Use Laplace transform to solve the differential equationy
′′−2y′−3y=0y″−2y′−3y=0
with the initial conditions y(0)=2y(0)=2 and y′(0)=−1y′(0)=−1 and y is a function of time t.
Solution
Let L[y(t)] = Y(s)
Then Laplace transform of the equation is
s2Y(s)-sy(0)-y’(0)-2[sY(s)-y(0)]-3Y(s)=0
(s2-2s-3)Y(s) = sy(0)+y’(0)-2y(0)
Using the initial conditions (s2-2s-3)Y(s) = 2s-5 => Y(s) = (2s-5)/(s2-2s-3) = (2s-5)/[(s-3)(s+1)]
(2s-5)/[(s-3)(s+1)] = A/(s-3)+B/(s+1), where A,B are arbitrary constants
From this equality
2s-5 = A(s+1)+B(s-3) => 2s-5 = (A+B)s+A-3B => A+B=2, A-3B=-5 => 4B=7, A+B=2 => B=7/4, A=1/4
So Y(s) = (1/4)/(s-3)+(7/4)/(s+1)
From the Table of Laplace Transforms 1/(s-a)<->e-at
Therefore y(t) = e3t /4+7 e-t/4
Answer
y(t) = e3t /4+7 e-t/4
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