
Emily W. answered 11/28/21
Knowledge in Foundations of Variable Mathematics
L{f(n)}= s^nY(s)− s^(n−1)y(0)−s^(n−2)y′(0)−⋯
-4dy/dt - y = 0 <— remember it’s really 0t here
Laplace applied individually to each term. Each term will become n+1 terms (n being the order of the derivative), stopping at the term where you hit an exponent of 0.
-4L{dy/dt} - L{y}= L{0t}
For the first term n= 1 (1st derivative) so we only need the first 2 terms of the transform
-4[s^1Y(s) + s^(1-1)y(0)]
= -4sY(s) - y(0)
For the second term n = 0 (not a derivative)
-1[s^0Y(s)]
= -1Y(s)
For the right side, (and in general for any #t, your laplace is #/s^2) we have 0t, which turns into 0/s^2
= 0 it remains 0
so we have -4sY(s) - y(0) - Y(s) = 0 plug in y(0) = -8
-4sY(s) - (-8) - Y(s) = 0 move the 8 to the other side
-4sY(s) - Y(s) = -8 I’m going to multiply everything by -1 to make it look a little better
4sY(s) + Y(s) = 8 factor out GCF which is Y(s)
Y(s)(4s+1) = 8
Y(s) = 8/(4s+1)
We need the denominator in the form s-a: factor by 4
8/4(s + 1/4) and we need it to say s-a so we will write it as a double negative
8/4(s - -1/4)
we can see that a = -1/4
The 8/4 can divide and make a 2
Y(s) = 2/(s- -1/4)
when the Laplace is in the form 1/s-a, the solutions is
f(t) = e^at
f(t) = 2e^(-1/4 t)