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DISCRETE-TIME LTI SYSTEMS: THE CONVOLUTION SUM
• In general, of course, the responses ℎ𝑘[𝑛] need not be related to each other for different values of k. However,
if the linear system is also time invariant, then these responses to time-shifted unit impulses are all time-
shifted versions of each other. Specifically, since 𝛿[𝑛 − 𝑘]is a time-shifted version of 𝛿[𝑛], the response
ℎ𝑘[𝑛] is a time-shifted version of ℎ0[𝑛]; i.e.,
• For notational convenience, we will drop the subscript on ℎ0[𝑛] and define the unit impulse (sample)
response
• That is, h[n] is the output of the LTI system when 𝛿[𝑛] is the input. Then for an LTI system.
This result is referred to as the convolution sum or superposition
sum. We will represent the operation of convolution
symbolically as
THE CONVOLUTION SUM: Example
THE CONVOLUTION SUM: Example
THE CONVOLUTION SUM: Example
THE CONVOLUTION SUM: Example
• Suggested examples: S. Palani, Signals and Systems, Chapter 3
• Example 3.45
• Example 3.50
• Example 3.52
CONTINUOUS-TIME LTI SYSTEMS: THE CONVOLUTION
INTEGRAL
2. CONTINUOUS-TIME LTI SYSTEMS: THE
CONVOLUTION INTEGRAL
For a CT system
• The unit impulse response of CT system
𝑥 𝑡 = න
−∞
∞
𝑥(𝜏)𝛿 𝑡 − 𝜏 𝑑𝜏
If the system is linear
𝒚 𝒕 = න
−∞
∞
𝒙 𝝉 𝒉𝝉 𝒕 𝒅𝝉
In case of time invariant system
𝒉𝝉 𝒕 = 𝒉 𝒕 − 𝝉
𝑦 𝑡 = ‫׬‬−∞
∞
𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏 (the output of LTI system)
This result is referred to as the convolution integral or
superposition integral. We will represent the operation
of convolution symbolically as
𝑥(𝑡) 𝑦(𝑡)
CT system
𝑥 𝑡 = 𝛿(𝑡 − 𝜏) 𝑦 𝑡 = ℎ𝜏(𝑡)
CT system
𝑥 𝑡 = 𝛿(𝑡) 𝑦 𝑡 = ℎ0(𝑡)
CONTINUOUS-TIME LTI SYSTEMS: THE CONVOLUTION
INTEGRAL
The convolution integral:
𝑦 𝑡 = න
−∞
∞
𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏
LTI System
Impulse Response: ℎ(𝑡)
𝑥(𝑡) 𝑦 𝑡) = 𝑥 𝑡 ∗ ℎ(𝑡 = න
−∞
∞
𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏
THE CONVOLUTION INTEGRAL
The following are the basic steps involved in convolution integral equation:
1. For the input signal 𝑥 𝑡 , express it as 𝑥 𝜏 .
2. Express impulse response function ℎ(𝑡) as ℎ(𝑡 − 𝜏) by substituting 𝑡 = 𝑡 − 𝜏
3. Integrate ‫׬‬−∞
∞
𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏 to get 𝑦(𝑡).
4. The limit of integration depends on the time limit of 𝑥 𝑡 . For causal signals 𝑥 𝑡 and ℎ 𝑡 (causal signal or
system : 𝑥 𝑡 =0 for 𝑥 < 0), the lower limit of convolution integral is zero and the upper limit is t.
5. Find 𝑦 𝑡 = ‫׬‬−∞
∞
𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏
THE CONVOLUTION INTEGRAL
B.P. Lathi, Linear Systems and Signals, 2005, Oxford University Press (optional)
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
• The graphical representation of convolution operation is shown in Fig. 3.8.
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
THE CONVOLUTION INTEGRAL: Example
• Suggested examples: S. Palani, Signals and Systems, Chapter 3
• Example 3.2
• Example 3.11
• Example 3.13
• Example 3.16
• Example 3.19
• Example 3.21

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signal and system chapter2-part3.pdf

  • 1. DISCRETE-TIME LTI SYSTEMS: THE CONVOLUTION SUM • In general, of course, the responses ℎ𝑘[𝑛] need not be related to each other for different values of k. However, if the linear system is also time invariant, then these responses to time-shifted unit impulses are all time- shifted versions of each other. Specifically, since 𝛿[𝑛 − 𝑘]is a time-shifted version of 𝛿[𝑛], the response ℎ𝑘[𝑛] is a time-shifted version of ℎ0[𝑛]; i.e., • For notational convenience, we will drop the subscript on ℎ0[𝑛] and define the unit impulse (sample) response • That is, h[n] is the output of the LTI system when 𝛿[𝑛] is the input. Then for an LTI system. This result is referred to as the convolution sum or superposition sum. We will represent the operation of convolution symbolically as
  • 2.
  • 6. THE CONVOLUTION SUM: Example • Suggested examples: S. Palani, Signals and Systems, Chapter 3 • Example 3.45 • Example 3.50 • Example 3.52
  • 7.
  • 8. CONTINUOUS-TIME LTI SYSTEMS: THE CONVOLUTION INTEGRAL 2. CONTINUOUS-TIME LTI SYSTEMS: THE CONVOLUTION INTEGRAL For a CT system • The unit impulse response of CT system 𝑥 𝑡 = න −∞ ∞ 𝑥(𝜏)𝛿 𝑡 − 𝜏 𝑑𝜏 If the system is linear 𝒚 𝒕 = න −∞ ∞ 𝒙 𝝉 𝒉𝝉 𝒕 𝒅𝝉 In case of time invariant system 𝒉𝝉 𝒕 = 𝒉 𝒕 − 𝝉 𝑦 𝑡 = ‫׬‬−∞ ∞ 𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏 (the output of LTI system) This result is referred to as the convolution integral or superposition integral. We will represent the operation of convolution symbolically as 𝑥(𝑡) 𝑦(𝑡) CT system 𝑥 𝑡 = 𝛿(𝑡 − 𝜏) 𝑦 𝑡 = ℎ𝜏(𝑡) CT system 𝑥 𝑡 = 𝛿(𝑡) 𝑦 𝑡 = ℎ0(𝑡)
  • 9. CONTINUOUS-TIME LTI SYSTEMS: THE CONVOLUTION INTEGRAL The convolution integral: 𝑦 𝑡 = න −∞ ∞ 𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏 LTI System Impulse Response: ℎ(𝑡) 𝑥(𝑡) 𝑦 𝑡) = 𝑥 𝑡 ∗ ℎ(𝑡 = න −∞ ∞ 𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏
  • 10.
  • 11. THE CONVOLUTION INTEGRAL The following are the basic steps involved in convolution integral equation: 1. For the input signal 𝑥 𝑡 , express it as 𝑥 𝜏 . 2. Express impulse response function ℎ(𝑡) as ℎ(𝑡 − 𝜏) by substituting 𝑡 = 𝑡 − 𝜏 3. Integrate ‫׬‬−∞ ∞ 𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏 to get 𝑦(𝑡). 4. The limit of integration depends on the time limit of 𝑥 𝑡 . For causal signals 𝑥 𝑡 and ℎ 𝑡 (causal signal or system : 𝑥 𝑡 =0 for 𝑥 < 0), the lower limit of convolution integral is zero and the upper limit is t. 5. Find 𝑦 𝑡 = ‫׬‬−∞ ∞ 𝑥 𝜏 ℎ 𝑡 − 𝜏 𝑑𝜏
  • 12. THE CONVOLUTION INTEGRAL B.P. Lathi, Linear Systems and Signals, 2005, Oxford University Press (optional)
  • 14. THE CONVOLUTION INTEGRAL: Example • The graphical representation of convolution operation is shown in Fig. 3.8.
  • 22. THE CONVOLUTION INTEGRAL: Example • Suggested examples: S. Palani, Signals and Systems, Chapter 3 • Example 3.2 • Example 3.11 • Example 3.13 • Example 3.16 • Example 3.19 • Example 3.21