Lesson 26 - Convolution

In this lesson, we introduce the method of convolution. This method is to be used when you have a composition of piecewise functions and need to take the Laplace transform of those functions.

Definition

The convolution f∗g of piecewise continuous functions f and g is defined for t≥0 as follows:

(f∗g)(t)=∫0tf(t−v) g(v) dv

Properties of Convolution

  1. (f∗g)(t)=(g∗f)(t)
  2. (f∗(g+h))(t)=(f∗g)(t)+(f∗h)(t)
  3. ((f∗g)∗h)(t)=(f∗(g∗h))(t)
  4. (f∗0)(t)=0

Theorem

L[(f∗g)(t)]=F(s)G(s), where F(s)=L[f(t)], G(s)=L[g(t)]

Example

Use convolution to find: L−1[1(s2+1)2]

L−1[1(s2+2)2]=L−1[1s2+1⋅1s2+1]

Identify f(t) and g(t). In this case, f(t)=g(t)=1s2+1.

Next, we take the Laplace transform of f(t) and g(t), which will be the same since the functions are the same.

L[f(t)]=L[g(t)]=sin⁡t

Now let's plug this into our definition above.

(f∗g)(t)=∫0tf(t−v) g(v) dv=∫0t sin⁡(t−v) sin⁡v dv

Now we can utilize a trig identity in order to solve this integral.

Recall sin⁡Asin⁡B=12[cos⁡(A−B)−cos⁡(A+B)]. Let's say A=v, and B=t−v.

=12∫0t [cos⁡(v−(t−v))−cos⁡(v+(t−v))] dv=12∫0t [cos⁡(2v−t)−cos⁡(t)] dv

Now we can perform the integration.

=12[12sin⁡t−tcos⁡t−12(sin⁡(−t))]

Recall sin⁡(−t)=−sin⁡t.

=12[sin⁡t−tcos⁡t]

So,

L−1[1(s2+1)2]=12[sin⁡t−tcos⁡t]

Try for Yourself

  1. L−1[1s(s2+1)]
  2. L−1[s(s2+1)2]
  3. L−1[s+1(s2+1)2]

Next Lesson: Lesson 27 - The Dirac Delta Function

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