Solve
d²y/dx²+ y = 1
given y (0) = 1 and y(π/2) = 0 using Laplace transform
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L{dy} + L{2y} = L{12e3t} dt
Now
L{dy} = −y(0)+sY(s)=−3+sY(s) dt
L{2y} = 2Y (s) and L{12e3t} = 12 s−3
Substituting these expressions into the transformed version of the differential equation gives:
[−3+sY(s)]+2Y(s) = 12 s−3
Solving for Y (s) we have (s+2)Y(s)= 12 +3= 3+3s
Therefore
®
s−3 s−3 Y (s) = 3(s + 1)
(s+2)(s−3)
Now, using partial fractions, this last expression can be written in a more convenient form:
Y(s)= 3/5 + 12/5 (s+2) (s−3)
and then, inverting:
y(t)=L−1{Y(s)}=3L−1{ 1 }+12L−1{ 1 } 5s+25s−3
thus
y(t) = 3 e−2tu(t) + 12 e3tu(t)
This is the solution to the given initial value problem.
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