Aa`ff  U0p0@  @p@ 0p     HH $ d HHHH̀̀̀ff@  d Footnote TableFootnote**. . / - :;,.!?-3  ^,8 i{TOCHeading seamlessly    EquationVariables[6"oB G L SW[_dinqr}x!$(+-/13579;=?  3AFH"J(L-N1P6R<T BWGYK[M\T^]accieqgwix*,-/2468:<ACEGIKMOQSTWY[#]-_8cKfPh 90774: Equation: (3) 53385: Equation: (1) 22012: Equation: (5)* 18447: Equation: (7) C"J=90774: Equation: (3)C"J=53385: Equation: (1)C"J=22012: Equation: (5)C"J=90774: Equation: (3)C"J=22012: Equation: (5)C"J=18447: Equation: (7)C"J=90774: Equation: (3)C"J= 22012: Equation: (5)<$lastpagenum><$monthname> <$daynum>, <$year>"<$monthnum>/<$daynum>/<$shortyear>;<$monthname> <$daynum>, <$year> <$hour>:<$minute00> <$ampm>"<$monthnum>/<$daynum>/<$shortyear><$monthname> <$daynum>, <$year>"<$monthnum>/<$daynum>/<$shortyear> <$fullfilename> <$filename> <$paratext[Title]> <$paratext[Heading]> <$curpagenum> <$marker1> <$marker2> (Continued)+ (Sheet <$tblsheetnum> of <$tblsheetcount>)Number in Parens(<$paranumonly>)Pagepage<$pagenum>Heading & Page <$paratext> on page<$pagenum>See Heading & Page%See <$paratext> on page<$pagenum>. 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'''''''''''(20)(21)'''(22)''' ''(23)(24)(BG(25)L(26)!!!%%%%& %! !"!$%&%(%*%,%.%I%K%M%O%Q%S%U%W%Y%[%]%_%a% c%e%g%i%k%!!!!%%%%%%%%!!!%%%%%%!!!!%%%%% %%%% %'%%)%%/%%2%4%6%8%:%<%[%%@%B%D%F%H%J%L%I%%P%R%T%V%X%Z%\%7%%`%b%d%f%h%9%%;%%y%%K%%M%%%%]%%_%%%%!!!%%%%%%!!!!!%%%%%%%%%%%%%%%%%%% %"%$%&%(%*%,%.%0%2%4%6%8%:%<%>%@%B%D%F%H%J%L%N%P%R%T%V%X%Z%\%^%`%b%d%f%h%j%l%n%p%r%t%v%x%z%|%~%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % %%%%%%%%%% %"%$%&%(%*%,%.%0%2%4%6%?%%A%%c%%e%%%%%%+%%-%%%%%%)%%(%I'hdkpdqs m| m||'graphicsdsp1FrameHeader.eps0001FRAMEPSFMACP0001H$ko!  vy,i@ vy,ivy,i<'equal[times[char[x],id[char[t]]],times[over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[(*n*)times[char[X],id[times[char[j],char[Omega]]],indexes[1,0,char[e],times[char[j],char[Omega],char[t]]]],minus[char[infty]],char[infty]],char[d],char[t]]]d ? HHˆ @ HHˆ‚&HF͒F h " )qA (uNote that the complex exponential # in Eq. %3$ has the same role as the complex exponential ' in Eq. &>VQ HZ)1(. Now lets consider the expression + for the frequencies , and -: w% h. @% (oIn other words, the discrete-time frequency variable is periodic with period /. As a result, we only evalu% jate the IDTFT computation over a frequency region that is arbitrary but of extent 0: This periodicity Scx@@occurs because the time variable  n l is always integer. ②,l h *1 ScQ xwhere the single subscript on the integral sign indicates that integration can be performed over  any l strip of @ H`2 of extent 3. This occurs because the entire integrand of Eq. 554 is periodic. Sc8h^The validity of Eqs. 7(3)6 and 9(5)8 can be confirmed by simple substitution: ԓ5 2 h; F͒a h :< @_v (Because  n l and  l l are always integers, the integral in Eq.  >(7)= l is equal to @ when A and zero otherwise. _v iHence the only nonzero term in the outer sum occurs when B, and it evaluates to C. This confirms ScH?that Eqs. D(3)? and F(5)E are transform pairs. UT[/`Basic DTFT examples Scۉ,`EThe decaying exponential.  lWe first consider the simple function !)q hH "Sc Y`Substituting directly produces #F͒* hI  ScP `bAs shown in class, the real and imaginary parts can be obtained by rationalizing the denominator: ]$ԓ5n hJ HHˆ BHHˆtE l~sxy,iA  tmdʨiE mdʨimdʨie'@equal[times[char[X],id[times[char[j],char[Omega]]]],int[times[char[x],id[char[t]],indexes[1,0,char[e],minus[times[char[j],char[Omega],char[t]]]],diff[char[t]]],minus[char[infty]],char[infty]]]~PodʪiF  t r J r r p@' char[Omega]pErK    y Qy y <@'times[char[x],id[char[t]]]0ayR   FqUFqFq)q'7indexes[1,0,char[e],times[char[j],char[Omega],char[t]]]HqFqV h Yh h @'-times[char[X],id[times[char[j],char[Omega]]]][vqh Z r ]r r p@' char[Omega]}q@†qr^ /b//֐)q'Btimes[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]z q/c ^eolڥogolڥoolڥomF'Vequal[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega],char[n]]]]],sum[times[char[x],id[(*i1i*)char[n]],indexes[1,0,char[e],minus[times[char[j],char[omega],char[n]]]]],minus[char[infty]],char[infty]]]~Hqlڧoh qlqqD)q'7indexes[1,0,char[e],times[char[j],char[omega],char[n]]]9{oqm FqvFqFq)q'7indexes[1,0,char[e],times[char[j],char[Omega],char[t]]]^{oFqw Pq !qqqD)q'7indexes[1,0,char[e],times[char[j],char[omega],char[n]]]vf>!vf>vf>`@'4indexes[0,1,char[omega],num[0.0000000000000000,"0"]]XDNQvf> $&> d'* Xf>$Xf>Xf>H@'fplus[indexes[0,1,char[omega],num[0.0000000000000000,"0"]],times[num[2.0000000000000000,"2"],char[pi]]]}QXf> !(&>##J\(J\J\O%'7equal[indexes[1,0,char[e],times[char[j],id[plus[indexes[0,1,char[omega],num[0.0000000000000000,"0"]],times[num[2.0000000000000000,"2"],char[pi]]]],char[n]]],times[indexes[1,0,char[e],times[char[j],indexes[0,1,char[omega],num[0.0000000000000000,"0"]],char[n]]],indexes[1,0,char[e],times[char[j],num[2.0000000000000000,"2"],char[pi],char[n]]]],indexes[1,0,char[e],times[char[j],indexes[0,1,char[omega],num[0.0000000000000000,"0"]],char[n]]]] HHˆ "HHˆwf iE'8~- h\ 9Scy dThe term on the left contributes a linear phase shift to the DTFT. The quantity inside the parenthe⌖Fm fses,`, is sometimes referred to as the discrete-time sinc function. It has the following properSc\+@ties: :-L2z4 hBy LHopitals rule, ] ;⌖і hM^ has regularly-occurring zero crossings at _ for all integer  k Scc bIn this section we summarize some of the properties of DTFTs along with some additional DTFT exam0JZjples. In some cases, brief proofs were provided in the lecture ... for the most part these proofs are not @6included in these notes in the interests of brevity. ?6$`LP1. Linearity.  lAs noted in class, the DTFT operation itself is linear. F)q^eR hP2. Time shift. d G x% h3P3. Multiplication by a complex exponential. e JF͒ h3E3. DTFT of an impulse. f  lfor all  n. KSc˛`WE4. DTFT of a constant.  lIn similar fashion, working from the right side we obtain OF͒E hg NScO mWhile this notation is cumbersome, it merely expresses the fact that a constant in time has a DTFT that is a @ kdelta function in frequency at h and that this function repreats periodically in frequency with period - Hi. LScF6-`TE5. DTFT of a complex exponential.  lUsing Property P3, we can now easily obtain _PF͒d hj. HHˆ"*HHˆE?&& l~J\ $+%%/p +/p /p @'+times[num[2.0000000000000000,"2"],char[pi]]. "'. . 2'prompt[]4c%/p (-))/p -/p /p @'+times[num[2.0000000000000000,"2"],char[pi]]'c%/p +/,, /@Ύ';equal[times[char[x],id[(*i1i*)char[n]]],times[over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]],indexes[1,0,char[e],times[char[j],char[omega],char[n]]],diff[char[omega]]],times[num[2.0000000000000000,"2"],char[pi]]]]]~I -1..! 1  E@' char[omega]H9Ŋ /300"/p 3/p /p @'+times[num[2.0000000000000000,"2"],char[pi]]~9ŏ/p 1522#d9o7d9od9o[2F'Uequal[prompt[],sum[(*n*)times[char[x],id[(*i1i*)char[l]],times[(*n*)over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[(*n*)times[string[" "],sum[(*n*)indexes[1,0,times[indexes[1,0,char[e],minus[times[char[j],char[omega],char[l]]]],char[e]],times[char[j],char[omega],char[n]]],equal[char[l],minus[char[infty]]],char[infty]],diff[char[omega]]],times[num[2.0000000000000000,"2"],char[pi]]]]],equal[char[l],minus[char[infty]]],char[infty]]]~d* 375 66+p;եo5p;եop;եoڕ'Dequal[times[char[x],id[(*i1i*)char[n]]],times[over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]],indexes[1,0,char[e],times[char[j],char[omega],char[n]]],diff[char[omega]]],times[num[2.0000000000000000,"2"],char[pi]]]],times[over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[(*n*)times[string[" "],sum[(*n*)times[char[x],id[(*i1i*)char[l]]],equal[char[l],minus[char[infty]]],char[infty]],indexes[1,0,times[indexes[1,0,char[e],minus[times[char[j],char[omega],char[l]]]],char[e]],times[char[j],char[omega],char[n]]],diff[char[omega]]],times[num[2.0000000000000000,"2"],char[pi]]]]]~Rd9o 5944,/p 9/p /p @'+times[num[2.0000000000000000,"2"],char[pi]]xFv/p 7;880 ;  _@'equal[char[n],char[l]]`v 9=::1 =  _@'equal[char[l],char[n]]M 4v ;?<<2 ?  uX@'!times[char[x],id[(*i1i*)char[n]]]v =A>>3t4qAt4qt4q)q'v4q ?F@@8Q.oFQ.oQ.ozF'>equal[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]],sum[times[char[x],id[(*i1i*)char[n]],indexes[1,0,char[e],minus[times[char[j],char[omega],char[n]]]]],equal[char[n],minus[char[infty]]],char[infty]],sum[times[indexes[1,0,char[alpha],char[n]],indexes[1,0,char[e],minus[times[char[j],char[omega],char[n]]]]],equal[char[n],num[0.0000000000000000,"0"]],char[infty]],sum[indexes[1,0,id[times[char[alpha],indexes[1,0,char[e],minus[times[char[j],char[omega]]]]]],char[n]],equal[char[n],num[0.0000000000000000,"0"]],char[infty]],over[num[1.0000000000000000,"1"],plus[num[1.0000000000000000,"1"],minus[indexes[1,0,times[char[alpha],char[e]],times[minus[(*n*)char[(*n*)j]],char[omega]]]]]]]d E/ HHˆ CHHˆc JgE%ScS`%By comparison of the terms we obtain &R| hK 'ScD!`and (R\J hL )ک~-lE h9Because M and N for any complex variable  Z, *u hO +Scݍ`Hence ,R hP -Sc`and .~-7 hS 0)q^e`] (ZWe note that T is an even function of U, V is odd, W is even and X is Scp?D@1odd, at least for this particular time function. 1%`XE2. The finite-duration pulse.  lWe next consider the finite duration causal pulse, 21e hY 3Sc" `"This sum is also easily obtained: 4F͒ hZ 5Sc mPlease note that we used the relation for the finite sum of exponentials discussed in recition in developing E@fthe last result. This expression can be further simplified by balancing the terms in the parentheses: 6ԓ5:+ h[ ]7ScaY`or HHˆ C/HHˆ'DD l~\S.o AHBB9m(H(܂m(Ԕ'Sequal[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]],over[num[1.0000000000000000,"1"],plus[num[1.0000000000000000,"1"],minus[times[char[alpha],indexes[1,0,char[e],minus[times[char[j],char[omega]]]]]]]],times[id[over[(*n*)num[1.0000000000000000,"1"],plus[num[1.0000000000000000,"1"],minus[times[char[alpha],indexes[1,0,char[e],minus[times[char[j],char[omega]]]]]]]]],id[over[plus[num[1.0000000000000000,"1"],minus[times[char[alpha],indexes[1,0,char[e],times[char[j],char[omega]]]]]],plus[num[1.0000000000000000,"1"],minus[times[char[alpha],indexes[1,0,char[e],times[char[j],char[omega]]]]]]]]],over[plus[(*n*)num[1.0000000000000000,"1"],minus[times[char[alpha],indexes[1,0,char[e],times[char[j],char[omega]]]]]],plus[num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]],over[plus[(*n*)num[1.0000000000000000,"1"],minus[times[char[alpha],cos[id[char[omega]]]]],minus[times[char[j],char[alpha],sin[id[char[omega]]]]]],plus[num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]]]N$¡o( F5GG:bi JbibiO'tequal[times[char[R],char[e],id[(*i1i*)times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]],over[plus[num[1.0000000000000000,"1"],minus[times[char[alpha],cos[id[char[omega]]]]]],plus[num[2.0000000000000000,"2"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]]]~Xebi! CLRIID;bi&LbibiO濎'Zequal[times[char[I],char[m],id[(*i1i*)times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]],over[minus[times[char[j],char[alpha],sin[id[char[omega]]]]],plus[num[2.0000000000000000,"2"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]]]~/3bi' CJNRKKD<iГ+NiГiГEک'vequal[indexes[1,0,abs[char[Z]],num[2.0000000000000000,"2"]],sqrt[plus[indexes[1,0,id[times[char[R],char[e],id[(*i1i*)char[Z]]]],num[2.0000000000000000,"2"]],indexes[1,0,id[times[char[I],char[m],id[(*i1i*)char[Z]]]],num[2.0000000000000000,"2"]]]]]oe‘iЕ, CLPMMD=ZI&/P[,I&ZI&H'yequal[angle[char[Z]],atan[id[over[times[char[I],char[m],id[(*i1i*)char[Z]]],times[char[R],char[e],id[(*i1i*)char[Z]]]]]]]1P¡L],I&0 CNR~-OOD> 4R  }'requal[indexes[1,0,abs[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],num[2.0000000000000000,"2"]],plus[indexes[1,0,id[over[plus[(*n*)num[1.0000000000000000,"1"],minus[times[char[alpha],cos[id[char[omega]]]]]],plus[num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]]],num[2.0000000000000000,"2"]],indexes[1,0,id[over[minus[times[char[alpha],sin[id[char[omega]]]]],plus[num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]]],num[2.0000000000000000,"2"]]],over[(*n*)plus[(*n*)num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]],indexes[1,0,id[plus[(*n*)num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]],num[2.0000000000000000,"2"]]]]lir 5 CPTuQQD?:TKG'-equal[abs[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],over[num[1.0000000000000000,"1"],sqrt[plus[(*n*)num[1.0000000000000000,"1"],minus[times[num[2.0000000000000000,"2"],char[alpha],cos[plus[(*n*)id[(*n*)char[omega]],indexes[1,0,char[alpha],num[2.0000000000000000,"2"]]]]]]]]]]~.; CRWRSSD@dvvI&@WԿI&I&Ij_'eequal[angle[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],atan[id[over[minus[times[char[alpha],sin[id[char[omega]]]]],plus[(*n*)num[1.0000000000000000,"1"],minus[times[char[alpha],cos[id[char[omega]]]]]]]]]]~nԿI&A CTY~-VVDCEY֛w)q'dtimes[char[R],char[e],id[(*i1i*)times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]]c4F CW[^eXXDD I[  E@' char[omega]ohJ CY\ZZDE-l 4ON C[^^e]]DFOO\OO֛')q'dtimes[char[I],char[m],id[(*i1i*)times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]]4$U C\a^e__DG$V^$$֓O)q'Gabs[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]5[a55֕)q'Iangle[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]45\ C^c^e``DHzpaczPzpc1e'equal[times[char[x],id[(*i1i*)char[n]]],lparen[(*i2i*)matrix[(*i1in*)2,1,comma[num[1.0000000000000000,"1"],leq[num[0.0000000000000000,"0"],char[n],plus[char[N],minus[num[1.0000000000000000,"1"]]]]],comma[num[0.0000000000000000,"0"],string[" otherwise"]]]]]~׈|Pb CaebbDI< Doge< Do< DoF'equal[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]],sum[times[char[x],id[(*i1i*)char[n]],indexes[1,0,char[e],minus[times[char[j],char[omega],char[n]]]]],equal[char[n],minus[char[infty]]],char[infty]],sum[indexes[1,0,char[e],minus[times[char[j],char[omega],char[n]]]],equal[char[n],num[0.0000000000000000,"0"]],plus[char[N],minus[num[1.0000000000000000,"1"]]]],sum[indexes[1,0,id[indexes[1,0,char[e],minus[times[char[j],char[omega]]]]],char[n]],equal[char[n],num[0.0000000000000000,"0"]],plus[char[N],minus[num[1.0000000000000000,"1"]]]],over[plus[num[1.0000000000000000,"1"],minus[indexes[1,0,char[e],minus[times[char[j],char[omega],char[N]]]]]],plus[num[1.0000000000000000,"1"],minus[indexes[1,0,char[e],times[minus[(*n*)char[(*n*)j]],char[omega]]]]]]]~> Doh CcgddDJǦogǦ܂Ǧoc'equal[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]],over[plus[num[1.0000000000000000,"1"],minus[indexes[1,0,char[e],minus[times[char[j],char[omega],char[N]]]]]],plus[num[1.0000000000000000,"1"],minus[indexes[1,0,char[e],times[minus[(*n*)char[(*n*)j]],char[omega]]]]]],times[id[over[indexes[1,0,char[e],minus[times[char[j],char[omega],fract[(*n*)char[(*n*)N],num[(*n*)2.0000000000000000,"2"]]]]],indexes[1,0,char[e],minus[times[char[j],fract[(*n*)char[(*n*)omega],num[(*n*)2.0000000000000000,"2"]]]]]]],id[over[plus[indexes[1,0,char[e],times[char[j],char[omega],fract[(*n*)char[(*n*)N],num[(*n*)2.0000000000000000,"2"]]]],minus[indexes[1,0,char[e],minus[times[char[j],char[omega],fract[(*n*)char[(*n*)N],num[(*n*)2.0000000000000000,"2"]]]]]]],plus[indexes[1,0,char[e],times[char[j],fract[(*n*)char[(*n*)omega],num[(*n*)2.0000000000000000,"2"]]]],minus[indexes[1,0,char[e],minus[times[char[j],fract[(*n*)char[(*n*)omega],num[(*n*)2.0000000000000000,"2"]]]]]]]]]],times[indexes[1,0,char[e],minus[times[char[j],char[omega],fract[(*n*)id[plus[(*n*)char[(*n*)N],minus[(*n*)num[(*n*)1.0000000000000000,"1"]]]],num[(*n*)2.0000000000000000,"2"]]]]],id[over[times[num[2.0000000000000000,"2"],char[j],sin[id[fract[(*n*)times[(*n*)char[(*n*)N],char[(*n*)omega]],num[(*n*)2.0000000000000000,"2"]]]]],times[num[2.0000000000000000,"2"],char[j],sin[id[fract[char[omega],num[2.0000000000000000,"2"]]]]]]]]]emWǨp Ce5ffDKI&uiI&I&Ut'equal[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]],times[indexes[1,0,char[e],minus[times[char[j],char[omega],fract[(*n*)id[plus[(*n*)char[(*n*)N],minus[(*n*)num[(*n*)1.0000000000000000,"1"]]]],num[(*n*)2.0000000000000000,"2"]]]]],id[over[sin[id[fract[(*n*)times[(*n*)char[(*n*)N],char[(*n*)omega]],num[(*n*)2.0000000000000000,"2"]]]],sin[id[fract[char[omega],num[2.0000000000000000,"2"]]]]]]]]~HI&v "-~-hh&Le_}xe_e_̳r-L'eequal[lim[over[sin[id[fract[(*n*)times[(*n*)char[(*n*)N],char[(*n*)omega]],num[(*n*)2.0000000000000000,"2"]]]],sin[id[fract[char[omega],num[2.0000000000000000,"2"]]]]],rightarrow[char[omega],num[0.0000000000000000,"0"]]],char[N]]H$lH$lHwkmHwlH$lnH$lHwmoHwlHHˆnpHHˆlHHˆoHHˆlH$rH$lHwqsHw lHHˆrHHˆ lHHˆHHˆ l $$ U$$acw%v_HScSBm $$ U$$uu l}$e  U{$e uW} eHeadings Table =g_~ "-*2jj&M}e  Ue uW~ e } e  U e uW e }$Cel Uw|$Celu!W  eHeading Level }Ce U{}Ceu!W  eParagraph Format } Ce U|~ Ceu!W  e Comments }$Sel U}$Selu"W  e3 }Se U~Seu"W UTUTe CellBodyNum } Se U& Seu"W  e d H$H$kW d HwHwlWd H$H$mWd HwHwnWd HHˆHHˆo_z+zd HHˆHHˆp_z+zd H$H$qWh018-791 Lecture 3 Notes-Q6R-Fall, 2005 HwHwrW` HHˆHHˆs_z+z` d  HR  HR HRHR!Footnote Hr3@  Hr3@ HzHz! Single LineH Footnote   H3D  H3D HH! Double LineH  Double Line  H   Single Line HZ   TableFootnote EGyR  EGyR EPwEPw! TableFootnotedtt HHˆHHˆmGt/vȂ޸`# NOTES FOR 18-791 LECTURES 3 and 4 |< h>Introduction to Discrete-Time Fourier Transforms (DTFTs)  Sc`$Distributed:  lSeptember 8, 2005 ńs pNotes:  lThis handout contains in brief outline form the lecture notes used for 18-791 lectures Number 3 and 2jg4, presented by videotape on September 6 and 8. Because the notes were transcribed some time after the jlecture was taped, there may be some minor differences between these notes and what is seen on the video. eAlso, topics have been merged across the two lectures, so the order of presentation may vary somwhat @from what is in the lecture.  UTm` Introduction Sc)j gLast week we talked about the time domain behavior of discrete-time signals and systems. Today we will 04ibegin (or more accurately we will begin to review) how we characterize discrete-time signals and systems @Cin the frequency domain using the discrete-time Fourier transform.  UT\`The DTFT and its inverse  Sct hProbably the easiest way to introduce the discrete-time Fourier transform (DTFT) is through its counter0hpart, the continuous-time Fourier transform (CTFT). As you will recall, the CTFT and its inverse can be @expressed as: t| h & ' h @ (mNote that we use the upper case variable  to indicate continuous-time angular frequency in this course. Sc<nAs we have discused, the first equation (which is actually the inverse CTFT) expresses the fact that a finite-@" genergy time function  can be represented as a weighted linear combination of complex exponentials )q7q g. The second equation (the actual CTFT) tells you how to compute the weights . 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HH²$ =HH²$«R Gf?MScS`GThis is simply a shifted delta function that is repeated periodically. Qi`SE6. DTFT of a cosine.  lFrom Eulers representation of trig functions we obtain R?x B hk I@&>e (mThis is simply a pair of delta functions of area l occuring at m, repeating periodically with period y9" Hn. D)q^e" hP4. Time reversal. o Ui h9We note that if a time function is  even l, q V h6Similarly, if a time function is  odd,  lr WSc mIn other words, if a time function is even, its DTFT is also even, and if a time function is odd its DTFT is \@also odd.  W S)q^e hP5. Complex conjugation. p T< h:We note that if a time function is  real l, s. X (wThis latter property is referred to as  Hermitian symmetry.  lIf t is Hermetian symmetric, its real part is SclxCneven, its imaginary part is odd, its magnitude is real, and its phase angle is odd. We note further that if a 0x^jreal time function is even or odd, both the Hermitian symmetry and the time reversal properties constrain qthe transform. Specifically, if a time function is both real and even, its DTFT is also real and even. If a time @kfunction is real and odd, its DTFT is both imaginary and odd. For example, the sine wave has the transform Y?x hu EoAG;`P6. Parsevals theorem. ZF͒LO hv [ScVD qThis relationship is important because the quantity on the left side of the equation is clearly the total energy '<gof the time function. Hence the energy in a frequency band can be obtained by integrating the function _J^e; hw over that frequency band. (Be sure to take the negative frequencies into account!) Because of its T Hephsycial meanining, the function x is sometimes referred to as the  energy density spectrum. \Scnl mP7. Initial value theorems.  lThese trivial-to-prove theorems are sometimes confused with Parsevals theoz@+rem. They sometimes help with computation. ]]F͒™. hy HH²$=HH²$'b>> l< A< < @@'.equal[char[omega],num[0.0000000000000000,"0"]]\ڡ< "[ I  @'char[pi][x  =GKHH>\f>Kf>f>SЉ@'Kequal[char[omega],pm[indexes[0,1,char[omega],num[0.0000000000000000,"0"]]]]Q0䮧f> =IM&>JJ>]/p M/p /p @'+times[num[2.0000000000000000,"2"],char[pi]]H"/p =KOLL>^OcOOcOc֨֎)q'LRarrow[times[char[x],id[(*i1i*)minus[char[n]]]],times[char[X],id[indexes[1,0,char[e],times[minus[(*n*)char[(*n*)j]],char[omega]]]]]]E"Qc =MS^eNN>_O_QO_O_֨Я)q'wLRarrow[times[ast[char[x]],id[(*i1i*)char[n]]],times[ast[char[X]],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]U]nQ_ =TW^ePP>`q̒Sq̒q̒S8)q'gequal[times[char[x],id[(*i1i*)char[n]]],LRarrow[times[char[x],id[(*i1i*)minus[char[n]]]],times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],times[char[X],id[indexes[1,0,char[e],minus[times[char[j],char[omega]]]]]]]qq̔ =OT^eRR>a䟰B씇 =SQ^eUU>bB쒇TB쒇B쒇Z!v)q'%equal[times[char[x],id[(*i1i*)char[n]]],LRarrow[times[minus[(*n*)char[(*n*)x]],id[(*i1i*)minus[char[n]]]],times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],times[minus[(*n*)diacritical[(*n*)0,1,0,0,0,char[(*n*)X]]],id[indexes[1,0,char[e],minus[times[char[j],char[omega]]]]]]]쒇W쒇쒇Uv)q' equal[(*n*)times[char[x],id[(*i1i*)char[n]]],times[(*n*)ast[(*n*)char[(*n*)x]],LRarrow[(*n*)id[(*i1i*)char[(*n*)n]],times[char[(*n*)X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]]],times[ast[char[X]],id[indexes[1,0,char[e],minus[times[char[j],char[omega]]]]]]]`uD씇 =QY^eVV>c/Y//֐)q'Btimes[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]L|Bm/ =W[^eXX>dJ([J(J(K?x'6equal[sin[id[times[indexes[0,1,char[omega],num[0.0000000000000000,"0"]],char[n]]]],LRarrow[over[plus[indexes[1,0,char[e],times[char[j],indexes[0,1,char[omega],num[0.0000000000000000,"0"]]]],minus[indexes[1,0,char[e],minus[times[char[j],indexes[0,1,char[omega],num[0.0000000000000000,"0"]],char[n]]]]]],times[num[2.0000000000000000,"2"],char[j]]],times[over[char[pi],char[j]],sum[id[plus[times[char[delta],id[plus[char[omega],minus[times[indexes[0,1,char[omega],num[0.0000000000000000,"0"]],minus[(*n*)times[(*n*)num[(*n*)2.0000000000000000,"2"],char[(*n*)pi],char[(*n*)r]]]]]]]],minus[times[char[delta],id[plus[char[omega],times[indexes[0,1,char[omega],num[0.0000000000000000,"0"]],minus[(*n*)times[(*n*)num[(*n*)2.0000000000000000,"2"],char[(*n*)pi],char[(*n*)r]]]]]]]]]],equal[char[r],minus[char[infty]]],char[infty]]]]]~ᎄL( =Y]ZZ>el.o!]l.ol.oNF'equal[sum[(*n*)indexes[1,0,abs[times[char[x],id[(*i1i*)char[n]]]],num[2.0000000000000000,"2"]],equal[char[n],minus[char[infty]]],char[infty]],times[over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[times[indexes[1,0,abs[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],num[2.0000000000000000,"2"]],diff[char[omega]]],times[num[2.0000000000000000,"2"],char[pi]]]]]~(l.o" =[_\\>f+__J'pindexes[1,0,abs[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],num[2.0000000000000000,"2"]]Hs, =]c^e^^>gdCbb HHˆD `HHˆ hhb_^② hz HHˆF`HHˆ?aa lŒ]j9 =_f^edd>h:c_J'pindexes[1,0,abs[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]]],num[2.0000000000000000,"2"]]zO)oIfzO)ozO)o'F'`equal[sum[(*n*)times[char[x],id[(*i1i*)char[n]]],equal[char[n],minus[char[infty]]],char[infty]],substitution[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]]],equal[char[omega],num[0.0000000000000000,"0"]]]]~|O)oJ =cee>ij殞Nhj殞j殞ֶsW'equal[times[char[x],id[(*i1i*)num[0.0000000000000000,"0"]]],times[over[num[1.0000000000000000,"1"],times[num[2.0000000000000000,"2"],char[pi]]],int[times[char[X],id[indexes[1,0,char[e],times[char[j],char[omega]]]],diff[char[omega]]],times[num[2.0000000000000000,"2"],char[pi]]]]]~Hl殠O `ggajF I CEII$I$ dLeftdRightd  Referenceddd CdUHeadingsd HTMLdHTMLd "d =d `*66f@E !EquationEquation. f@ !CellBody. f@ ! 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