Convolution Integral-Electrical Circuit Analysis-Lecture Slides, Slides of Electrical Circuit Analysis

This lecture is part of lecture series on Electrical Circuit Analysis course. It was delivered by Prof. Mursleen Sayed at Bengal Engineering and Science University. It includes: Convolution, Integral, Linear, Time, Invariant, Excitation, Impulse, Response, Input, Output

Typology: Slides

2011/2012

Uploaded on 07/23/2012

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Convolution Integral
Linear time-invariant
circuit represented by
block
h(t) impulse response of
circuit
x(t) input excitation signal
y(t) output desired signal
Y(s) = H(s).X(s)
y(t) = h(t) * x(t) = x(t) * h(t)
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Convolution Integral

Linear time-invariantcircuit represented byblock

h(t) impulse response ofcircuit

x(t) input excitation signal

y(t) output desired signal

Y(s) = H(s).X(s)

y(t) = h(t) * x(t) = x(t) * h(t)

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Convolution Integral 

Convolution Integral relates the output y(t) of alinear time-invariant circuit to the input x(t) of thecircuit and the circuit’s impulse response h(t)

 

The convolution integral is used to extract theresponse of a circuit to an arbitrary source

It allows evaluation of x(t) and h(t) in time domain,where x(t) and h(t) are known through experimentaldata

 

 

λ d ) λ ( x ) λ t ( h λ d ) λ t ( x ) λ ( h ) t ( y

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Example 

h(

) = e

u(

v

i^

= 4t

for 0

t

v

(i

for 0

v

(-i

for -

v

(t-i

)= 4(t-

for t-

t

λ

λ  e

λ

λ 

λ

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Example 

For 0

t

20 0

λ

x(t- )

λ

5

10

t-

t-

5 t 0

 

20 0

λ

x(t- )

λ

5

10

t-

t-

10 t 5

 

20 0

λ

x(t- )

λ

5

10

t-

t-

   t 10

t

t

t

t 0

λ

o

λ d e ) λ t ( 4 v ) 1 t e ( 4 v

t

o

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Example 

t^

vo

1

2

3

4

5

6

7

8

9

10

11

12

13

14

15

) 1 t e ( 4 v

t

o

) e e 5 ( 4 v ) 5 t ( t o 

) e 5 e e ( 4 v ) 10 t ( ) 5 t ( t o 

5.00 0. 25.0020.00 15.0010.

0

1

2

3

4

5

6

7

8

9

10

11

12

13

14

15

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Graphic Interpretation of theConvolution Integral

λ

λ

λ

λ

τ^1

τ^2

λ

τ^1 

τ^2 

λ

λ

τ^1 

τ^2 

λ

λ

τ^1  λ λ

λ

λ

λ

λ

τ^1

τ^2

λ

λ

λ

λ

λ

τ^1

λ^

λ

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