Second Order first degree differential equations with constant coefficients
A general second order linear differential
equation with constant coefficients is of the form
where
ϕ(D) = aD2 + bD + c (a,b and c are constants)
To solve the equation (1), we first solve the equation ϕ ( D )
y = 0. The solution so
obtained is called complementary function (C.F).
Next we operate on f (
x) with 1/ ϕ ( D) , the solution so obtained is called particular integral (P.I)
Type 1 : f(x) = 0
(i.e) ϕ(D)y = 0
To solve this, put ϕ ( D)
= 0
Replace D by m. This equation is called auxiliary
equation . ϕ( m ) = 0 is a quadratic
equation. So we have two roots, say m1 and m2.
Now we have the following three cases
Here
A and B are arbitrary constants
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