHz ~}2ns ~c-~ -w ~w 1 MHz. WHAT DEVIATION FROM LINEAR PHASE CAN WE SPECIFY? SOLUTION: NEW SPEC: STEP 1: WHAT IS THE NORMALIZED GROUP DELAY FUNCTION? Atg(tu) =C1W STEP 2: WHAT IS THE CORRESPONDIN6 PHASE CHARACTERISTIC? li¢(w) =~C1W2. STEP 3: CALCULATE C1 FROM SPEC. AND SUBSTITUTE IN Ml>(w) 11 t C1=~ [sl =[r~dJ STEP 4: SUBSTlTUOE NUMERiCAl VALUES AND SOLVE FOR u-adJor[degJ 2- -Mg·oo li""w)-:!' !!.s·w ¥'\' - 2. W Z. 28 www.HPARCHIVE.com f:,.¢ (rad) = -3 -lns·21T·1MHz==21T·.1O [rad] A¢ (deg) = ~. ~!&(rad) == o.3G@egloverlMHz CONT: CONVERSIONS 6 tg (10) --+ 6~(w) b) PARABOLIC DELAY SPEC: Atg(W) " /1}10nS ~+w -w '----r--' 1 MHz. SAME STEPS MIN EXAMPLE a): 1. ,6.tg(w)= czw z 2. A(/J(w) = -1 C ZW -1 3. A(/J(W) = "3. ~ti"l 1.20 3 ~.(.IJ {h/).¢(W) +w 3 -1 =:3Mg·w z 4. A¢[rdd]= 2;·10- [rad]=U[deg] 29 www.HPARCHIVE.com we -w '-v-------' 1 MHz. HEWLETT'ft PACKARD PRINTED IN U.S.A. www.HPARCHIVE.com