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7.2 Inverse Transforms and Transforms of Derivatives: Class Notes

7.2a

Theorem 7.2.1: Some Inverse Transforms

Example

Find the inverse Laplace transform.

ℒ−1{1s4}

Solution

This matches part (b) with n=3⇒n!=6. The numerator needs to be 6, so multiply and divide by 6:

ℒ−1{1s4}=16ℒ−1{6s4}=16t3

Answer: ℒ−1{1s4}=16t3

ℒ−1{10ss2+16}

Solution

The s2+16 in the denominator means a trig function, with k=4. The s in the numerator makes it cosine:

ℒ−1{10ss2+16}=10ℒ−1{ss2+16}=10cos⁡4t

Answer: ℒ−1{10ss2+16}=10cos⁡4t

ℒ−1{s+1s2+2}

Solution

Here k=2. Split the fraction; the second piece needs k=2 in the numerator, so multiply and divide by 2:

ℒ−1{s+1s2+2}=ℒ−1{ss2+2+12·1·2s2+2}=cos⁡2t+12sin⁡2t

Answer: ℒ−1{s+1s2+2}=cos⁡2t+12sin⁡2t

ℒ−1{s+1s2−4s}

Solution

The denominator factors as s(s−4), so use partial fraction decomposition (PFD):

s+1s(s−4)=As+Bs−4⇒s+1=A(s−4)+Bs

s=0: 1=−4A, so A=−14. s=4: 5=4B, so B=54.

ℒ−1{−1/4s+5/4s−4}=−14+54e4t

Answer: ℒ−1{s+1s2−4s}=−14+54e4t

7.2b

Example

Use the Laplace transform to solve the Initial-Value Problem.

2dydt+y=0,y(0)=−3

Solution

Plan: Apply the Laplace transform to both sides.

2ℒ{dydt}+ℒ{y(t)}=ℒ{0}

The transform ℒ takes y(t) to Y(s), and the inverse transform ℒ−1 takes Y(s) back to y(t). To transform the equation, we need the transform of a derivative.

Transforms of derivatives

ℒ{f′(t)}=∫0∞e−stf′(t)dt

Integrate by parts with u=e−st,dv=f′(t)dt, so du=−se−stdt,v=f(t).

ℒ{f′(t)}=f(t)est|0∞+s∫0∞e−stf(t)dt=−f(0)+sF(s)

If f(t) is of exponential order, f(t)est→0 as t→∞ (for large enough s), so only the lower limit contributes. So

ℒ{f′(t)}=sF(s)−f(0)

The value f(0) comes from the initial condition.

Plan (cont): Solve for Y(s) and use ℒ−1.

Back to the example: transform 2dydt+y=0 and substitute y(0)=−3:

2(sY(s)−y(0))+Y(s)=02sY(s)+6+Y(s)=0(2s+1)Y(s)=−6Y(s)=−62s+1=−3s+1/2y(t)=−3e−t/2

Answer: y(t)=−3e−t/2

The second derivative. The same steps give the transform of f″:

ℒ{f″(t)}=∫0∞e−stf″(t)dt

Integrate by parts with u=e−st,dv=f″(t)dt, so du=−se−stdt,v=f′(t).

ℒ{f″(t)}=f′(t)est|0∞+s∫0∞e−stf′(t)dt=−f′(0)+sℒ{f′(t)}=−f′(0)+s(sF(s)−f(0))

ℒ{f″(t)}=s2F(s)−sf(0)−f′(0)

Guess: ℒ{f‴(t)}=s3F(s)−s2f(0)−sf′(0)−f″(0)

7.2c

Theorem: Transform of a Derivative

If f,f′,…,f(n−1) are continuous on [0,∞) and are of exponential order and if f(n)(t) is piecewise continuous on [0,∞), then

ℒ{f(n)(t)}=snF(s)−sn−1f(0)−sn−2f′(0)−⋯−f(n−1)(0),

where F(s)=ℒ{f(t)}.

Example

Use the Laplace transform to solve the Initial-Value Problem.

y″−4y′=6e3t−3e−t,y(0)=1,y′(0)=−1

Solution

Transform each term, matching colors to the equation:

s2Y(s)−sy(0)−y′(0)−4(sY(s)−y(0))=6s−3−3s+1

Substitute y(0)=1 and y′(0)=−1, then solve for Y(s):

(s2−4s)Y(s)−s+1+4=6s−3−3s+1(s2−4s)Y(s)=6s−3−3s+1+s−5(s2−4s)Y(s)=6(s+1)−3(s−3)+(s−5)(s+1)(s−3)(s+1)(s−3)(s2−4s)Y(s)=6s+6−3s+9+s3−7s2+7s+15(s+1)(s−3)Y(s)=s3−7s2+10s+30s(s−4)(s+1)(s−3)

Partial fractions:

s3−7s2+10s+30s(s−4)(s+1)(s−3)=As+Bs−4+Cs+1+Ds−3

s3−7s2+10s+30=A(s−4)(s+1)(s−3)+Bs(s+1)(s−3)+Cs(s−4)(s−3)+Ds(s−4)(s+1)

Substitute each root of the denominator; every term but one becomes zero:

s=0:30=A(−4)(1)(−3)⇒A=52s=4:64−112+40+30=B(4)(5)(1)⇒B=1110s=−1:−1−7−10+30=C(−1)(−5)(−4)⇒C=−35s=3:27−63+30+30=D(3)(−1)(4)⇒D=−2

Y(s)=5/2s+11/10s−4−3/5s+1−2s−3

Answer: y(t)=52+1110e4t−35e−t−2e3t