Now ![]()
To solve this, we need to work in voltages, not current.
We start with
.
The voltage across a capacitor is given by
.
It follows that
.
So for this example we have:
![]()
Substituting known values:
![]()
Then
![]()
Taking Laplace:![]()
Since
, we have:
![]()

So, taking inverse Laplace
![]()
NOTE: For the part:
, we use:
![]()
So we have:
![]()

1. To find the Inverse Laplace:

2. To solve the original DE:

Exact solution for v(t):

To see what this means, we could write it as follows:

To see what our expression for v(t) means, we graph it as follows:
