Presentation is loading. Please wait.

Presentation is loading. Please wait.

بسم الله الرحمن الرحيم Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly University.

Similar presentations


Presentation on theme: "بسم الله الرحمن الرحيم Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly University."— Presentation transcript:

1 بسم الله الرحمن الرحيم Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly University of Khartoum Department of Electrical and Electronic Engineering Fourth Year (2013- 2014) Digital Signal processing معالجة الإشارة الرقمية Digital Signal processing معالجة الإشارة الرقمية

2 ContentContent Frequency Domain Concepts  Continuous-time sinusoidal signals  Discrete-time sinusoidal signals  Harmonically Related Complex Exponentials 2014 - 2015 2

3 3

4 4 The Concept of Frequency in Continuous- time signals The concept of frequency is directly related to the concept of time. A simple harmonic oscillation: Signal parameters: A : Amplitude Ω : Frequency in radians/sec θ : phase in radians Ω = 2π F F : frequency in cycles/sec or Hz. T=1/F is the period of the signal

5 2014 - 2015 5 The Concept of Frequency in Continuous- time signals

6 The Analog signal is characterized by the following characteristics: 6

7 For F= 0, T p = ∞ 2014 - 2015 7

8 8 Continuous time sinusoidal signals By definition frequency is an inherently positive physical quantity. However, only for mathematical convenience, we need to introduce negative frequencies.

9 2014 - 2015 9 As time progresses the phasors rotate in opposite directions with angular frequencies : ± Ω radians/sec Continuous time sinusoidal signals

10 2014 - 2015 10 The Concept of Frequency in Continuous- time signals Representation of a cosine function by phasors

11 2014 - 2015 11

12 2014 - 2015 12 Discrete-time sinusoidal signals Signal parameters: n : integer variable A : Amplitude ω : Frequency in radians/sample (ω = 2π f) θ : phase in radians f : frequency in cycles/sample.(f=1/N) N : is the period

13 2014 - 2015 13 Example Example of a discrete-time sinusoidal signal: (ω =π/6 radians per sample (f =1/12 cycles per sample) and θ = π/3 ) n x(n)

14 2014 - 2015 14 Discrete-time sinusoidal signals (cont) 1 Properties B1. A Discrete time sinusoid is periodic only if its frequency f is a rational number B1. A Discrete time sinusoid is periodic only if its frequency f is a rational number.

15 2014 - 2015 15 Proof: By definition, a discrete time signal is periodic if and only if x(N+n) =x(n) f 0 is the fundamental frequency The relationship is true if there exists an integer k such that

16 2014 - 2015 16 Discrete-time sinusoidal signals (cont) A discrete-time signal is periodic, if its frequency f 0 can be expressed as the ratio of two integers. (i.e., f 0 is rational.) integer

17 2014 - 2015 17 Discrete-time sinusoidal signals (cont) Any small change in frequency can result a large change in the period:

18 2014 - 2015 18 Discrete-time sinusoidal signals (cont) Properties B2. Discrete-time sinusoids whose frequencies are separated by an integer multiple of 2 π are identical.

19 2014 - 2015 19 Proof Consider the sinusoid As a result, all sinusoidal sequences Where are indistinguishable (i.e., identical) Discrete-time Sinusoidal Signals (cont)

20 2014 - 2015 20 On the other hand, Sequences of any two sinusoids with frequencies in the range are distinct (unique) Consequently, discrete time sinusoidal signals with frequencies

21 21 Any sequence resulting from a sinusoid with frequencies is identical to a sequence obtained from a sinusoidal with frequencies Because of this similarity, we call the sinusoid having the frequency an alias of a corresponding sinusoid with frequency. Discrete-time sinusoidal signals (cont) 2014 - 2015

22 22 NoticeNotice The difference between discrete time sinusoids and continuous time sinusoids, is that the continuous time signals result in distinct signals for Ω or F in the range Discrete-time sinusoidal signals (cont)

23 2014 - 2015 23 Discrete-time sinusoidal signals (cont) Properties B3. The highest rate of oscillation in a discrete-time sinusoids is attained when ω = π ( or ω = -π) or equivalently f = ½ ( or f = - ½ )

24 2014 - 2015 Discrete-time sinusoidal signals (cont) When the frequency varies from 0 to π. We take values of ω 0 =0, π/8, π/4, π/2, π corresponding to f = 0, 1/16, 1/8, ¼, ½. Which result in periodic sequences having periods N=∞, 16, 8, 4, 2 as depicted in the Figure below. 24

25 2014 - 2015 25

26 2014 - 2015 26

27 Harmonically Related Complex Exponentials These are sets of periodic complex exponentials with fundamental frequencies that are multiples of a single positive frequency. 2014 - 2015 27

28 Text Book: John G. Proakis, and D. Manolakis, Digital Signal Processing: Principles, Algorithms and Applications, This lecture covered the following: 2014 - 2015 28

29 2014 - 2015 29 Next Lecture


Download ppt "بسم الله الرحمن الرحيم Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly Lecture (3) Frequency Domain Concepts Dr. Iman Abuel Maaly University."

Similar presentations


Ads by Google