Michael K. answered 02/09/21
PhD professional for Math, Physics, and CS Tutoring and Martial Arts
Laplace Transforms change differential equations into more manageable algebraic equations.
Let's define L{y(t)} = F(s), so we are going to use the definition int_{lb=0}_{ub=∞} (y(t)*exp(-st)dt to convert from the t variable to the s variable
Now using integration by parts we can determine what L{y'(t)} is as well as L{y''(t)} is with respect to the definition L{y(t)} or F(s). In doing so we will need to utilize the initial conditions.
L{y'(t)} = s*F(s) - y(0)
L{y"(t)} = s2F(s) - s*y(0) - y'(0)
L{6t-8} = 6 * 1/s2 - 8/s
So, we have...
s2F(s) - s*y(0) - y'(0) - 4*(s*F(s) - y(0)) + 3F(s) = (6 - 8s)/s2
s2F(s) - s*0 - 0 - 4*(s*F(s) - 0) + 3F(s) = (6 - 8s)/s2
s2F(s) - 4sF(s) + 3F(s) = (6 - 8s)/s2
F(s) = (6 - 8s)/s2 * 1/(s2 - 4s + 3)
F(s) = -2(4s - 3)/s2 * 1/(s2 - 4s + 3)
F(s) = -2(4s - 3)/s2 * 1/(s - 3)(s - 1)
F(s) = -2(4s - 3) / s2(s - 3)(s - 1)
Now we need to break into partial fractions to use the inverse Laplace Transform to solve the problem...
A/s2 + B/(s-1) + C/(s-3) = (4s - 3) / s2(s - 3)(s - 1)
I don't need to worry about the overall constant factor of -2
Finding the common denominator, we get three (four but with same answer) equations in three unknowns...
B = -C. ( to cancel the s3 terms)
-B + A -3C = 0 (to cancel the s2 term)
-4A = 4 to account for the s term
-3A = 3 to account for the constant term
A = -1
Plugging back into the second equation with help fo first equations gives...
-B + 1 + 3B = 0 ---> B = 1/2
Therefore C = -1/2
F(s) = -2 [ -1/s2 + 1/(2*(s-3)) - 1/(2*(s-1))
Using the inverse transform now is trivial...
y(t) = L-1{F(s)} = -2 * (-t + 1/2*e^(3t) - 1/2*e^(t))
y(t) = 2t + e3t - et