# 8. Using Inverse Laplace Transforms to Solve Differential Equations

## Laplace Transform of Derivatives

We use the following notation:

(a) If we have the function `g(t)`, then `G(s) = G = Lap{g(t)}`.

(b) *g*(0) is the value of the function *g*(*t*) at *t* = 0.

(c) *g*'(0), *g*’’(0),... are the values of the derivatives of the function at *t* = 0.

If `g(t)` is continuous and *g*'(0), *g*’’(0),... are finite, then we have the following.

### First Derivative

`Lap{g"'"(t)}= Lap{(dg)/(dt)}` `=sG-g(0)`

### Second Derivative

`Lap{g"''"(t)}=s^2G-s\ g(0) - g"'"(0)`

We saw many of these expressions in the Table of Laplace Transforms.

**
NOTATION NOTE:** If instead of

*g*(

*t*) we have a function

*y*of

*x*, then Equation (2) would simply become:

`Lap{y’’(x)} = s^2Y − s\ y (0) − y’(0)`

Likewise, if we have an expression for current *i* and it is a function of *t*, then the equation would become:

`Lap{i’’(t)} = s^2I − s\ i(0) − i\ ’(0)`

### For the *n-*th derivative

`Lap{(d^ng)/(dt^n)}` `=s^nG-s^(n-1)g(0)-s^(n-2)g ’ (0)-` `...-g^(n-1)(0)`

**NOTATION NOTE:** If we have *y* and it is a function of *t*, then the notation would become:

`Lap{(d^ny)/(dt^n)}` `=s^nY-s^(n-1)y(0)-s^(n-2)y ’ (0)-` `...-y^(n-1)(0)`

## Subsidiary Equation

The **subsidiary equation** is the equation in terms of *s*, *G* and the coefficients *g**'*(0), *g**’’*(0),... etc., obtained by taking the transforms of all the terms in a linear differential equation.

The subsidiary equation is expressed in the form *G* = *G*(*s*).

## Examples

Write down the subsidiary equations for the following differential equations and hence solve them.

### Example 1

`(dy)/(dt)+y=sin\ 3t`, given that *y* = 0 when *t* = 0.

Answer

Taking Laplace transform of both sides gives:

`(sY-y(0))+Y=3/(s^2+9)`

`sY+Y=3/(s^2+9)` (since `y(0) = 0`)

`(s+1)Y=3/(s^2+9)`

Solving for *Y* and finding the partial fraction decomposition gives:

`Y=3/((s+1)(s^2+9))` `=A/(s+1)+(Bs+C)/(s^2+9)`

`3=A(s^2+9)+(s+1)(Bs+C)`

Substituting convenient values of `s` gives us:

`s=-1` gives `3=10A`, which gives `A=3/10`.

`s=0` gives `3=9A+C`, which gives `C=3/10`.

`s=1` gives `3=10A+2B+2C`, which gives us `B=-3/10`.

So

`Y=3/((s+1)(s^2+9))`

`=3/10(1/(s+1)+(-s+1)/(s^2+9))`

`=3/10(1/(s+1)-s/(s^2+9)+1/(s^2+9))`

Finding the inverse Laplace tranform gives us the solution for *y *as a function of *t*:

`y=3/10e^(-t)-3/10cos\ 3t+1/10sin\ 3t`

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#### Solution Graph for Example 1

This is the graph of the solution we obtained in the example above.

### Example 2

Solve `(d^2y)/(dt^2)+2(dy)/(dt)+5y=0`, given that `y = 1,` and `(dy)/(dt)=0,` when `t = 0.`

Answer

Taking Laplace transform of both sides and appying initial conditions of `y(0) = 1` and `y"'"(0) = 0` gives:

`{s^2Y-sy(0)-y"'"(0)}+` `2{sY-` `y(0)}+5Y=` `0`

`(s^2Y-s)+2(sY-1)+5Y=0`

`(s^2+2s+5)Y=s+2`

Solving for *Y* and completing the square on the denominator gives:

`Y=(s+2)/(s^2+2s+5)`

`=(s+2)/((s^2+2s+1)+4)`

`=(s+2)/((s+1)^2+4)`

`=(s+1)/((s+1)^2+4)+1/2 2/((s+1)^2+4)`

Now, finding the inverse Laplace Transform gives us the solution for *y* as a function of *t*:

`y=e^(-t)cos\ 2t+1/2e^(-t) sin\ 2t`

#### Solution Graph for Example 2

Here is the graph of what we just found:

### Example 3

`(d^2y)/(dt^2)-2(dy)/(dt)+y=e^t`, given that *y* = -2, and `(dy)/(dt)=-3` when *t* = 0.

Answer

Taking Laplace transform of both sides:

`{s^2Y-sy(0)-y"'"(0)}-` `2{sY-y(0)}+Y` `=1/(s-1)`

Applying the initial condition and simplifying gives:

`(s^2Y+2s+3)-2(sY+2)+Y` `=(1)/(s-1) `

`(s^2-2s+1)Y` `=(1)/(s-1)-2s+1 `

`(s-1)^2Y=(1)/(s-1)-2s+1 `

Solving for *Y*:

`Y=(1)/((s-1)^3)+(-2s+1)/((s-1)^2)` `=1/2(2)/((s-1)^3)+(-2s+1)/((s-1)^2) `

For the first term, we use: `Lap^{:-1:} {(n!)/((s-a)^[n+1])}=e^[at]t^n`, with *a* = 1 and *n* = 2.

So

`Lap^{:-1:}{1/2 (2)/((s-1)^3)}` `=1/2 e^t t^2 `

For the second term, we express in partial fractions:

`(-2s+1)/((s-1)^2)` `=(A)/(s-1)+(B)/((s-1)^2) `

`-2s+1=A(s-1)+B `

Comparing coefficients:

`-2s=As ` gives `A = -2`.

`1=-A+B ` gives `B = -1`.

So `(-2s+1)/((s-1)^2)` `=-(2)/(s-1)-(1)/((s-1)^2) `

And

`Lap^{:-1:} { - (2)/(s-1) - (1)/((s-1)^2)}` `=-2e^t - te^t`

Putting our inverse Laplace transform expressions together, the solution for *y* is:

`y(t)=1/2 t^2 e^t - 2e^t - te^t`

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#### Solution Graph for Example 3

## Application

The current *i*(*t*) in an electrical circuit is given by the DE

`(d^2i)/(dt^2)+2(di)/(dt)=0,if 0 < t < 10`

`=1,if 10 < t < 20`

`=0,if t > 20`

and *i*(0) = 0, *i*’(0) = 0.

Determine the current as a function of *t*.

Answer

We need to write the RHS of the DE in terms of unit step functions.

`(d^2i)/(dt^2)+2(di)/(dt)` `=u(t-10)-u(t-20)`

Now, taking Laplace transform of both sides gives us:

`(s^2I-s\ i(0)-i"'"(0))+2(sI-i(0))` `=(e^(-10s))/s-(e^(-20s))/s`

`s^2I+2sI` `=1/s(e^(-10s)-e^(-20s))`

`(s^2+2s)I` `=1/s(e^(-10s)-e^(-20s))`

Solving for `I` gives:

`I=1/s((e^(-10s)-e^(-20s))/(s^2+2s))` `=1/(s^2(s+2))(e^(-10s)-e^(-20s))`

We need to find the Inverse Laplace of this expression. First, we concentrate on the `1/(s^2(s+2))` part and ignore the `(e^(-10s)-e^(-20s))` part for now.

Now, we find the partial fractions: `1/(s^2(s+2))` `=A/s+B/s^2+C/(s+2)`

Multiply both sides by `s^2(s+2)`:

`1=As(s+2)+B(s+2)+Cs^2`

`s = 0` gives `1 = 2B` gives `B=1/2`

`s=-2` gives `1 = 4C` gives `C=1/4`

`s=1` gives `1 = 3A + 3B + C` gives `A= -1/4`

So `1/(s^2(s+2))` `=-1/(4s)+1/(2s^2)+1/(4(s+2))`

Now, the inverse Laplace of this expression is:

`Lap^{:-1:}{1/(s^2(s+2))}`

`Lap^{:-1:}{-1/(4s)+1/(2s^2)+1/(4(s+2))}`

`=-1/4+1/2t+1/4e^(-2t)`

So since

`I=1/(s^2(s+2))e^(-10s)-1/(s^2(s+2))e^(-20s)`,

then we have, using the Time-Displacement Theorem (see the Table of Laplace Transforms):

`i(t)=` `[-1/4*u(t-10)+` `1/2(t-10)*u(t-10)+` `{:1/4e^(-2(t-10))*u(t-10)]-` `[-1/4*u(t-20)+` `1/2(t-20)*u(t-20)+` `{:1/4e^(-2(t-20))*u(t-20)]`

`=1/4(2t-21+e^(-2(t-10)))*u(t-10)` `+1/4(41-2t-e^(-2(t-20)))*u(t-20)`

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#### Solution Graph for the Application (current at time *t*)

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