An ordinary differential equation of the form
(1)
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Such an equation has singularities for finite under the following conditions: (a) If either or diverges as , but and remain finite as , then is called a regular or nonessential singular point. (b) If diverges faster than so that as , or diverges faster than so that as , then is called an irregular or essential singularity.
Singularities of equation (1) at infinity are investigated by making the substitution , so , giving
(2)
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(3)
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(4)
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(5)
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Then (3) becomes
(6)
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Case (a): If
(7)
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(8)
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remain finite at (), then the point is ordinary. Case (b): If either diverges no more rapidly than or diverges no more rapidly than , then the point is a regular singular point. Case (c): Otherwise, the point is an irregular singular point.
Morse and Feshbach (1953, pp. 667-674) give the canonical forms and solutions for second-order ordinary differential equations classified by types of singular points.
For special classes of linear second-order ordinary differential equations, variable coefficients can be transformed into constant coefficients. Given a second-order linear ODE with variable coefficients
(9)
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Define a function ,
(10)
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(11)
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(12)
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(13)
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(14)
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This will have constant coefficients if and are not functions of . But we are free to set to an arbitrary positive constant for by defining as
(15)
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Then
(16)
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(17)
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and
(18)
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(19)
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Equation (◇) therefore becomes
(20)
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which has constant coefficients provided that
(21)
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Eliminating constants, this gives
(22)
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So for an ordinary differential equation in which is a constant, the solution is given by solving the second-order linear ODE with constant coefficients
(23)
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for , where is defined as above.
A linear second-order homogeneous differential equation of the general form
(24)
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can be transformed into standard form
(25)
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with the first-order term eliminated using the substitution
(26)
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Then
(27)
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(28)
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(29)
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(30)
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(31)
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so
(32)
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(33)
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Therefore,
(34)
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where
(35)
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If , then the differential equation becomes
(36)
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which can be solved by multiplying by
(37)
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to obtain
(38)
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(39)
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(40)
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For a nonhomogeneous second-order ordinary differential equation in which the term does not appear in the function ,
(41)
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let , then
(42)
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So the first-order ODE
(43)
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if linear, can be solved for as a linear first-order ODE. Once the solution is known,
(44)
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(45)
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On the other hand, if is missing from ,
(46)
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let , then , and the equation reduces to
(47)
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which, if linear, can be solved for as a linear first-order ODE. Once the solution is known,
(48)
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Nonhomogeneous ordinary differential equations can be solved if the general solution to the homogenous version is known, in which case variation of parameters can be used to find the particular solution. In particular, the particular solution to a nonhomogeneous second-order ordinary differential equation
(49)
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can be found using variation of parameters to be given by the equation
(50)
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where and are the homogeneous solutions to the unforced equation
(51)
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and is the Wronskian of these two functions.