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 fg of piecewise continuous functions f and g is defined for t0 as follows:

(fg)(t)=0tf(tv) g(v) dv

Properties of Convolution

  1. (fg)(t)=(gf)(t)
  2. (f(g+h))(t)=(fg)(t)+(fh)(t)
  3. ((fg)h)(t)=(f(gh))(t)
  4. (f0)(t)=0

Theorem

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

Example

Use convolution to find: L1[1(s2+1)2]

L1[1(s2+2)2]=L1[1s2+11s2+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)]=sint

Now let's plug this into our definition above.

(fg)(t)=0tf(tv) g(v) dv=0t sin(tv) sinv dv

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

Recall sinAsinB=12[cos(AB)cos(A+B)]. Let's say A=v, and B=tv.

=120t [cos(v(tv))cos(v+(tv))] dv=120t [cos(2vt)cos(t)] dv

Now we can perform the integration.

=12[12sinttcost12(sin(t))]

Recall sin(t)=sint.

=12[sinttcost]

So,

L1[1(s2+1)2]=12[sinttcost]

Try for Yourself

  1. L1[1s(s2+1)]
  2. L1[s(s2+1)2]
  3. L1[s+1(s2+1)2]

Next Lesson: Lesson 27 - The Dirac Delta Function

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