Lesson 27 - The Dirac Delta Function

Here, we explore time shift equations a bit more by introducing the Dirac delta function. δ(ta).

  1. The Dirac delta function δ(ta) is characterized by the following two properties:

a)

u(ta)={0tat=a

b)

f(t) δ(ta) dt=f(a)

for any continuous function f(t) on an open interval containing t=0.

  1. L[δ(ta)]=eas, L1[eas]=δ(ta)

  2. Reminder: L1[easF(s)]=u(ta)f(ta)

  3. We can use: L1[as2a2]=sinhat, L1[ss2a2]=coshat

Examples

Find: L[δ(t1)δ(t3)]

L[δ(t1)]L[δ(t3)]=ese3s

Find: L[etδ(t3)]

Here, we take the Laplace transform of the δ(t3) function. However, now that we have an et, we perform a shift based on the term et.

First, we will take the Laplace transform of the Dirac delta function.

L[δ(t3)]=e3s

Now, we will apply the time shift. The time shift is in the form eat. Here, a=1, so we will shift the opposite of the sign of a, so a negative shift.

ete3(s1)

So,

L[etδ(t3)]=e3(s1)

Let's try another.

Find: L[e3tδ(t5)]

L[e3tδ(t5)]=e5(s+3)

Again, we take the Laplace transform of δ(t5), this gives us e5s. Then we shift by the a in eat. This gives us 35(s+3).

Try For Yourself

  1. Find: L[e2tδ(t+2)]
  2. Find: L[etδ(t3)]
  3. Find: L[e2tδ(t1)]

We can also take the inverse Laplace transform of a Dirac delta function. We typically find the inverse Laplace transform of F(s) as we normally do, then we time shift from the time shift term. Let's look at an example.

Example

L1[1ss2+3s+2e2s]

First, identify F(s).

F(s)=1s2+3s+2

Now, we take the inverse Laplace transform of F(s).

L1[F(s)]=L1[1s2+3s+2]=L1[1(s+1)(s+2)]

Partial fraction decomposition:

1(s+1)(s+2)=As+1+Bs+21=A(s+2)+B(s+1)s=11=A1=(s+2)+B(s+1)s=21=B

So,

1(s+1)(s+2)=1s+21s+2

Now,

L1[e2s(1s+11s+2)]

We know the Laplace transforms of 1s+1 and 1s+2.

L1[1s+1]L1[1s+2]=ete2t

Now, we apply the inverse Laplace transform of the time shift e2s.

e(t2)e2(t2)

Try for Yourself

  1. Find: L1[1s2+2s+5e2s]

On the page, you will find additional practice problems including an application problem regarding Dirac delta functions.

Next Lesson: Lesson 27.1 - Extra Practice Solving IVPs Containing Dirac Delta Functions

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