y′′−y=0
Assume that n=0∑∞anxn is a solution. Then you have
y′=n=1∑∞nanxn−1, y′′=n=2∑∞n(n−1)anxn−2
n=2∑∞n(n−1)anxn−2=n=0∑∞anxn
n=0∑∞(n+2)(n+1)an+2xn=n=0∑∞anxn By equating coefficients, we have
(n+2)(n+1)an+2=anWe obtain the recursion formula
an+2=(n+2)(n+1)an,n≥0 a0,a1
a2=1⋅2a0, a3=2⋅3a1
a4=1⋅2⋅3⋅4a0, a5=2⋅3⋅4⋅5a1
⋮ ⋮
a2k=(2k)!a0, a2k+1=(2k+1)!a1Thus, we can represent the general solution as the sum of two series—one for the
even-powered terms with coefficients in terms of a0 and one for the odd-powered
terms with coefficients in terms of a1
y=a0k=0∑∞(2k)!x2k+a1k=0∑∞(2k+1)!x2k+1 The solution has two arbitrary constants, and as we would expect in the
general solution of a second-order differential equation.
y=C1ex+C2e−x
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