King Fahd University of Petroleum & Minerals Computer Engineering Dept

Size: px
Start display at page:

Download "King Fahd University of Petroleum & Minerals Computer Engineering Dept"

Transcription

1 King Fahd University of Petroleum & Minerals Computer Engineering Dept COE 4 Data and Computer Communications erm 5 Dr. shraf S. Hasan Mahmoud Rm -4 Ext ashraf@kfupm.edu.sa /7/6 Dr. shraf S. Hasan Mahmoud Lecture Contents. Fourier nalysis a. Fourier Series Expansion b. Fourier ransform c. Ideal Low/band/high pass filters. Introduction to Z-ransform /7/6 Dr. shraf S. Hasan Mahmoud

2 Signals signal is a function representing information Voice signal microphone output Video signal camera output Etc. ypes of Signals nalog continuous-value continuous-time Discrete discrete-value continuous-time Digital predetermined discrete levels much easier to reproduce at receiver with no errors Binary only two predetermined levels: e.g. and /7/6 Dr. shraf S. Hasan Mahmoud 3 Example of Continuous-Value Continuous-time signal s (t) and s (t) are two example of analog signals s (t) s (t) /7/6 Dr. shraf S. Hasan Mahmoud 4 t t

3 Example of Discrete-Value Continuous-time signal d (t) and d (t) are two example of discrete signals d (t) takes more than two levels d (t) takes only two levels - binary d (t) d (t) /7/6 Dr. shraf S. Hasan Mahmoud 5 t Note d (t) extends to ± t ime Domain Representation ime domain representation we plot value (voltage, current, electric field intensity, etc.) versus time Can infer rate of change (speed or frequency) information e.g. s (t) seems faster than s (t) Using calculus terms: rate of change for s (t) > rate of change for s () s (t) d (t) pplies to BOH analog and digital signals t t s (t) d (t) t t /7/6 Dr. shraf S. Hasan Mahmoud 6 3

4 Frequency - Bandwidth s (t) faster than s (t) s (t) contains higher frequencies than those contained in s (t) s (t) and s (t) contain more than one frequency Minimum frequency f min Maximum frequency f max Bandwidth Range of frequencies contained in signal f max f min pplies to BOH analog and digital signals /7/6 Dr. shraf S. Hasan Mahmoud 7 Frequency Bandwidth () For our example signals, assume: S(t): fmin Hz, fmax 5 Hz S(t): fmin 5 Hz, fmax Hz his means: BW for s (t) 5 49 Hz BW for s (t) Hz pplies to BOH analog and digital signals Note that: because s (t) is faster than s (t) it should contain frequencies higher than those in s (t) E.g. s (t) contains frequencies (5,] which do not exist in s (t) /7/6 Dr. shraf S. Hasan Mahmoud 8 4

5 Frequency Bandwidth (3) Consider the discrete signals d (t) and d (t) he function plots have points of infinite slope rate of change frequency herefore for signals that look like d (t) and d (t), fmax Furthermore, BW Example: d (t) contains frequencies from some minimum fmin Hz to fmax Hz pplies to BOH analog and digital signals /7/6 Dr. shraf S. Hasan Mahmoud 9 Example of Signal BW Consider the human speech ypically fmin ~ Hz fmax ~ 35 Hz BW of the human speech signal 3 Hz /7/6 Dr. shraf S. Hasan Mahmoud 5

6 Bandwidth for Systems For a system to respond (amplify, process, x, Rx, etc.) for a particular signal with all its details, the system should have an equal or greater bandwidth compared to that of the signal Example: he system required to process s (t) should have a greater bandwidth than the system required to process s (t) /7/6 Dr. shraf S. Hasan Mahmoud Bandwidth for Systems () Example : consider the human ear system Responds to a range of frequencies only fmin Hz fmax, Hz BW 9,98 Hz It does not respond to sounds with frequencies outside this range Example 3: consider the copper wire It passes (electric) signals only between a certain fmin and a certain fmax he higher the quality of the wire the wider the BW More on Systems BW later! /7/6 Dr. shraf S. Hasan Mahmoud 6

7 Frequency Representation How to represent signals and indicate their frequency content? he X-axis: frequency (in Hertz or Hz) What is the Y-axis then? the answer will be postponed! f max 5 Hz pplies to BOH analog and digital signals f min Hz BW for s (t): range of frequencies f f min 5 Hz BW for s (t): range of frequencies f max Hz f /7/6 Dr. shraf S. Hasan Mahmoud 3 Periodic Signals pplies to BOH analog and digital signals periodic signal repeats itself every seconds Period seconds In calculus terms: s(t) is periodic if s(t) s(t+) for any - < t < For previous examples: s (t), s (t), and d (t) are not periodic however, d (t) is periodic /7/6 Dr. shraf S. Hasan Mahmoud 4 7

8 Periodic Signals () pplies to BOH analog and digital signals periodic signal has a FUNDMENL FREQUENCY f f / where is the period periodic signal may also has frequencies other than the fundamental frequency f fmin < f < fmax x x x x x x BW for periodic s(t) f min f max /7/6 Dr. shraf S. Hasan Mahmoud 5 f Periodic Signals (3) pplies to BOH analog and digital signals Examples of other periodic signals: s 3 (t) t s 5 (t) ~ t s 4 (t) t t /7/6 Dr. shraf S. Hasan Mahmoud 6 8

9 Energy/Power of Signals Energy for any signal is defined as E s s( t) dt pplies to BOH analog and digital signals where the integral is carried over LL range of t In other words, Es is the area under the absolute squared of the signal he unit of energy is Joules /7/6 Dr. shraf S. Hasan Mahmoud 7 Energy/Power of Signals () pplies to BOH analog and digital signals Note that for periodic signal E s is equal to infinity since it is defined on (-, ) However power is FINIE for these type of signals Power is defined as the average of the absolute squared of the signal, i.e. P s he unit of power is Joules/sec or Watt s( t) /7/6 Dr. shraf S. Hasan Mahmoud 8 dt Note the integral can be performed on [,], [-/, /], or any continuous interval of length 9

10 VERY SPECIL nalog Signal function of the form s(t) cos(πft + θ) s(t) cos(θ) - Period t /7/6 Dr. shraf S. Hasan Mahmoud 9 Characteristics of COSINE Completely specified by: mplitude Phase - θ Frequency f s(t ) cos(θ) Periodic signal repeats itself every seconds / f ime to review your trigonometry!! E.g. sin(x) cos(x-π/) /7/6 Dr. shraf S. Hasan Mahmoud

11 Characteristics of COSINE () Energy for this signal, E s infinity Power for this signal, P g / Note P g is dependent only on the amplitude Exercise: Verify the above results using the power formula It contains ONLY ONE frequency f he purest form of analog signals Frequency representation: x BW for s (t) f min f max f Hz /7/6 Dr. shraf S. Hasan Mahmoud f Characteristics of COSINE (3) Very Useful Properties (f /) cos( πft + θ ) dt cos( πnft + θ ) dt cos (πft + θ ) dt / cos (πnft + θ ) dt / cos(πnft)cos(πmft) dt / n m n m /7/6 Dr. shraf S. Hasan Mahmoud

12 Example of Cosine Functions Y (t) has a frequency f of Hz ( ½ sec) n amplitude of 3 P Y 3 / 4.5 Watts Y (t) - has a frequency f of Hz ( / sec) n amplitude of P Y /.5 Watts value Examples of analog contineous-time functions y 3 cos(*pi**t) y cos(*pi**t) time - t /7/6 Dr. shraf S. Hasan Mahmoud 3 ONLY FOR PERIODIC SIGNLS Fourier Series Expansion Can we use the basic cosine functions to represent periodic signals? YES Fourier Series Expansion t s 3 (t) t factorization t t /7/6 Dr. shraf S. Hasan Mahmoud 4

13 Fourier Series Expansion () For a periodic signal s(t) can be represented as a sum of sinusoidal signals as in s( t) + n cos(πnft) + Bn sin(πnf [ t ] ) n where the coefficients are computed using: s( t) dt n s( t)cos(πnf t) dt /7/6 Dr. shraf S. Hasan Mahmoud 5 B f is the fundamental frequency of s(t) and is equal to / n s( t)sin(πnf t) dt Fourier Series Expansion (3) nother form for the series: C s( t) + Cn cos(πnft + θn ) n where the coefficients are computed using: C n n C + B n B n B θ n n θ n tan n n /7/6 Dr. shraf S. Hasan Mahmoud 6 C n 3

14 Notes on Fourier Series Expansion he representation (the sum of sinusoids) is completely identical and equivalent to the original specification of s(t) It is applies to any periodic signal analog or digital! Very powerful tool it reveals all frequencies contained in the original periodic signal s(t) /7/6 Dr. shraf S. Hasan Mahmoud 7 Notes on Fourier Series Expansion () In general, s(t) contains DC term the zero frequency term / (possibly infinite) number of harmonics (or sinusoids) at multiples of the fundamental frequency, f he contribution of a harmonic with frequency nf is proportional to n +B n or C n E.g. if C n ~, then we say the harmonic at nf (or higher does not contribute significantly towards building s(t) more on this when we discuss total power! /7/6 Dr. shraf S. Hasan Mahmoud 8 4

15 Notes on Fourier Series Expansion (3) harmonic with frequency equal to nf (n>), has a period of /(n) In general the series expansion of s(t) contains INFINIE number of terms (harmonics) However for less than % accurate representation one can ignore higher terms terms with frequencies greater than certain n * f /7/6 Dr. shraf S. Hasan Mahmoud 9 Notes on Fourier Series Expansion (4) Lets define the following function: s_e(nk) o be the series expansion of s(t) up to and including the n k term It should be noted that s_e(nk) is periodic with period Examples: s _ e( n ) / s _ e( n ) / + cos(π ft) + B sin(πf t) + C cos(π f t + ) / θ /7/6 Dr. shraf S. Hasan Mahmoud 3 5

16 Notes on Fourier Series Expansion (5) Examples cont d: s _ e( n ) / + cos(πf t) + B sin(πf t) + cos(π f t) + B sin(π f t) / + C cos(π ft + θ) + C cos(π ft + θ) s _ e( n ) [ cos(πnf t) + B sin(πnf t ] + ) n n n / + Cn cos(πnft + θn) n /7/6 Dr. shraf S. Hasan Mahmoud 3 Notes on Fourier Series Expansion (6) It is obvious that s(t) is % represented by s_e(n ) s_e(n n* < ) produces a less than % accurate representation of the original s(t) For most practical periodic signals s_e(n) provides a more than enough accuracy in representing s(t) No need for infinite number of terms /7/6 Dr. shraf S. Hasan Mahmoud 3 6

17 Example : Consider the following s(t) Over one period, the signal is defined as s(t) s(t) -/4 < t < /4 /4 < t < 3/4 -/4 /4 3/4 5/4 t Finding the Series Expansion: he DC term s t dt ( ) /7/6 Dr. shraf S. Hasan Mahmoud 33 Example : cont d he term n : n s( t)cos(πnf t) dt cos(πnft) dt t sin(πnft) πnf t nπ sin( ) πn πn πn n,4,6,... n,5,9,... n 3,7,,... Remember. f /. cos(ax) dx -/a sin(ax) 3. sin(nπ) for integer n 4. sin(nπ/) for n,5,9, 5. sin(nπ/) - for n3,7,, /7/6 Dr. shraf S. Hasan Mahmoud 34 7

18 Example : cont d herefore n is given by: ( ) ( n ) / πn n,4,6,... n,3,5,7,... Remember (-) (n-)/ for n,5,9, - for n 3,7,, /7/6 Dr. shraf S. Hasan Mahmoud 35 Example : cont d he term B n : B n s( t)sin(πnf t) dt sin(πnft) dt t nπ nπ cos(πnft) cos( ) cos( ) πnf t πn Remember. cos(ax)dx -/a sin(ax). cos(x) cos(-x) /7/6 Dr. shraf S. Hasan Mahmoud 36 8

19 Example : cont d herefore, the overall series expansion is given by ( n ) / ( ) s( t) + cos(πnft) π n n,3,5 s( t) + cos(πf t) cos(π 3 ft) π 3π + cos(π 5 ft) cos(π 7 ft) π 7π /7/6 Dr. shraf S. Hasan Mahmoud 37 Example : cont d Original s(t) and the series up to and including n i.e. Comparing: vs. s(t) s_e(n) / original s(t) up to n /7/6 Dr. shraf S. Hasan Mahmoud 38 9

20 Example : cont d Original s(t) and the series up to and including n i.e. Comparing:..8 original s(t) up to n vs. s(t).6.4. s_e(n) / + -. /π cos(πf t) /7/6 Dr. shraf S. Hasan Mahmoud 39 Example : cont d Original s(t) and the series up to and including n 3 i.e. Comparing:..8 original s(t) up to n 3 vs. s(t).6.4. s_e(n3) / + /πcos(πf t) /(3π)cos(π3f t) /7/6 Dr. shraf S. Hasan Mahmoud 4

21 Example : cont d Original s(t) and the series up to and including n i.e. Comparing: vs. s(t) original s(t) up to n s_e(n) / + /πcos(πf t) /(3π)cos(π3f t) + /(5π)cos(π5f t) /(7π)cos(π7f t) +/(π)cos(πf t) /7/6 Dr. shraf S. Hasan Mahmoud 4 Example: cont d clear all ; ; t -:.:; n_max ; s (*square(*pi/*(t+/4))+)/; figure() plot(t, s); grid axis([ -..]); he matlab code for plotting and evaluating the Fourier Series Expansion his code builds the series incrementally using the for loop Make sure you study this code!! s_e /*ones(size(t)); for n::n_max s_e s_e + (-)^((n-)/) * */(n*pi) * cos(*pi*n/*t); end figure() plot(t, s,'b-', t, s_e,'r--'); axis([ -..]); legend('original s(t)', 'up to n '); grid /7/6 Dr. shraf S. Hasan Mahmoud 4

22 Notes Previous Example he more terms included in the series expansion the closer the representation to the original s(t) i.e. comparing s(t) with s_e(nn*), the greater the n* the closer the representation is How to measure closeness? nswer: Let s use power!! /7/6 Dr. shraf S. Hasan Mahmoud 43 Power Calculation Using Fourier Series Expansion Rule: if s(t) is represented using Fourier Series expansion, then its power can be calculated using: P s s( t) dt 4 + [ n + Bn ] n + C n 4 n /7/6 Dr. shraf S. Hasan Mahmoud 44

23 Power Calculation Using Fourier Series Expansion () he previous result is based on the following two facts: () For f(t) constant power of f(t) constant Proof: power / X constant dt / X constant X constant Watts /7/6 Dr. shraf S. Hasan Mahmoud 45 Power Calculation Using Fourier Series Expansion (3) he previous result is based on the following facts (continued): () For f(t) cos(πnf t+θ) power of f(t) / Proof: Pf f ( t) dt cos (πnft + [ + cos(4πnft + θ )] dt [ + ] θ ) dt /7/6 Dr. shraf S. Hasan Mahmoud 46 3

24 Example : Problem: What is the power of the signal s(t) used in previous example? nd find n* such that the power contained in s_e(nn*) is 95% of that existing in s(t)? Solution: Let the power of s(t) be given by P s s s( t) dt P.5 /7/6 Dr. shraf S. Hasan Mahmoud 47 Example : cont d Now it is desired to compute the power using the Fourier Series Expansion What is the power in s_e(n) /? ns: we apply the power formula: P s _ e( n ) s _ e( n ) 4 4 /7/6 Dr. shraf S. Hasan Mahmoud 48 dt.5 4

25 Example : cont d What is the power in s_e(n) / + /π cos(πf t) ns: we can use the result on slide Power Calculation Using Fourier Series Expansion: P s _ e( n ) s _ e( n ) dt π. 456 π /7/6 Dr. shraf S. Hasan Mahmoud 49 Example : cont d What is the power in s_e(n3) / + /π cos(πf t) /(3π) cos(π3f t) ns: we can use the result on slide Power Calculation Using Fourier Series Expansion: Ps _ e( n 3) s _ e( n 3) dt π 9π + 4 π 9π /7/6 Dr. shraf S. Hasan Mahmoud 5 5

26 Example : cont d What is the power in s_e(n5) / + /π cos(πf t) /(3π) cos(π3f t) + /(5π) cos(π5f t) ns: we can use the result on slide Power Calculation Using Fourier Series Expansion: P s _ e( n 5) s _ e( n 5) dt π 9π + 4 π 9π 5π π /7/6 Dr. shraf S. Hasan Mahmoud 5 Example : cont d What is the power in ( n ) / ( ) s _ e( n ) + cos(πnft) π n,3,5 n ns: we can use the result on slide Power Calculation Using Fourier Series Expansion: P s _ e( n ) s _ e( n ) dt π. 5 n n π his the EXC SME power contained in s(t) his is expected since s(t) is % represented by s_e(n ) /7/6 Dr. shraf S. Hasan Mahmoud 5 n n 6

27 Example : cont d s_e(nk) Expression Power % Power + k /.5 (.5 )/(.5 ) 5% k / + /πcos(πf t).456 (.456 )/(.5 ) 9.5% k * / + /πcos(πf t) % k 3 / + /πcos(πf t) /(3π)cos(π3f t) k 5 / + /πcos(πf t) /(3π)cos(π3f t) + /(5π)cos(π5f t) % % + % power power of s_e(nk) relative to original power in s(t) which is equal to.5 /7/6 Dr. shraf S. Hasan Mahmoud * 53 For k, the expression s_e(nk) is the same as that for s_e(k). Why? Example : cont d herefore, s_e(nn*) such that 95% of power is contained n* 3 /7/6 Dr. shraf S. Hasan Mahmoud 54 7

28 Power Spectral Density Function Fourier Series Expansion: Specifies all the basic harmonics contained in the original function s(t) C n / ( n +B n ) / determines the power contribution of the nth harmonic with frequency nf he power Spectral Density function is a function specifying: how much power is contributed by a given frequency /7/6 Dr. shraf S. Hasan Mahmoud 55 Power Spectral Density Function () ypical PSD function for periodic signals: PSD(f) C / s( t) Periodic s(t) () Fourier Series Expansion + Cn cos(πnft + θn) n () Power calculation ( /) C / Ps s( t) dt + 4 n C n f f C 3 / C 4 / (3) Plotting power versus frequency frequency f f 3f 4f /7/6 Dr. shraf S. Hasan Mahmoud 56 8

29 Power Spectral Density Function (3) mathematical expression for PSD(f) can be written as f PSD( f ) Cn / f n f otherwise nother way (more compact) of writing PSD(f) is as follows: PSD( f ) δ ( f ) + Cn δ ( f nf) 4 where δ(t) is defined by δ ( f ) f f /7/6 Dr. shraf S. Hasan Mahmoud 57 n Power Spectral Density Function (4) δ(f) is referred to as the dirac function or unit impulse function δ(f) f /7/6 Dr. shraf S. Hasan Mahmoud 58 9

30 Note on the PSD Function PSD function has units of Watts/Hz For periodic signals PSD is a discrete function - defined for integer multiples of the fundamental frequency Specifies the power contribution of every harmonic component C n / nf he separation between the discrete components is at least f It is exactly f if all C n s are not zeros E.g. for the previous s(t) example, C n for even n separation f /7/6 Dr. shraf S. Hasan Mahmoud 59 Note on the PSD Function () o calculate the total power of signal Integrate PSD over all contained frequencies For discrete PSD: integration summation herefore total power of s(t), P s ( n /) + C n / in Watts /7/6 Dr. shraf S. Hasan Mahmoud 6 3

31 Example 3: Find the PSD function of the periodic signal s(t) considered in Example. From Example, s(t) is given by s t) + π ( ) n ( n ) ( n,3,5 cos(πnf t) Using Example : Power at the zero frequency (/) /4 Power at the nth harmonic (n odd) is equal to /(nπ) Power at the nth harmonic (n even) is zero herefore the PSD function is given by PSD( f ) 4 δ ( f ) + π /7/6 Dr. shraf S. Hasan Mahmoud 6 / n,3,5 δ ( f nf ) n Example 3: cont d he PSD is plotted as shown (, ) PSD( f ) δ ( f ) + 4 π n,3,5 δ ( f nf ) n.5. Power Spectral Density function for s(t) -, frequency - Hz /7/6 Dr. shraf S. Hasan Mahmoud 6 3

32 Example 3: cont d Matlab Code to plot PSD clear all ; ; t -:.:; n_max ; Frequency [::n_max]; PwrSepctralD zeros(size(frequency)); % Record the DC term power at f PwrSepctralD() (/)^; % Record the nth harmonic power at f nf for n::n_max PwrSepctralD(n+) (*/(n*pi))^ / ; end figure() stem(frequency, PwrSepctralD,'rx'); title('power Spectral Density function for s(t) -, '); xlabel('frequency - Hz'); grid he stem function is typically used to plot discrete functions /7/6 Dr. shraf S. Hasan Mahmoud 63 Example 4: his is a typical exam question Problem: Consider the periodic half-wave rectified signal s(t) depicted in figure. Write a mathematical expression for s(t) Calculate the Fourier Series Expansion for s(t) Calculate the total power for s(t) Find n* such that s_e(n*) has 95% of the total power Determine the PSD function for s(t) Plot the PSD function for s(t) s(t) - /7/6 Dr. shraf S. Hasan Mahmoud 64 t 3

33 Example 4: cont d nswer: (a) o write a mathematical expression for s(t), remember that the general form of a sinusoidal function is given by cos(π X Freq X t), or cos(π /Period X t) herefore s(t) is given by s(t) cos(π/ t) -/4 < t /4 /4 < t 3/4 /7/6 Dr. shraf S. Hasan Mahmoud 65 Example 4: cont d nswer: (b) he F.S.E of s(t): he DC term is given by s( t) dt cos(πt / ) dt sin(πt / ) π π s( t) π [ cos(πnf t) + B sin(πnf t ] + ) n n n [ sin( π / ) sin( / ) ] t π t /7/6 Dr. shraf S. Hasan Mahmoud 66 33

34 Example 4: cont d Remember: sin(ax+bx) sin(ax-bx) [cos(ax)cos(bx)] dx (a+b) (a-b) for a b sin(a+/-b) sin(a)cos(b) +/- cos(a)sin(b) nswer: he n term is given by (remember / f ) n s( t)cos(πnf t) dt cos(πt / )cos(πnft) dt sin 4 cos π ( π ( n + ) ft) π ( n + ) f ( nπ / ) ( n + ) cos + sin + 4 ( nπ / ) ( n ) ( π ( n ) ft) π ( n ) f t t /7/6 Dr. shraf S. Hasan Mahmoud his means: the n should be 67 special! For n For n Example 4: cont d But cos(nπ/) n odd, n (-) (+n/) n even herefore n ( π (+ n / ) (+ n / ) ) ( )( ) + ( n + ) ( n ) For n even For n odd, n /7/6 Dr. shraf S. Hasan Mahmoud 68 34

35 Example 4: cont d he expression for n (for even n) can be further simplified to n ( π ( π ( ) π n ( ) ( ) π (+ n / ) (+ n / ) ) ( )( ) + ( n + ) ( n ) (+ n / ) (+ n / ) ) ( n ) + ( )( ) ( n + ) ( n + )( n ) (+ n / ) (+ n / ) [ ( n ) ( ) ( n ) ] + (+ n / ) ( n ) For n even /7/6 Dr. shraf S. Hasan Mahmoud 69 Example 4: cont d n is still not completely specified we still need to calculate it for n; in other words we need to calculate : n s( t)cos(π ft) dt cos(πt / )cos(πf t) herefore: cos (πf t) dt t + sin 4 πf ( 4πf t) t sin + 4 /7/6 Dr. shraf S. Hasan Mahmoud 7 dt ( π ) sin( π ) 8πf t 35

36 Example 4: cont d his mean n is equal to the following: n /π n n odd, n / n (-) (+n/) n, 4, 6, π(n -) he above expression specifies n for LL POSSIBLE values of n specification is complete /7/6 Dr. shraf S. Hasan Mahmoud 7 Example 4: cont d We still need to compute B n : B n cos 4 Remember: - cos(ax+bx) cos(ax-bx) [sin(ax)cos(bx)] dx (a+b) (a-b) for a b s( t)sin(πnf t) dt cos(πt / )sin(πnft) dt ( π ( n + ) ft) π ( n + ) f cos 4 ( π / ( n + ) ) + cos( π / ( n + ) ) ( n + ) ( π ( n ) ft) π ( n ) f t cos cos π n t For n ( π / ( n ) ) cos( π / ( n ) ) ( ) For n /7/6 Dr. shraf S. Hasan Mahmoud his means: the n should be 7 special! 36

37 Remember: Example 4: cont d sin(ax) cos(ax) sin(ax) B B n is still NO completely specified we still need to calculate it for n; in other words we need to calculate B : n s( t)sin(π ft) dt cos(πt / )sin(πf t) herefore: B cos(πf t)sin(πf t) dt sin(4πf t) t cos(4πf t) π t 4π 4π [ cos( π ) cos( )] his means B n for all n /7/6 Dr. shraf S. Hasan Mahmoud 73 dt dt Example 4: cont d o summarize: n /π n n odd, n / n nd (-) (+n/) n, 4, 6, π(n -) B n for all n Having computed n and B n we are now in a position to write the Fourier Series Expansion for s(t) /7/6 Dr. shraf S. Hasan Mahmoud 74 37

38 Example 4: cont d he Fourier Series Expansion for s(t) is given by s( t) [ cos(πnf t) + B sin(πnf t ] + ) n n n + π ( ) (+ n / ) cos(πf t) + cos(πnf t) π n,4,6 n he C n terms (there is a typo in the textbook) are as follows: C /π C / (-) (+n/) C n , n, 4, 6, π(n ) /7/6 Dr. shraf S. Hasan Mahmoud n odd, n 75 Remember: Example 4: cont d sin(ax) ½ cos(ax) sin(ax) Plot for s(t) and the Fourier Series Expansion for k,,, and 4. Original signal and its Fourier Series Expansion orignal s(t) s e (k) s e (k) s e (k) s e (k4).8 Note: s k increases s_e(nk) approaches the original s(t) mplitude ime (sec) /7/6 Dr. shraf S. Hasan Mahmoud 76 38

39 Example 4: cont d he total power of s(t) is given by: P s 3 s( t) dt t sin(4πt / ) + 8 t / π cos (πt / ) t t 4 herefore total power of s(t).5 /7/6 Dr. shraf S. Hasan Mahmoud 77 Example 4: cont d o find n* such that power of s_e(nn*) 95% of total power: s_e(nk) Expression Power % Power + k /π.3 (.3 )/(.5 ) 4.5% k /π + / cos(πf t).63 (.6 )/(.5 ) 9.5% k /π + / cos(πf t) + /(3π) cos(πf t).488 (.488 )/(.5 ) 99.5% herefore n* power of s_e(n).488 which is 99.5% of total power of s(t) /7/6 Dr. shraf S. Hasan Mahmoud 78 39

40 Example 4: cont d he PSD function for s(t) is as follows: Power for DC term (/π) Power for harmonic at f f : (/) / /8 Power for harmonic at f nf (n,4,6, ): [/(π(n -))] / /(π(n -)) herefore PSD function equals to PSD( f ) δ ( f ) + π δ ( f 8 f ) + π δ ( f nf ) n,4,6 ( n ) /7/6 Dr. shraf S. Hasan Mahmoud 79 Example 4: cont d Plot of he PSD function for s(t).4.. Power spectral density for s(t) Power - Watts Multiples of fundamental freuqncy f (Hz) /7/6 Dr. shraf S. Hasan Mahmoud 8 4

41 Fourier ransform Fourier Series Expansion analysis is applicable for PERIODIC signals ONLY here are important signals that are not periodic such as Your voice waveform Pulse signal p(t) used for modulation and transmission Examples: p (t) and p (t) p (t) p (t) τ/ τ/ t /7/6 Dr. shraf S. Hasan Mahmoud τ/ τ/ 8 t Fourier ransform () How to find the frequency content of such signals? Use FOURIER RNSFORM X ( f ) πjft x( t) e dt πjft x( t) X ( f ) e df /7/6 Dr. shraf S. Hasan Mahmoud 8 4

42 Notes on Fourier ransform F. describes a two-way transformation x(t) X(f) where x(t) is the time representation of the signal, while X(f) is the frequency representation of the signal X(f) is defined on a continuous range of frequencies ll frequencies within the range of X(f) where X(f) is not zero contribute towards building x(t) /7/6 Dr. shraf S. Hasan Mahmoud 83 Notes on Fourier ransform () he magnitude of the contribution of a particular frequency f* in x(t) is proportional to X(f*) Example: Consider the F.. pair shown below clearly frequencies belonging to (-/τ,/τ) contribute significantly more compared to frequencies belonging to (/τ, ) or (-,-/τ) x(t) X(f) F.. τ/ τ/ t -/τ /τ f /7/6 Dr. shraf S. Hasan Mahmoud 84 4

43 Properties of Fourier ransform If x(t) is time-limited X(f) is not frequency-limited i.e. the range of X(f) (-, ) X(f) is complex-valued (has magnitude and phase) in general, i.e. () C If x(t) is a real-valued symmetric X(f) is real-valued, i.e. () R /7/6 Dr. shraf S. Hasan Mahmoud 85 Relation between Fourier Series Expansion and Fourier ransform Consider the following two signals: s (t) x(t) is the same as s(t) except that its period x(t) -/4 /4 3/4 5/4 t τ/ τ/ t S(f) For S(f) Separation between the discrete frequencies equal to f or / X(f) -3/ -/ / -/τ /τ 3/ f f -4/ -/ 4/ Separation become zero as and the / discrete function S(f) continuous function X(f) /7/6 Dr. shraf S. Hasan Mahmoud 86 43

44 Relation between Fourier Series Expansion and Fourier ransform () he separation between spectral lines for a periodic signal is / s infinity and s(t) becomes non periodic the separation between spectral lines zero (i.e. it becomes continuous) /7/6 Dr. shraf S. Hasan Mahmoud 87 Example 5: Problem: Consider the square pulse function shown in figure: Write a mathematical expression for p(t) Find the Fourier transform for p(t) Plot P(f) p(t) -τ/ τ/ t /7/6 Dr. shraf S. Hasan Mahmoud 88 44

45 Example 5: cont d nswer: p(t) can be expressed as p(t) t τ/ otherwise he F.. for p(t), P(f) is given by P( f ) πjft p( t) e dt /7/6 Dr. shraf S. Hasan Mahmoud 89 P(f) is real-valued for this specific example of p(t); why? Example 5: cont d Which is equal to P( f ) p( t) e dt πjf πf τ πjft πjft e τ τ πjft e dt τ πjfτ πjfτ ( e e ) j sin( πfτ ) τ πfτ /7/6 Dr. shraf S. Hasan Mahmoud 9 dt πjf πjfτ πjfτ ( e e ) Remember: Euler identity : e jx cos(x) + j sin(x), OR cos(x) (e jx +e -jx )/ sin(x) (e jx -e -jx )/(j) 45

46 Example 5: cont d P(f) plot for and τ Note: P(f) is define on (-, ) P(f) is continuous (except at f Hz) P(f) ZERO for f n/τ Fourier ransform of p(t) -, aw For practical pulses P(f) approaches zero as f ±. Most of the energy of p(t) is contained in the period of (-/τ, /τ) frequency - Hz /7/6 Dr. shraf S. Hasan Mahmoud 9 Energy Spectral Density Function (ESDF) ESDF is defined as () () () where P(f) is the F.. of the pulse p(t). P*(f) is the complex conjugate of P(f). ESDF is a measure of how much energy is contained at a particular frequency f Units of ESDF is Joules per Hz How would you compare ESDF with PSDF? /7/6 Dr. shraf S. Hasan Mahmoud 9 46

47 Example 5 (For Volts and aw sec) - cont d.8 (a) pulse (time domain).8 (b) Magnitude of F. (freq. domain) amplide (volts).6.4. abs(p(f)) time - (sec) -4-4 frequency - (Hz) < () otherwise () () (a) sin() () () () sin() -4-4 /7/6 Dr. shraf S. Hasan Mahmoud frequency - (Hz) 93 (b) (c) ESDP (Joules/Hz) (c) ESDF (freq. domain) Example 5 (For Volts and aw sec) Matlab Code Code for producing plots on previous slide clear all; LineWidth 3; FontSize 4; %Example of rectangular pulse ; aw ; % parameters for the rectangle pulse t_step.; f_step.; Nmax 4; t -aw:t_step:aw; % define the time axis f -Nmax/aw:f_step:Nmax/aw; % define the frequency axis p_t *rectpuls(t/aw); % he rectangle pulse of height and width aw P_f *aw*sin(pi*aw*f)./(pi*aw*f); % he corresponding F. P(f) ESDF_f P_f.*conj(P_f)/(*pi); % he ESDF figure(); clf; set(gca, 'FontSize', FontSize); h plot(t, p_t, '-r', 'LineWidth', LineWidth); xlabel('time - (sec)'); ylabel('amplide (volts)'); grid on; figure(); clf; set(gca, 'FontSize', FontSize); h plot(f, abs(p_f), '-r', 'LineWidth', LineWidth); xlabel('frequency - (Hz)'); ylabel('abs(p(f))'); grid on; figure(3); clf; set(gca, 'FontSize', FontSize); h plot(f, ESDF_f, '-r', 'LineWidth', LineWidth); xlabel('frequency - (Hz)'); ylabel('esdp (Joules/Hz)'); grid on; /7/6 Dr. shraf S. Hasan Mahmoud 94 47

48 Example 6: Repeat example 5 for triangular pulse shown in textbook Figure. page 839. Let be equal to seconds and be equal to 3 volts. /7/6 Dr. shraf S. Hasan Mahmoud 95 Example 7: Problem: If the FSE expansion for the function g(t) is as given below. Compute the FSE for the function s(t) without computing the FSE coefficients for s(t). g(t) s(t) -Τ/ Τ/ t -Τ/ Τ/ t /7/6 Dr. shraf S. Hasan Mahmoud 48

49 Z-ransform Digital signals Discrete-time signals sampled continues-time signals E.g. I/O signal used by micro-controllers Systems described by difference equations E.g. CD player contains digital signal processing system (digital filter) to manipulate the digital audio signal For such systems input and output are related by difference equations and the Z- transform is used to solve these systems /7/6 Dr. shraf S. Hasan Mahmoud 97 Z-ransform - Introduction For Modern systems analog signal /D samples Signal processor samples D/ analog output processing filtering noise, equalizing music, adding effects to audio/video, etc. /7/6 Dr. shraf S. Hasan Mahmoud 98 49

50 Z-ransform - Definition Let y(t) be a continuous-time signal (function) Define sampling period hen y(k) y k y(k) for k,,, 3, defines uniformly spaced samples of the original signal y(t) he Z-ransform for yk is defined as () if the summation converges /7/6 Dr. shraf S. Hasan Mahmoud 99 Z-ransform Example Compute the Z-transform for the sequence () for k,,, and <a< Compute the Z-transform for the sequence plot for y(k) is shown for < a < Note the y(k) is defined only on specific indices (time samples) pplying the definition () for a/z < sample index (k) /7/6 Dr. shraf S. Hasan Mahmoud for k,,, signal y(k) ( ) y and a.5 pair () 5

51 Z-ransform Example Compute the Z-transform for the sequence () (.9) for k,,, and <a< Compute the Z-transform for the sequence plot for y(k) is shown for < a < Using the previous result for.9/z <. () signal y(k) y and a sample index (k) /7/6 Dr. shraf S. Hasan Mahmoud Z-ransform Example 3 Compute the Z-transform for the sequence () Compute the Z-transform for the sequence Using the definition for all z. Δ() -5 5 sample index (k) /7/6 Dr. shraf S. Hasan Mahmoud signal δ(k) () () Discrete-time Delta Function () pair () 5

52 Z-ransform Example 3 Compute the Z-transform for the sequence (),,, otherwise Compute the Z-transform for the sequence Using the definition Discrete-time Unit-Step Function signal δ(k) sample index (k) () () for /z <. () pair (3) /7/6 Dr. shraf S. Hasan Mahmoud 3 Z-ransform Example 4 Compute the Z-transform for the sequence Discrete-time arbitrary function 6 5 y(k) [, 4, 6, 4,, ] for k,,, 3, 4, and 5, respectively Compute the Z-transform for the sequence signal δ(k) 4 3 Using the definition () for /z <. () sample index (k) /7/6 Dr. shraf S. Hasan Mahmoud 4 5

53 Inverse Z-ransform Example 5 Compute the Inverse Z-ransform for We use pair () y and a 3 Or y(k) is given by for k,,, () (.3).3 y(k) may be rewritten as (.3) () /7/6 Dr. shraf S. Hasan Mahmoud 5 Inverse Z-ransform Example 6 Compute the Inverse Z-ransform for Solution? () (.3)(.9) /7/6 Dr. shraf S. Hasan Mahmoud 6 53

ω 0 = 2π/T 0 is called the fundamental angular frequency and ω 2 = 2ω 0 is called the

ω 0 = 2π/T 0 is called the fundamental angular frequency and ω 2 = 2ω 0 is called the he ime-frequency Concept []. Review of Fourier Series Consider the following set of time functions {3A sin t, A sin t}. We can represent these functions in different ways by plotting the amplitude versus

More information

ENSC327 Communications Systems 2: Fourier Representations. Jie Liang School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. Jie Liang School of Engineering Science Simon Fraser University ENSC327 Communications Systems 2: Fourier Representations Jie Liang School of Engineering Science Simon Fraser University 1 Outline Chap 2.1 2.5: Signal Classifications Fourier Transform Dirac Delta Function

More information

E2.5 Signals & Linear Systems. Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & 2)

E2.5 Signals & Linear Systems. Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & 2) E.5 Signals & Linear Systems Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & ) 1. Sketch each of the following continuous-time signals, specify if the signal is periodic/non-periodic,

More information

LOPE3202: Communication Systems 10/18/2017 2

LOPE3202: Communication Systems 10/18/2017 2 By Lecturer Ahmed Wael Academic Year 2017-2018 LOPE3202: Communication Systems 10/18/2017 We need tools to build any communication system. Mathematics is our premium tool to do work with signals and systems.

More information

EA2.3 - Electronics 2 1

EA2.3 - Electronics 2 1 In the previous lecture, I talked about the idea of complex frequency s, where s = σ + jω. Using such concept of complex frequency allows us to analyse signals and systems with better generality. In this

More information

Fourier Analysis and Power Spectral Density

Fourier Analysis and Power Spectral Density Chapter 4 Fourier Analysis and Power Spectral Density 4. Fourier Series and ransforms Recall Fourier series for periodic functions for x(t + ) = x(t), where x(t) = 2 a + a = 2 a n = 2 b n = 2 n= a n cos

More information

Review of Fourier Transform

Review of Fourier Transform Review of Fourier Transform Fourier series works for periodic signals only. What s about aperiodic signals? This is very large & important class of signals Aperiodic signal can be considered as periodic

More information

Assignment 3 Solutions

Assignment 3 Solutions Assignment Solutions Networks and systems August 8, 7. Consider an LTI system with transfer function H(jw) = input is sin(t + π 4 ), what is the output? +jw. If the Solution : C For an LTI system with

More information

Digital Signal Processing

Digital Signal Processing Digital Signal Processing Introduction Moslem Amiri, Václav Přenosil Embedded Systems Laboratory Faculty of Informatics, Masaryk University Brno, Czech Republic amiri@mail.muni.cz prenosil@fi.muni.cz February

More information

EE303: Communication Systems

EE303: Communication Systems EE303: Communication Systems Professor A. Manikas Chair of Communications and Array Processing Imperial College London Introductory Concepts Prof. A. Manikas (Imperial College) EE303: Introductory Concepts

More information

EE 3054: Signals, Systems, and Transforms Summer It is observed of some continuous-time LTI system that the input signal.

EE 3054: Signals, Systems, and Transforms Summer It is observed of some continuous-time LTI system that the input signal. EE 34: Signals, Systems, and Transforms Summer 7 Test No notes, closed book. Show your work. Simplify your answers. 3. It is observed of some continuous-time LTI system that the input signal = 3 u(t) produces

More information

2.3 Oscillation. The harmonic oscillator equation is the differential equation. d 2 y dt 2 r y (r > 0). Its solutions have the form

2.3 Oscillation. The harmonic oscillator equation is the differential equation. d 2 y dt 2 r y (r > 0). Its solutions have the form 2. Oscillation So far, we have used differential equations to describe functions that grow or decay over time. The next most common behavior for a function is to oscillate, meaning that it increases and

More information

GATE EE Topic wise Questions SIGNALS & SYSTEMS

GATE EE Topic wise Questions SIGNALS & SYSTEMS www.gatehelp.com GATE EE Topic wise Questions YEAR 010 ONE MARK Question. 1 For the system /( s + 1), the approximate time taken for a step response to reach 98% of the final value is (A) 1 s (B) s (C)

More information

Solutions to Problems in Chapter 4

Solutions to Problems in Chapter 4 Solutions to Problems in Chapter 4 Problems with Solutions Problem 4. Fourier Series of the Output Voltage of an Ideal Full-Wave Diode Bridge Rectifier he nonlinear circuit in Figure 4. is a full-wave

More information

Properties of Fourier Series - GATE Study Material in PDF

Properties of Fourier Series - GATE Study Material in PDF Properties of Fourier Series - GAE Study Material in PDF In the previous article, we learnt the Basics of Fourier Series, the different types and all about the different Fourier Series spectrums. Now,

More information

Each of these functions represents a signal in terms of its spectral components in the frequency domain.

Each of these functions represents a signal in terms of its spectral components in the frequency domain. N INTRODUCTION TO SPECTRL FUNCTIONS Revision B By Tom Irvine Email: tomirvine@aol.com March 3, 000 INTRODUCTION This tutorial presents the Fourier transform. It also discusses the power spectral density

More information

Topic 3: Fourier Series (FS)

Topic 3: Fourier Series (FS) ELEC264: Signals And Systems Topic 3: Fourier Series (FS) o o o o Introduction to frequency analysis of signals CT FS Fourier series of CT periodic signals Signal Symmetry and CT Fourier Series Properties

More information

Chapter 1 Fundamental Concepts

Chapter 1 Fundamental Concepts Chapter 1 Fundamental Concepts Signals A signal is a pattern of variation of a physical quantity as a function of time, space, distance, position, temperature, pressure, etc. These quantities are usually

More information

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University ENSC37 Communications Systems : Fourier Representations School o Engineering Science Simon Fraser University Outline Chap..5: Signal Classiications Fourier Transorm Dirac Delta Function Unit Impulse Fourier

More information

Tutorial Sheet #2 discrete vs. continuous functions, periodicity, sampling

Tutorial Sheet #2 discrete vs. continuous functions, periodicity, sampling 2.39 utorial Sheet #2 discrete vs. continuous functions, periodicity, sampling We will encounter two classes of signals in this class, continuous-signals and discrete-signals. he distinct mathematical

More information

CMPT 889: Lecture 3 Fundamentals of Digital Audio, Discrete-Time Signals

CMPT 889: Lecture 3 Fundamentals of Digital Audio, Discrete-Time Signals CMPT 889: Lecture 3 Fundamentals of Digital Audio, Discrete-Time Signals Tamara Smyth, tamaras@cs.sfu.ca School of Computing Science, Simon Fraser University October 6, 2005 1 Sound Sound waves are longitudinal

More information

2 Frequency-Domain Analysis

2 Frequency-Domain Analysis 2 requency-domain Analysis Electrical engineers live in the two worlds, so to speak, of time and frequency. requency-domain analysis is an extremely valuable tool to the communications engineer, more so

More information

Lecture 27 Frequency Response 2

Lecture 27 Frequency Response 2 Lecture 27 Frequency Response 2 Fundamentals of Digital Signal Processing Spring, 2012 Wei-Ta Chu 2012/6/12 1 Application of Ideal Filters Suppose we can generate a square wave with a fundamental period

More information

EE401: Advanced Communication Theory

EE401: Advanced Communication Theory EE401: Advanced Communication Theory Professor A. Manikas Chair of Communications and Array Processing Imperial College London Introductory Concepts Prof. A. Manikas (Imperial College) EE.401: Introductory

More information

Chapter 2. Signals. Static and Dynamic Characteristics of Signals. Signals classified as

Chapter 2. Signals. Static and Dynamic Characteristics of Signals. Signals classified as Chapter 2 Static and Dynamic Characteristics of Signals Signals Signals classified as. Analog continuous in time and takes on any magnitude in range of operations 2. Discrete Time measuring a continuous

More information

Correlation, discrete Fourier transforms and the power spectral density

Correlation, discrete Fourier transforms and the power spectral density Correlation, discrete Fourier transforms and the power spectral density visuals to accompany lectures, notes and m-files by Tak Igusa tigusa@jhu.edu Department of Civil Engineering Johns Hopkins University

More information

Ver 3808 E1.10 Fourier Series and Transforms (2014) E1.10 Fourier Series and Transforms. Problem Sheet 1 (Lecture 1)

Ver 3808 E1.10 Fourier Series and Transforms (2014) E1.10 Fourier Series and Transforms. Problem Sheet 1 (Lecture 1) Ver 88 E. Fourier Series and Transforms 4 Key: [A] easy... [E]hard Questions from RBH textbook: 4., 4.8. E. Fourier Series and Transforms Problem Sheet Lecture. [B] Using the geometric progression formula,

More information

Signals and Systems: Part 2

Signals and Systems: Part 2 Signals and Systems: Part 2 The Fourier transform in 2πf Some important Fourier transforms Some important Fourier transform theorems Convolution and Modulation Ideal filters Fourier transform definitions

More information

Figure 3.1 Effect on frequency spectrum of increasing period T 0. Consider the amplitude spectrum of a periodic waveform as shown in Figure 3.2.

Figure 3.1 Effect on frequency spectrum of increasing period T 0. Consider the amplitude spectrum of a periodic waveform as shown in Figure 3.2. 3. Fourier ransorm From Fourier Series to Fourier ransorm [, 2] In communication systems, we oten deal with non-periodic signals. An extension o the time-requency relationship to a non-periodic signal

More information

Wave Phenomena Physics 15c. Lecture 10 Fourier Transform

Wave Phenomena Physics 15c. Lecture 10 Fourier Transform Wave Phenomena Physics 15c Lecture 10 Fourier ransform What We Did Last ime Reflection of mechanical waves Similar to reflection of electromagnetic waves Mechanical impedance is defined by For transverse/longitudinal

More information

I. Signals & Sinusoids

I. Signals & Sinusoids I. Signals & Sinusoids [p. 3] Signal definition Sinusoidal signal Plotting a sinusoid [p. 12] Signal operations Time shifting Time scaling Time reversal Combining time shifting & scaling [p. 17] Trigonometric

More information

CHAPTER 4 FOURIER SERIES S A B A R I N A I S M A I L

CHAPTER 4 FOURIER SERIES S A B A R I N A I S M A I L CHAPTER 4 FOURIER SERIES 1 S A B A R I N A I S M A I L Outline Introduction of the Fourier series. The properties of the Fourier series. Symmetry consideration Application of the Fourier series to circuit

More information

Problem Sheet 1 Examples of Random Processes

Problem Sheet 1 Examples of Random Processes RANDOM'PROCESSES'AND'TIME'SERIES'ANALYSIS.'PART'II:'RANDOM'PROCESSES' '''''''''''''''''''''''''''''''''''''''''''''''''''''''''''''''''Problem'Sheets' Problem Sheet 1 Examples of Random Processes 1. Give

More information

ECE6604 PERSONAL & MOBILE COMMUNICATIONS. Week 3. Flat Fading Channels Envelope Distribution Autocorrelation of a Random Process

ECE6604 PERSONAL & MOBILE COMMUNICATIONS. Week 3. Flat Fading Channels Envelope Distribution Autocorrelation of a Random Process 1 ECE6604 PERSONAL & MOBILE COMMUNICATIONS Week 3 Flat Fading Channels Envelope Distribution Autocorrelation of a Random Process 2 Multipath-Fading Mechanism local scatterers mobile subscriber base station

More information

EE5713 : Advanced Digital Communications

EE5713 : Advanced Digital Communications EE5713 : Advanced Digital Communications Week 12, 13: Inter Symbol Interference (ISI) Nyquist Criteria for ISI Pulse Shaping and Raised-Cosine Filter Eye Pattern Equalization (On Board) 20-May-15 Muhammad

More information

(Refer Slide Time: 01:30)

(Refer Slide Time: 01:30) Networks and Systems Prof V.G K.Murti Department of Electrical Engineering Indian Institute of Technology, Madras Lecture - 11 Fourier Series (5) Continuing our discussion of Fourier series today, we will

More information

Summary of Fourier Transform Properties

Summary of Fourier Transform Properties Summary of Fourier ransform Properties Frank R. Kschischang he Edward S. Rogers Sr. Department of Electrical and Computer Engineering University of oronto January 7, 207 Definition and Some echnicalities

More information

Chapter 2: The Fourier Transform

Chapter 2: The Fourier Transform EEE, EEE Part A : Digital Signal Processing Chapter Chapter : he Fourier ransform he Fourier ransform. Introduction he sampled Fourier transform of a periodic, discrete-time signal is nown as the discrete

More information

Review Quantitative Aspects of Networking. Decibels, Power, and Waves John Marsh

Review Quantitative Aspects of Networking. Decibels, Power, and Waves John Marsh Review Quantitative spects of Networking Decibels, ower, and Waves John Marsh Outline Review of quantitative aspects of networking Metric system Numbers with Units Math review exponents and logs Decibel

More information

1 Understanding Sampling

1 Understanding Sampling 1 Understanding Sampling Summary. In Part I, we consider the analysis of discrete-time signals. In Chapter 1, we consider how discretizing a signal affects the signal s Fourier transform. We derive the

More information

OSE801 Engineering System Identification. Lecture 05: Fourier Analysis

OSE801 Engineering System Identification. Lecture 05: Fourier Analysis OSE81 Engineering System Identification Lecture 5: Fourier Analysis What we will study in this lecture: A short introduction of Fourier analysis Sampling the data Applications Example 1 Fourier Analysis

More information

EE4061 Communication Systems

EE4061 Communication Systems EE4061 Communication Systems Week 11 Intersymbol Interference Nyquist Pulse Shaping 0 c 2015, Georgia Institute of Technology (lect10 1) Intersymbol Interference (ISI) Tx filter channel Rx filter a δ(t-nt)

More information

Lecture 8 ELE 301: Signals and Systems

Lecture 8 ELE 301: Signals and Systems Lecture 8 ELE 30: Signals and Systems Prof. Paul Cuff Princeton University Fall 20-2 Cuff (Lecture 7) ELE 30: Signals and Systems Fall 20-2 / 37 Properties of the Fourier Transform Properties of the Fourier

More information

LINEAR SYSTEMS. J. Elder PSYC 6256 Principles of Neural Coding

LINEAR SYSTEMS. J. Elder PSYC 6256 Principles of Neural Coding LINEAR SYSTEMS Linear Systems 2 Neural coding and cognitive neuroscience in general concerns input-output relationships. Inputs Light intensity Pre-synaptic action potentials Number of items in display

More information

Lab Fourier Analysis Do prelab before lab starts. PHSX 262 Spring 2011 Lecture 5 Page 1. Based with permission on lectures by John Getty

Lab Fourier Analysis Do prelab before lab starts. PHSX 262 Spring 2011 Lecture 5 Page 1. Based with permission on lectures by John Getty Today /5/ Lecture 5 Fourier Series Time-Frequency Decomposition/Superposition Fourier Components (Ex. Square wave) Filtering Spectrum Analysis Windowing Fast Fourier Transform Sweep Frequency Analyzer

More information

PART 1. Review of DSP. f (t)e iωt dt. F(ω) = f (t) = 1 2π. F(ω)e iωt dω. f (t) F (ω) The Fourier Transform. Fourier Transform.

PART 1. Review of DSP. f (t)e iωt dt. F(ω) = f (t) = 1 2π. F(ω)e iωt dω. f (t) F (ω) The Fourier Transform. Fourier Transform. PART 1 Review of DSP Mauricio Sacchi University of Alberta, Edmonton, AB, Canada The Fourier Transform F() = f (t) = 1 2π f (t)e it dt F()e it d Fourier Transform Inverse Transform f (t) F () Part 1 Review

More information

Mathematics for Engineers II. lectures. Power series, Fourier series

Mathematics for Engineers II. lectures. Power series, Fourier series Power series, Fourier series Power series, Taylor series It is a well-known fact, that 1 + x + x 2 + x 3 + = n=0 x n = 1 1 x if 1 < x < 1. On the left hand side of the equation there is sum containing

More information

A3. Frequency Representation of Continuous Time and Discrete Time Signals

A3. Frequency Representation of Continuous Time and Discrete Time Signals A3. Frequency Representation of Continuous Time and Discrete Time Signals Objectives Define the magnitude and phase plots of continuous time sinusoidal signals Extend the magnitude and phase plots to discrete

More information

CMPT 889: Lecture 2 Sinusoids, Complex Exponentials, Spectrum Representation

CMPT 889: Lecture 2 Sinusoids, Complex Exponentials, Spectrum Representation CMPT 889: Lecture 2 Sinusoids, Complex Exponentials, Spectrum Representation Tamara Smyth, tamaras@cs.sfu.ca School of Computing Science, Simon Fraser University September 26, 2005 1 Sinusoids Sinusoids

More information

In this Lecture. Frequency domain analysis

In this Lecture. Frequency domain analysis In this Lecture Frequency domain analysis Introduction In most cases we want to know the frequency content of our signal Why? Most popular analysis in frequency domain is based on work of Joseph Fourier

More information

LECTURE 12 Sections Introduction to the Fourier series of periodic signals

LECTURE 12 Sections Introduction to the Fourier series of periodic signals Signals and Systems I Wednesday, February 11, 29 LECURE 12 Sections 3.1-3.3 Introduction to the Fourier series of periodic signals Chapter 3: Fourier Series of periodic signals 3. Introduction 3.1 Historical

More information

ESE 250: Digital Audio Basics. Week 4 February 5, The Frequency Domain. ESE Spring'13 DeHon, Kod, Kadric, Wilson-Shah

ESE 250: Digital Audio Basics. Week 4 February 5, The Frequency Domain. ESE Spring'13 DeHon, Kod, Kadric, Wilson-Shah ESE 250: Digital Audio Basics Week 4 February 5, 2013 The Frequency Domain 1 Course Map 2 Musical Representation With this compact notation Could communicate a sound to pianist Much more compact than 44KHz

More information

Phasor mathematics. Resources and methods for learning about these subjects (list a few here, in preparation for your research):

Phasor mathematics. Resources and methods for learning about these subjects (list a few here, in preparation for your research): Phasor mathematics This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,

More information

ECE 301 Fall 2011 Division 1. Homework 1 Solutions.

ECE 301 Fall 2011 Division 1. Homework 1 Solutions. ECE 3 Fall 2 Division. Homework Solutions. Reading: Course information handout on the course website; textbook sections.,.,.2,.3,.4; online review notes on complex numbers. Problem. For each discrete-time

More information

Problem Value

Problem Value GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL of ELECTRICAL & COMPUTER ENGINEERING FINAL EXAM DATE: 30-Apr-04 COURSE: ECE-2025 NAME: GT #: LAST, FIRST Recitation Section: Circle the date & time when your Recitation

More information

Square Root Raised Cosine Filter

Square Root Raised Cosine Filter Wireless Information Transmission System Lab. Square Root Raised Cosine Filter Institute of Communications Engineering National Sun Yat-sen University Introduction We consider the problem of signal design

More information

Fourier Series and Transforms. Revision Lecture

Fourier Series and Transforms. Revision Lecture E. (5-6) : / 3 Periodic signals can be written as a sum of sine and cosine waves: u(t) u(t) = a + n= (a ncosπnft+b n sinπnft) T = + T/3 T/ T +.65sin(πFt) -.6sin(πFt) +.6sin(πFt) + -.3cos(πFt) + T/ Fundamental

More information

Fourier Transform. Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function

Fourier Transform. Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function Objectives: Be able to Fourier Transform Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function Filters with a Single Sinusoidal Input: Suppose

More information

Distortion Analysis T

Distortion Analysis T EE 435 Lecture 32 Spectral Performance Windowing Spectral Performance of Data Converters - Time Quantization - Amplitude Quantization Quantization Noise . Review from last lecture. Distortion Analysis

More information

EE301 Signals and Systems In-Class Exam Exam 3 Thursday, Apr. 19, Cover Sheet

EE301 Signals and Systems In-Class Exam Exam 3 Thursday, Apr. 19, Cover Sheet EE301 Signals and Systems In-Class Exam Exam 3 Thursday, Apr. 19, 2012 Cover Sheet Test Duration: 75 minutes. Coverage: Chaps. 5,7 Open Book but Closed Notes. One 8.5 in. x 11 in. crib sheet Calculators

More information

Mathematics for Chemists 2 Lecture 14: Fourier analysis. Fourier series, Fourier transform, DFT/FFT

Mathematics for Chemists 2 Lecture 14: Fourier analysis. Fourier series, Fourier transform, DFT/FFT Mathematics for Chemists 2 Lecture 14: Fourier analysis Fourier series, Fourier transform, DFT/FFT Johannes Kepler University Summer semester 2012 Lecturer: David Sevilla Fourier analysis 1/25 Remembering

More information

SEISMIC WAVE PROPAGATION. Lecture 2: Fourier Analysis

SEISMIC WAVE PROPAGATION. Lecture 2: Fourier Analysis SEISMIC WAVE PROPAGATION Lecture 2: Fourier Analysis Fourier Series & Fourier Transforms Fourier Series Review of trigonometric identities Analysing the square wave Fourier Transform Transforms of some

More information

The (Fast) Fourier Transform

The (Fast) Fourier Transform The (Fast) Fourier Transform The Fourier transform (FT) is the analog, for non-periodic functions, of the Fourier series for periodic functions can be considered as a Fourier series in the limit that the

More information

Homework 9 Solutions

Homework 9 Solutions 8-290 Signals and Systems Profs. Byron Yu and Pulkit Grover Fall 207 Homework 9 Solutions Part One. (6 points) Compute the convolution of the following continuous-time aperiodic signals. (Hint: Use the

More information

MATHEMATICAL TOOLS FOR DIGITAL TRANSMISSION ANALYSIS

MATHEMATICAL TOOLS FOR DIGITAL TRANSMISSION ANALYSIS ch03.qxd 1/9/03 09:14 AM Page 35 CHAPTER 3 MATHEMATICAL TOOLS FOR DIGITAL TRANSMISSION ANALYSIS 3.1 INTRODUCTION The study of digital wireless transmission is in large measure the study of (a) the conversion

More information

Line Codes and Pulse Shaping Review. Intersymbol interference (ISI) Pulse shaping to reduce ISI Embracing ISI

Line Codes and Pulse Shaping Review. Intersymbol interference (ISI) Pulse shaping to reduce ISI Embracing ISI Line Codes and Pulse Shaping Review Line codes Pulse width and polarity Power spectral density Intersymbol interference (ISI) Pulse shaping to reduce ISI Embracing ISI Line Code Examples (review) on-off

More information

L6: Short-time Fourier analysis and synthesis

L6: Short-time Fourier analysis and synthesis L6: Short-time Fourier analysis and synthesis Overview Analysis: Fourier-transform view Analysis: filtering view Synthesis: filter bank summation (FBS) method Synthesis: overlap-add (OLA) method STFT magnitude

More information

EE482: Digital Signal Processing Applications

EE482: Digital Signal Processing Applications Professor Brendan Morris, SEB 3216, brendan.morris@unlv.edu EE482: Digital Signal Processing Applications Spring 2014 TTh 14:30-15:45 CBC C222 Lecture 02 DSP Fundamentals 14/01/21 http://www.ee.unlv.edu/~b1morris/ee482/

More information

Example: Bipolar NRZ (non-return-to-zero) signaling

Example: Bipolar NRZ (non-return-to-zero) signaling Baseand Data Transmission Data are sent without using a carrier signal Example: Bipolar NRZ (non-return-to-zero signaling is represented y is represented y T A -A T : it duration is represented y BT. Passand

More information

Sinusoids. Amplitude and Magnitude. Phase and Period. CMPT 889: Lecture 2 Sinusoids, Complex Exponentials, Spectrum Representation

Sinusoids. Amplitude and Magnitude. Phase and Period. CMPT 889: Lecture 2 Sinusoids, Complex Exponentials, Spectrum Representation Sinusoids CMPT 889: Lecture Sinusoids, Complex Exponentials, Spectrum Representation Tamara Smyth, tamaras@cs.sfu.ca School of Computing Science, Simon Fraser University September 6, 005 Sinusoids are

More information

Signals and Systems Lecture Notes

Signals and Systems Lecture Notes Dr. Mahmoud M. Al-Husari Signals and Systems Lecture Notes This set of lecture notes are never to be considered as a substitute to the textbook recommended by the lecturer. ii Contents Preface v 1 Introduction

More information

SIGNALS AND SYSTEMS: PAPER 3C1 HANDOUT 6a. Dr David Corrigan 1. Electronic and Electrical Engineering Dept.

SIGNALS AND SYSTEMS: PAPER 3C1 HANDOUT 6a. Dr David Corrigan 1. Electronic and Electrical Engineering Dept. SIGNALS AND SYSTEMS: PAPER 3C HANDOUT 6a. Dr David Corrigan. Electronic and Electrical Engineering Dept. corrigad@tcd.ie www.mee.tcd.ie/ corrigad FOURIER SERIES Have seen how the behaviour of systems can

More information

Lecture 5. The Digital Fourier Transform. (Based, in part, on The Scientist and Engineer's Guide to Digital Signal Processing by Steven Smith)

Lecture 5. The Digital Fourier Transform. (Based, in part, on The Scientist and Engineer's Guide to Digital Signal Processing by Steven Smith) Lecture 5 The Digital Fourier Transform (Based, in part, on The Scientist and Engineer's Guide to Digital Signal Processing by Steven Smith) 1 -. 8 -. 6 -. 4 -. 2-1 -. 8 -. 6 -. 4 -. 2 -. 2. 4. 6. 8 1

More information

Problem Set 8 Mar 5, 2004 Due Mar 10, 2004 ACM 95b/100b 3pm at Firestone 303 E. Sterl Phinney (2 pts) Include grading section number

Problem Set 8 Mar 5, 2004 Due Mar 10, 2004 ACM 95b/100b 3pm at Firestone 303 E. Sterl Phinney (2 pts) Include grading section number Problem Set 8 Mar 5, 24 Due Mar 1, 24 ACM 95b/1b 3pm at Firestone 33 E. Sterl Phinney (2 pts) Include grading section number Useful Readings: For Green s functions, see class notes and refs on PS7 (esp

More information

16.362: Signals and Systems: 1.0

16.362: Signals and Systems: 1.0 16.362: Signals and Systems: 1.0 Prof. K. Chandra ECE, UMASS Lowell September 1, 2016 1 Background The pre-requisites for this course are Calculus II and Differential Equations. A basic understanding of

More information

Chapter 1 Fundamental Concepts

Chapter 1 Fundamental Concepts Chapter 1 Fundamental Concepts 1 Signals A signal is a pattern of variation of a physical quantity, often as a function of time (but also space, distance, position, etc). These quantities are usually the

More information

A First Course in Digital Communications

A First Course in Digital Communications A First Course in Digital Communications Ha H. Nguyen and E. Shwedyk February 9 A First Course in Digital Communications 1/46 Introduction There are benefits to be gained when M-ary (M = 4 signaling methods

More information

Amplitude and Phase A(0) 2. We start with the Fourier series representation of X(t) in real notation: n=1

Amplitude and Phase A(0) 2. We start with the Fourier series representation of X(t) in real notation: n=1 VI. Power Spectra Amplitude and Phase We start with the Fourier series representation of X(t) in real notation: A() X(t) = + [ A(n) cos(nωt) + B(n) sin(nωt)] 2 n=1 he waveform of the observed segment exactly

More information

Fundamentals of the Discrete Fourier Transform

Fundamentals of the Discrete Fourier Transform Seminar presentation at the Politecnico di Milano, Como, November 12, 2012 Fundamentals of the Discrete Fourier Transform Michael G. Sideris sideris@ucalgary.ca Department of Geomatics Engineering University

More information

L29: Fourier analysis

L29: Fourier analysis L29: Fourier analysis Introduction The discrete Fourier Transform (DFT) The DFT matrix The Fast Fourier Transform (FFT) The Short-time Fourier Transform (STFT) Fourier Descriptors CSCE 666 Pattern Analysis

More information

Signal Processing Signal and System Classifications. Chapter 13

Signal Processing Signal and System Classifications. Chapter 13 Chapter 3 Signal Processing 3.. Signal and System Classifications In general, electrical signals can represent either current or voltage, and may be classified into two main categories: energy signals

More information

3. Use absolute value notation to write an inequality that represents the statement: x is within 3 units of 2 on the real line.

3. Use absolute value notation to write an inequality that represents the statement: x is within 3 units of 2 on the real line. PreCalculus Review Review Questions 1 The following transformations are applied in the given order) to the graph of y = x I Vertical Stretch by a factor of II Horizontal shift to the right by units III

More information

Frequency Response and Continuous-time Fourier Series

Frequency Response and Continuous-time Fourier Series Frequency Response and Continuous-time Fourier Series Recall course objectives Main Course Objective: Fundamentals of systems/signals interaction (we d like to understand how systems transform or affect

More information

FROM ANALOGUE TO DIGITAL

FROM ANALOGUE TO DIGITAL SIGNALS AND SYSTEMS: PAPER 3C1 HANDOUT 7. Dr David Corrigan 1. Electronic and Electrical Engineering Dept. corrigad@tcd.ie www.mee.tcd.ie/ corrigad FROM ANALOGUE TO DIGITAL To digitize signals it is necessary

More information

8: Correlation. E1.10 Fourier Series and Transforms ( ) Fourier Transform - Correlation: 8 1 / 11. 8: Correlation

8: Correlation. E1.10 Fourier Series and Transforms ( ) Fourier Transform - Correlation: 8 1 / 11. 8: Correlation E. Fourier Series and Transforms (25-5585) - Correlation: 8 / The cross-correlation between two signals u(t) and v(t) is w(t) = u(t) v(t) u (τ)v(τ +t)dτ = u (τ t)v(τ)dτ [sub: τ τ t] The complex conjugate,

More information

3.2 Complex Sinusoids and Frequency Response of LTI Systems

3.2 Complex Sinusoids and Frequency Response of LTI Systems 3. Introduction. A signal can be represented as a weighted superposition of complex sinusoids. x(t) or x[n]. LTI system: LTI System Output = A weighted superposition of the system response to each complex

More information

2 Background: Fourier Series Analysis and Synthesis

2 Background: Fourier Series Analysis and Synthesis Signal Processing First Lab 15: Fourier Series Pre-Lab and Warm-Up: You should read at least the Pre-Lab and Warm-up sections of this lab assignment and go over all exercises in the Pre-Lab section before

More information

Detailed Solutions to Exercises

Detailed Solutions to Exercises Detailed Solutions to Exercises Digital Signal Processing Mikael Swartling Nedelko Grbic rev. 205 Department of Electrical and Information Technology Lund University Detailed solution to problem E3.4 A

More information

Lecture 28 Continuous-Time Fourier Transform 2

Lecture 28 Continuous-Time Fourier Transform 2 Lecture 28 Continuous-Time Fourier Transform 2 Fundamentals of Digital Signal Processing Spring, 2012 Wei-Ta Chu 2012/6/14 1 Limit of the Fourier Series Rewrite (11.9) and (11.10) as As, the fundamental

More information

FOURIER TRANSFORM AND

FOURIER TRANSFORM AND Version: 11 THE DISCRETE TEX d: Oct. 23, 2013 FOURIER TRANSFORM AND THE FFT PREVIEW Classical numerical analysis techniques depend largely on polynomial approximation of functions for differentiation,

More information

ENGIN 211, Engineering Math. Fourier Series and Transform

ENGIN 211, Engineering Math. Fourier Series and Transform ENGIN 11, Engineering Math Fourier Series and ransform 1 Periodic Functions and Harmonics f(t) Period: a a+ t Frequency: f = 1 Angular velocity (or angular frequency): ω = ππ = π Such a periodic function

More information

Digital Band-pass Modulation PROF. MICHAEL TSAI 2011/11/10

Digital Band-pass Modulation PROF. MICHAEL TSAI 2011/11/10 Digital Band-pass Modulation PROF. MICHAEL TSAI 211/11/1 Band-pass Signal Representation a t g t General form: 2πf c t + φ t g t = a t cos 2πf c t + φ t Envelope Phase Envelope is always non-negative,

More information

Homework 6 EE235, Spring 2011

Homework 6 EE235, Spring 2011 Homework 6 EE235, Spring 211 1. Fourier Series. Determine w and the non-zero Fourier series coefficients for the following functions: (a 2 cos(3πt + sin(1πt + π 3 w π e j3πt + e j3πt + 1 j2 [ej(1πt+ π

More information

Digital Communications

Digital Communications Digital Communications Chapter 9 Digital Communications Through Band-Limited Channels Po-Ning Chen, Professor Institute of Communications Engineering National Chiao-Tung University, Taiwan Digital Communications:

More information

2.161 Signal Processing: Continuous and Discrete

2.161 Signal Processing: Continuous and Discrete MIT OpenCourseWare http://ocw.mit.edu.6 Signal Processing: Continuous and Discrete Fall 008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. M MASSACHUSETTS

More information

Fourier Transform for Continuous Functions

Fourier Transform for Continuous Functions Fourier Transform for Continuous Functions Central goal: representing a signal by a set of orthogonal bases that are corresponding to frequencies or spectrum. Fourier series allows to find the spectrum

More information

Lecture 7 ELE 301: Signals and Systems

Lecture 7 ELE 301: Signals and Systems Lecture 7 ELE 30: Signals and Systems Prof. Paul Cuff Princeton University Fall 20-2 Cuff (Lecture 7) ELE 30: Signals and Systems Fall 20-2 / 22 Introduction to Fourier Transforms Fourier transform as

More information

Math 345: Applied Mathematics

Math 345: Applied Mathematics Math 345: Applied Mathematics Introduction to Fourier Series, I Tones, Harmonics, and Fourier s Theorem Marcus Pendergrass Hampden-Sydney College Fall 2012 1 Sounds as waveforms I ve got a bad feeling

More information

Communication Systems Lecture 21, 22. Dong In Kim School of Information & Comm. Eng. Sungkyunkwan University

Communication Systems Lecture 21, 22. Dong In Kim School of Information & Comm. Eng. Sungkyunkwan University Communication Systems Lecture 1, Dong In Kim School of Information & Comm. Eng. Sungkyunkwan University 1 Outline Linear Systems with WSS Inputs Noise White noise, Gaussian noise, White Gaussian noise

More information

Summary: ISI. No ISI condition in time. II Nyquist theorem. Ideal low pass filter. Raised cosine filters. TX filters

Summary: ISI. No ISI condition in time. II Nyquist theorem. Ideal low pass filter. Raised cosine filters. TX filters UORIAL ON DIGIAL MODULAIONS Part 7: Intersymbol interference [last modified: 200--23] Roberto Garello, Politecnico di orino Free download at: www.tlc.polito.it/garello (personal use only) Part 7: Intersymbol

More information