2 The convolution theorem

Let f ( t ) and g ( t ) be causal functions with Laplace transforms F ( s ) and G ( s ) respectively, i.e. L { f ( t ) } = F ( s ) and L { g ( t ) } = G ( s ) . Then it can be shown that

Key Point 16

The Convolution Theorem

L − 1 { F ( s ) G ( s ) } = ( f ∗ g ) ( t )  or equivalently L { ( f ∗ g ) ( t ) } = F ( s ) G ( s )
Example 5

Find the inverse transform of 6 s ( s 2 + 9 ) .

  1. Using partial fractions
  2. Using the convolution theorem.
Solution
  1. 6 s ( s 2 + 9 ) = ( 2 ∕ 3 ) s − ( 2 ∕ 3 ) s s 2 + 9 and so L − 1 6 s ( s 2 + 9 ) = 2 3 L − 1 1 s − 2 3 L − 1 s s 2 + 9 = 2 3 u ( t ) − 2 3 cos 3 t . u ( t )
  2. Let us choose F ( s ) = 2 s  and G ( s ) = 3 s 2 + 9 then

    f ( t ) = L − 1 { F ( s ) } = 2 u ( t )  and g ( t ) = L − 1 { G ( s ) } = sin 3 t . u ( t )

    So

    L − 1 { F ( s ) G ( s ) } = ( f ∗ g ) ( t ) (by the convolution theorem) = ∫ 0 t 2 u ( t − x ) sin 3 x . u ( x ) d x

    Now the variable t can take any value from − ∞ to + ∞ . If t < 0 then the variable of integration, x , is negative and so u ( x ) = 0 . We conclude that

    ( f ∗ g ) ( t ) = 0  if t < 0

    that is, ( f ∗ g ) ( t ) is a causal function . Let us now consider the other possibility for t , that is the range t ≥ 0 . Now, in the range of integration 0 ≤ x ≤ t and so

    u ( t − x ) = 1 u ( x ) = 1

    since both t − x and x are non-negative. Therefore

    L − 1 { F ( s ) G ( s ) } = ∫ 0 t 2 sin 3 x d x = − 2 3 cos 3 x 0 t = − 2 3 ( cos 3 t − 1 ) t ≥ 0

    Hence

    L − 1 { 6 s ( s 2 + 9 ) } = − 2 3 ( cos 3 t − 1 ) u ( t )

    which agrees with the value obtained above using the partial fraction approach.

Task!

Use the convolution theorem to find the inverse transform of H ( s ) = s ( s − 1 ) ( s 2 + 1 ) .

Begin by choosing two functions of s , that is, F ( s ) and G ( s ) :

Although there are many possibilities it would seem sensible to choose

F ( s ) = 1 s − 1 and G ( s ) = s s 2 + 1

since, by inspection, we can write down their inverse Laplace transforms:

f ( t ) = L − 1 { F ( s ) } = e t u ( t )  and g ( t ) = L − 1 { G ( s ) } = cos t . u ( t )

Now construct the convolution integral:

h ( t ) = L − 1 { H ( s ) } = L − 1 { F ( s ) G ( s ) } = ∫ 0 t f ( t − x ) g ( x ) d x = ∫ 0 t e t − x u ( t − x ) cos x . u ( x ) d x

Now complete the evaluation of the integral, treating the cases t < 0 and t ≥ 0 separately:

You should find h ( t ) = 1 2 ( sin t − cos t + e t ) u ( t ) since h ( t ) = 0 if t < 0 and

h ( t ) = ∫ 0 t e t − x cos x d x  if t ≥ 0 = [ e t − x sin x ] 0 t − ∫ 0 t ( − 1 ) e t − x sin x d x (integrating by parts) = sin t + [ − e t − x cos x ] 0 t − ∫ 0 t ( − e t − x ) ( − cos x ) d x = sin t − cos t + e t − h ( t )  or 2 h ( t ) = sin t − cos t + e t t ≥ 0

Finally h ( t ) = 1 2 ( sin t − cos t + e t ) u ( t )

Exercises
  1. Find the convolution of
    1. 2 t u ( t ) and t 3 u ( t )
    2. e t u ( t ) and t u ( t )
    3. e − 2 t u ( t ) and e − t u ( t ) .

       In each case reverse the order to check that ( f ∗ g ) ( t ) = ( g ∗ f ) ( t ) .

  2. Use the convolution theorem to determine the inverse Laplace transforms of
    1. 1 s 2 ( s + 1 )
    2. 1 ( s − 1 ) ( s − 2 )
    3. 1 ( s 2 + 1 ) 2
    1. 1 10 t 5
    2. − t − 1 + e t
    3. e − t − e − 2 t
    1. ( t − 1 + e − t ) u ( t )
    2. ( − ( e t + e 2 t ) u ( t )
    3. 1 2 ( sin t − t cos t ) u ( t )